Solutions for Chapter 1 – Mole Balances P1-1. This problem helps the student understand the course goals and objectives. Part (d) gives hints on how to solve problems when they get stuck. P1-2. Encourages students to get in the habit of writing down what they learned from each chapter. It also gives tips on problem solving. P1-3. Helps the student understand critical thinking and creative thinking, which are two major goals of the course. P1-4. Requires the student to at least look at the wide and wonderful resources available on the CDROM and the Web. P1-5. The ICMs have been found to be a great motivation for this material. P1-6. Uses Example 1-1 to calculate a CSTR volume. It is straight forward and gives the student an idea of things to come in terms of sizing reactors in chapter 4. An alternative to P1-15. P1-7. Straight forward modification of Example 1-1. P1-8. Helps the student review and member assumption for each design equation. P1-9. The results of this problem will appear in later chapters. Straight forward application of chapter 1 principles. P1-10. Straight forward modification of the mole balance. Assigned for those who emphasize bioreaction problems. P1-11. Will be useful when the table is completed and the students can refer back to it in later chapters. Answers to this problem can be found on Professor Susan Montgomery’s equipment module on the CD-ROM. See P1-14. P1-12. Many students like this straight forward problem because they see how CRE principles can be applied to an everyday example. It is often assigned as an in-class problem where parts (a) through (f) are printed out from the web. Part (g) is usually omitted. P1-13. Shows a bit of things to come in terms of reactor sizing. Can be rotated from year to year with P1-6. P1-14. I always assign this problem so that the students will learn how to use POLYMATH/MATLAB before needing it for chemical reaction engineering problems. P1-15 and P1-16. Help develop critical thinking and analysis. CDP1-A Similar to problems 3, 4, and 10. 1-2 Summary Assigned Alternates Difficulty Time (min) P1-1 AA SF 60 P1-2 I SF 30 P1-3 O SF 30 P1-4 O SF 30 P1-5 AA SF 30 P1-6 AA SF 15 P1-7 I SF 15 P1-8 S SF 15 P1-9 S SF 15 P1-10 O FSF 15 P1-11 I SF 1 P1-12 O FSF 30 P1-13 O SF 60 P1-14 AA SF 60 P1-15 O -- 30 P1-16 O FSF 15 CDP1-A AA FSF 30 1-13 Assigned = Always assigned, AA = Always assign one from the group of alternates, O = Often, I = Infrequently, S = Seldom, G = Graduate level 1-3 Alternates In problems that have a dot in conjunction with AA means that one of the problem, either the problem with a dot or any one of the alternates are always assigned. Time Approximate time in minutes it would take a B/B+ student to solve the problem. Difficulty SF = Straight forward reinforcement of principles (plug and chug) FSF = Fairly straight forward (requires some manipulation of equations or an intermediate calculation). IC = Intermediate calculation required M = More difficult OE = Some parts open-ended. * Note the letter problems are found on the CD-ROM. For example A CDP1-A. Summary Table Ch-1 Review of Definitions and Assumptions 1,5,6,7,8,9 Introduction to the CD-ROM 1,2,3,4 Make a calculation 6 Open-ended 8 1-4 P1-1 Individualized solution. P1-2 (b) The negative rate of formation of a species indicates that its concentration is decreasing as the reaction proceeds ie. the species is being consumed in the course of the reaction. A positive number indicates production of the particular compound. (c) The general equation for a CSTR is: FA 0 V FA rA Here rA is the rate of a first order reaction given by: rA = - kCA Given : CA = 0.1CA0 , k = 0.23 min-1, v0 = 10dm3 min-1 Substituting in the above equation we get: V CA0 v0 C Av0 kC A C A0 v0 (1 0.1) 0.1kC A0 V = 391.304 m3 (d) k = 0.23 min-1 From mole balance: dNA Rate law: rA k dt rA V rA k CA NA V Combine: dNA dt k NA 1-5 (10dm3 / min)(0.9) (0.23 min 1 )(0.1) at t 0 , NAO = 100 mol and t t= N 1 ln A0 k NA 1 ln 100 0.23 t , NA = (0.01)NAO min t = 20 min P1-3 Individualized solution. P1-4 Individualized solution. P1-5 Individualized solution. P1-6 Individualized solution P1-7 (a) The assumptions made in deriving the design equation of a batch reactor are: - Closed system: no streams carrying mass enter or leave the system. - Well mixed, no spatial variation in system properties - Constant Volume or constant pressure. 1-6 P1- 7 (b) The assumptions made in deriving the design equation of CSTR, are: - Steady state. - No spatial variation in concentration, temperature, or reaction rate throughout the vessel. P1-7(c) The assumptions made in deriving the design equation of PFR are: - Steady state. - No radial variation in properties of the system. P1-7 (d) The assumptions made in deriving the design equation of PBR are: - Steady state. - No radial variation in properties of the system. P1-7 (e) For a reaction, A B -rA is the number of moles of A reacting (disappearing) per unit time per unit volume [=] moles/ (dm3.s). -rA’ is the rate of disappearance of species A per unit mass (or area) of catalyst *=+ moles/ (time. mass of catalyst). rA’ is the rate of formation (generation) of species A per unit mass (or area) of catalyst *=+ moles/ (time. mass catalyst). -rA is an intensive property, that is, it is a function of concentration, temperature, pressure, and the type of catalyst (if any), and is defined at any point (location) within the system. It is independent of amount. On the other hand, an extensive property is obtained by summing up the properties of individual subsystems within the total system; in this sense, rA is independent of the ‘extent’ of the system. P 1-8 Rate of homogenous reaction rA is defined as the mole of A formed per unit volume of the reactor per second. It is an Intensive property and the concentration, temperature and hence the rate varies with spatial coordinates. 1-7 rA' on the other hand is defined as g mol of A reacted per gm. of the catalyst per second. Here mass of catalyst is the basis as this is what is important in catalyst reactions and not the reactor volume. Applying general mole balance we get: dN j dt Fj0 Fj r j dV No accumulation and no spatial variation implies 0 F j0 Fj r j dV Also rj = ρb rj` and W = Vρb where ρb is the bulk density of the bed. => 0 ( Fj 0 Fj ) rj' ( b dV ) Hence the above equation becomes Fj 0 W Fj r ' j We can also just apply the general mole balance as dN j dt ( Fj 0 Fj ) rj' (dW ) Assuming no accumulation and no spatial variation in rate, we get the same form Fj 0 W as above: Fj rj' P1-9 Applying mole balance to Penicillin: Penicillin is produced in the cells stationary state (See Chapter 9), so there is no cell growth and the nutrients are used in making product. Let’s do part c first. 1-8 [Flowrate In (moles/time)] penicillin + [generation rate (moles/time)]penicillin – [ Flowrate Out(moles/time)] penicillin = [rate of accumulation (moles/time)]penicillin dNp dt Fp,in + Gp – Fp,out = Fp,in = 0 (because no penicillin inflow) V Gp = rp .dV Therefore, V rp .dV - Fp,out = dNp dt Assuming steady state for the rate of production of penicillin in the cells stationary state, dNp =0 dt And no variations V Fp ,in Fp ,out rp Or, V Fp ,out rp Similarly, for Corn Steep Liquor with FC = 0 V FC 0 FC rC FC 0 rC Assume RNA concentration does not change in the stationary state and no RNA is generated or destroyed. P1-10 Given A 2 * 1010 ft 2 TSTP V 4 * 1013 ft 3 T = 534.7 R R 0.7302 atm ft 3 lbmol R 491.69 R H 2000 ft PO = 1atm CS yA = 0.02 1-9 2.04 *10 10 lbmol ft 3 C = 4*105 cars FS = CO in Santa Ana winds vA 3000 FA = CO emission from autos ft 3 per car at STP hr P1-10 (a) Total number of lb moles gas in the system: N N= PV 0 RT 1atm (4 1013 ft 3 ) = 1.025 x 1011 lb mol atm. ft 3 0.73 534.69 R lbmol.R P1-10 (b) Molar flowrate of CO into L.A. Basin by cars. FA y A FT FT 3000 ft 3 hr car yA v A C P0 R TSTP 1lbmol 400000 cars 359 ft 3 (See appendix B) FA = 6.685 x 104 lb mol/hr P1-10 (c) Wind speed through corridor is v = 15mph W = 20 miles The volumetric flowrate in the corridor is vO = v.W.H = (15x5280)(20x5280)(2000) ft3/hr = 1.673 x 1013 ft3/hr P1-10 (d) Molar flowrate of CO into basin from Sant Ana wind. FS v0 CS = 1.673 x 1013 ft3/hr 2.04 10 10 lbmol/ft3 = 3.412 x 103lbmol/hr P1-10 (e) 1-10 Rate of emission of CO by cars + Rate of CO by Wind - Rate of removal of CO = FA FS vo C co V dC co dt (V=constant, N co dN CO dt C coV ) P1-10 (f) t = 0 , C co C coO t Cco dt V 0 CcoO dCco FS voCco FA F FS vo C coO V ln A vo FA FS vo C co t P1-10 (g) Time for concentration to reach 8 ppm. CCO 0 2.04 10 8 lbmol , CCO ft 3 2.04 lbmol 10 8 4 ft 3 From (f), F FS vO .CCO 0 V ln A vo FA FS vO .CCO t 3 lbmol lbmol 3 lbmol 13 ft 3.4 10 1.673 10 2.04 10 8 3 4 ft hr hr hr ft 3 ln ft 3 lbmol lbmol ft 3 lbmol 1.673 1013 6.7 104 3.4 103 1.673 1013 0.51 10 8 hr hr hr hr ft 3 6.7 104 t = 6.92 hr P1-10 (h) (1) to = 0 tf = 72 hrs C co = 2.00E-10 lbmol/ft3 a = 3.50E+04 lbmol/hr vo = 1.67E+12 ft3 /hr b = 3.00E+04 lbmol/hr Fs = 341.23 lbmol/hr V = 4.0E+13 ft3 a b sin t 6 Fs vo C co V dC co dt Now solving this equation using POLYMATH we get plot between Cco vs t 1-11 See Polymath program P1-10-h-1.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 72 72 C 2.0E-10 2.0E-10 v0 1.67E+12 1.67E+12 a 3.5E+04 3.5E+04 3.5E+04 3.5E+04 b 3.0E+04 3.0E+04 3.0E+04 3.0E+04 F 341.23 341.23 341.23 V 4.0E+13 4.0E+13 4.0E+13 2.134E-08 1.877E-08 1.67E+12 1.67E+12 341.23 4.0E+13 ODE Report (RKF45) Differential equations as entered by the user [1] d(C)/d(t) = (a+b*sin(3.14*t/6)+F-v0*C)/V Explicit equations as entered by the user [1] v0 = 1.67*10^12 [2] a = 35000 [3] b = 30000 [4] F = 341.23 [5] V = 4*10^13 1-12 (2) tf = 48 hrs Fs = 0 a t 6 b sin vo C co V Now solving this equation using POLYMATH we get plot between Cco vs t See Polymath program P1-10-h-2.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 48 48 C 2.0E-10 2.0E-10 v0 1.67E+12 1.67E+12 a 3.5E+04 3.5E+04 3.5E+04 3.5E+04 b 3.0E+04 3.0E+04 3.0E+04 3.0E+04 V 4.0E+13 4.0E+13 4.0E+13 4.0E+13 1.904E-08 1.693E-08 1.67E+12 1.67E+12 ODE Report (RKF45) Differential equations as entered by the user [1] d(C)/d(t) = (a+b*sin(3.14*t/6)-v0*C)/V Explicit equations as entered by the user [1] v0 = 1.67*10^12 [2] a = 35000 [3] b = 30000 [4] V = 4*10^13 1-13 dC co dt (3) Changing a Increasing ‘a’ reduces the amplitude of ripples in graph. It reduces the effect of the sine function by adding to the baseline. Changing b The amplitude of ripples is directly proportional to ‘b’. As b decreases amplitude decreases and graph becomes smooth. Changing v0 As the value of v0 is increased the graph changes to a “shifted sin-curve”. And as v0 is decreased graph changes to a smooth increasing curve. P1-11 (a) – rA = k with k = 0.05 mol/h dm3 CSTR: The general equation is FA 0 V FA rA Here CA = 0.01CA0 , v0 = 10 dm3/min, FA = 5.0 mol/hr Also we know that FA = CAv0 and FA0 = CA0v0, CA0 = FA0/ v0 = 0.5 mol/dm3 Substituting the values in the above equation we get, V C A0v0 C A v0 k (0.5)10 0.01(0.5)10 0.05 1-14 V = 99 dm3 FR: The general equation is dFA dV rA k , Now FA = CAv0 and FA0 = CA0v0 => dC A v0 dV k Integrating the above equation we get v0 C A dC A k CA0 V dV => V 0 v0 (C A0 k CA ) Hence V = 99 dm3 Volume of PFR is same as the volume for a CSTR since the rate is constant and independent of concentration. P1-11 (b) - rA = kCA with k = 0.0001 s-1 CSTR: We have already derived that V C A0v0 C A v0 v0 C A0 (1 0.01) kC A rA k = 0.0001s-1 = 0.0001 x 3600 hr-1= 0.36 hr-1 V (10dm 3 / hr )(0.5mol / dm 3 )(0.99) => V = 2750 dm3 1 3 (0.36hr )(0.01 * 0.5mol / dm ) PFR: From above we already know that for a PFR dC Av0 dV rA kC A Integrating v0 C A dC A k CA0 C A v0 C A0 ln k CA V dV 0 V Again k = 0.0001s-1 = 0.0001 x 3600 hr-1= 0.36 hr-1 1-15 Substituing the values in above equation we get V = 127.9 dm3 P1-11 (c) - rA = kCA2 with k = 3 dm3/mol.hr CSTR: CA0 v 0 CA v 0 rA V v 0CA0 (1 0.01) kCA 2 Substituting all the values we get (10dm 3 /hr)(0.5mol /dm 3 )(0.99) (3dm 3 /hr)(0.01* 0.5mol /dm 3 ) 2 V => V = 66000 dm3 PFR: dCA v 0 dV rA kCA 2 Integrating C v 0 A dCA k C CA 2 A0 => V V dV => 0 v0 1 ( k CA 10dm 3 /hr 1 ( 3 3dm /mol.hr 0.01CA0 1 ) V CA 0 1 ) = 660 dm3 CA0 P1-11 (d) CA = .001CA0 t NA0 NA dN rAV Constant Volume V=V0 t C A 0 dC A CA rA Zero order: t 1 CA0 0.001CA0 k .999CAo 0.05 9.99 h First order: 1-16 t 1 CA0 ln k CA 1 1 ln 0.001 .001 6908 s Second order: t 1 1 k CA 1 CA0 1 1 3 0.0005 1 0.5 666 h P1-12 (a) Initial number of rabbits, x(0) = 500 Initial number of foxes, y(0) = 200 Number of days = 500 dx dt k1 x k2 xy …………………………….(1) dy dt k3 xy k4 y ……………………………..(2) Given, k1 0.02day 1 k2 0.00004 /(day k3 0.0004 /(day rabbits ) k4 0.04day 1 foxes ) See Polymath program P1-12-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 500 500 x 500 2.9626929 519.40024 4.2199691 y 200 1.1285722 4099.517 117.62928 k1 0.02 0.02 k2 4.0E-05 4.0E-05 0.02 0.02 4.0E-05 4.0E-05 1-17 k3 4.0E-04 4.0E-04 k4 0.04 0.04 4.0E-04 0.04 4.0E-04 0.04 ODE Report (RKF45) Differential equations as entered by the user [1] d(x)/d(t) = (k1*x)-(k2*x*y) [2] d(y)/d(t) = (k3*x*y)-(k4*y) Explicit equations as entered by the user [1] k1 = 0.02 [2] k2 = 0.00004 [3] k3 = 0.0004 [4] k4 = 0.04 When, tfinal = 800 and k3 0.00004 /(day rabbits ) 1-18 Plotting rabbits Vs. foxes P1-12 (b) POLYMATH Results See Polymath program P1-12-b.pol. POLYMATH Results NLES Solution Variable Value f(x) Ini Guess x 2.3850387 2.53E-11 2 y 3.7970279 1.72E-12 2 NLES Report (safenewt) Nonlinear equations [1] f(x) = x^3*y-4*y^2+3*x-1 = 0 [2] f(y) = 6*y^2-9*x*y-5 = 0 P1-13 Enrico Fermi Problem – no definite solution P1-14 Mole Balance: V= FA0 FA rA 1-19 Rate Law : rA kC A2 Combine: V= FA0 FA kC A2 FA0 v0C A dm3 2molA 3 . s dm3 FA v0C A 3 6molA s dm3 0.1molA . s dm3 0.3molA s mol s V= dm3 mol (0.03 )(0.1 3 ) 2 mol.s dm (6 0.3) 19, 000dm3 1-20 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . Solutions for Chapter 2 - Conversion and Reactor Sizing P2-1. This problem will keep students thinking about writing down what they learned every chapter. P2-2. This “forces” the students to determine their learning style so they can better use the resources in the text and on the CDROM and the web. P2-3. ICMs have been found to motivate the students learning. P2-4. Introduces one of the new concepts of the 4th edition whereby the students “play” with the example problems before going on to other solutions. P2-5. This is a reasonably challenging problem that reinforces Levenspiels plots. P2-6. Straight forward problem alternative to problems 7, 8, and 11. P2-7. To be used in those courses emphasizing bio reaction engineering. P2-8. The answer gives ridiculously large reactor volume. The point is to encourage the student to question their numerical answers. P2-9. Helps the students get a feel of real reactor sizes. P2-10. Great motivating problem. Students remember this problem long after the course is over. P2-11. Alternative problem to P2-6 and P2-8. P2-12. Novel application of Levenspiel plots from an article by Professor Alice Gast at Massachusetts Institute of Technology in CEE. CDP2-A Similar to 2-8 CDP2-B Good problem to get groups started working together (e.g. cooperative learning). CDP2-C Similar to problems 2-7, 2-8, 2-11. CDP2-D Similar to problems 2-7, 2-8, 2-11. Summary P2-1 P2-2 P2-3 Assigned O A A Alternates Difficulty Time (min) 15 30 30 P2-4 P2-5 P2-6 P2-7 P2-8 P2-9 P2-10 P2-11 P2-12 CDP2-A CDP2-B CDP2-C CDP2-D O O AA S AA S AA AA S O O O O 7,8,11 6,8,11 6,7,8 8,B,C,D 8,B,C,D 8,B,C,D 8,B,C,D M FSF FSF SF SF SF SF M FSF FSF FSF FSF 75 75 45 45 45 15 1 60 60 5 30 30 45 Assigned = Always assigned, AA = Always assign one from the group of alternates, O = Often, I = Infrequently, S = Seldom, G = Graduate level Alternates In problems that have a dot in conjunction with AA means that one of the problems, either the problem with a dot or any one of the alternates are always assigned. Time Approximate time in minutes it would take a B/B+ student to solve the problem. Difficulty SF = Straight forward reinforcement of principles (plug and chug) FSF = Fairly straight forward (requires some manipulation of equations or an intermediate calculation). IC = Intermediate calculation required M = More difficult OE = Some parts open-ended. ____________ * Note the letter problems are found on the CD-ROM. For example A CDP1-A. Summary Table Ch-2 Straight forward 1,2,3,4,9 Fairly straight forward 6,8,11 More difficult 5,7, 12 Open-ended 12 Comprehensive 4,5,6,7,8,11,12 Critical thinking P2-8 P2-1 Individualized solution. P2-2 (a) Example 2-1 through 2-3 If flow rate FAO is cut in half. v1 = v/2 , F1= FAO/2 and CAO will remain same. Therefore, volume of CSTR in example 2-3, 1 FA0 X 2 rA F1 X rA V1 1 6.4 2 3.2 If the flow rate is doubled, F2 = 2FAO and CAO will remain same, Volume of CSTR in example 2-3, V2 = F2X/-rA = 12.8 m3 P2-2 (b) Example 2-4 Levenspiel Plot 4.5 4 3.5 Fao/-ra 3 2.5 2 1.5 1 0.5 0 0 0.2 0.4 Now, FAO = 0.4/2 = 0.2 mol/s, Table: Divide each term X [FAO/-rA](m3) 0.82 FA 0 rA 0.8 FA 0 in Table 2-3 by 2. rA 0 0.445 Reactor 1 V1 = 0.82m3 V = (FAO/-rA)X 0.6 Conversion 0.1 0.545 0.2 0.665 0.4 1.025 0.6 1.77 0.7 2.53 0.8 4 Reactor 2 V2 = 3.2 m3 X1 3.2 X1 By trial and error we get: X1 = 0.546 and X2 = 0.8 Overall conversion XOverall = (1/2)X1 + (1/2)X2 = (0.546+0.8)/2 = 0.673 P2-2 (c) Example 2-5 (1) For first CSTR, at X=0 ; FA 0 rA X2 X2 1 FA0 rA 1.28m3 at X=0.2 ; FA0 rA .94 m3 From previous example; V1 ( volume of first CSTR) = .188 m3 Also the next reactor is PFR, Its volume is calculated as follows 0.5 V2 0.2 FAO dX rA 0.247 m3 For next CSTR, X3 = 0.65, FAO rA 2 m 3 , V3 = FAO ( X 3 X 2 ) rA (2) Now the sequence of the reactors remain unchanged. But all reactors have same volume. First CSTR remains unchanged Vcstr = .1 = (FA0/-rA )*X1 => X1 = .088 Now For PFR: X2 V 0.088 FAO dX rA , By estimation using the levenspiel plot X2 = .183 For CSTR, .3m3 VCSTR2 = FAO X 3 X 2 rA 0.1m3 => X3 = .316 (3) The worst arrangement is to put the PFR first, followed by the larger CSTR and finally the smaller CSTR. Conversion X1 = 0.20 X2 = 0.60 X3 = 0.65 Original Reactor Volumes V1 = 0.188 (CSTR) V2 = 0.38 (PFR) V3 = 0.10 (CSTR) Worst Arrangement V1 = 0.23 (PFR) V2 = 0.53 (CSTR) V3 = 0.10 (CSTR) For PFR, X1 = 0.2 X1 V1 0 FAO dX rA Using trapezoidal rule, XO = 0.1, X1 = 0.1 X1 V1 XO rA f XO f X1 0.2 1.28 0.98 m3 2 0.23m3 For CSTR, For X2 = 0.6, FAO 1.32m3 , rA V2 = FAO rA V3 = 0.1 m3 FAO X2 rA X 1 = 1.32(0.6 – 0.2) = 0.53 m3 For 2nd CSTR, For X3 = 0.65, 2m3 , P2-3 Individualized solution. P2-4 Solution is in the decoding algorithm given with the modules. P2-5 X 0 0.1 0.2 0.4 0.6 0.7 0.8 3 FAO/-rA (m ) 0.89 1.08 1.33 2.05 3.54 5.06 8.0 V = 1.6 m3 P2-5 (a) Two CSTRs in series For first CSTR, V = (FAo/-rAX1) X => X1 = 0.53 For second CSTR, V = (FAo/-rAX2) (X2 – X1) => X2 = 0.76 P2-5 (b) Two PFRs in series X1 V 0 FAo dX rA X2 X1 FAo dX rA By extrapolating and solving, we get X1 = 0.62 X2 = 0.84 P2-5 (c) Two CSTRs in parallel with the feed, FAO, divided equally between two reactors. FANEW/-rAX1 = 0.5FAO/-rAX1 V = (0.5FAO/-rAX1) X1 Solving we get, Xout = 0.68 P2-5 (d) Two PFRs in parallel with the feed equally divided between the two reactors. FANEW/-rAX1 = 0.5FAO/-rAX1 By extrapolating and solving as part (b), we get Xout = 0.88 P2-5 (e) A CSTR and a PFR are in parallel with flow equally divided Since the flow is divided equally between the two reactors, the overall conversion is the average of the CSTR conversion (part C) and the PFR conversion (part D) Xo = (0.60 + 0.74) / 2 = 0.67 P2-5 (f) A PFR followed by a CSTR, XPFR = 0.50 (using part(b)) V = (FAo/-rA-XCSTR) (XCSTR – XPFR) Solving we get, XCSTR = 0.70 P2-5 (g) A CSTR followed by a PFR, XCSTR = 0.44 (using part(a)) X PFR V FAO dX X CSTR rA By extrapolating and solving, we get XPFR = 0.72 P2-5 (h) A 1 m3 PFR followed by two 0.5 m3 CSTRs, For PFR, XPFR = 0.50 (using part(b)) CSTR1: V = (FAo/-rA-XCSTR) (XCSTR – XPFR) = 0.5 m3 XCSTR = 0.63 CSTR2: V = (FAo/-rA-XCSTR2) (XCSTR2 – XCSTR1) = 0.5 m3 XCSTR2 = 0.72 P2-6 Exothermic reaction: A B + C X 0 0.20 0.40 0.45 0.50 0.60 0.80 0.90 P2-6 (a) r(mol/dm3.min) 1 1.67 5 5 5 5 1.25 0.91 1/-r(dm3.min/mol) 1 0.6 0.2 0.2 0.2 0.2 0.8 1.1 To solve this problem, first plot 1/-rA vs. X from the chart above. Second, use mole balance as given below. CSTR: Mole balance: VCSTR FA0 X rA 300mol / min 0.4 => 5mol / dm 3 . min =>VCSTR = 24 dm3 PFR: X V PFR FA 0 Mole balance: dX rA 0 = 300(area under the curve) VPFR = 72 dm3 P2-6 (b) For a feed stream that enters the reaction with a previous conversion of 0.40 and leaves at any conversion up to 0.60, the volumes of the PFR and CSTR will be identical because of the rate is constant over this conversion range. .6 VPFR FA 0 dX r A .4 FA0 .6 dX rA .4 P2-6 (c) VCSTR = 105 dm3 Mole balance: VCSTR FA0 X rA F A 0 .6 X rA .4 105dm 3 300mol / min X rA 0.35dm 3 min/ mol Use trial and error to find maximum conversion. At X = 0.70, 1/-rA = 0.5, and X/-rA = 0.35 dm3.min/mol Maximum conversion = 0.70 P2-6 (d) From part (a) we know that X1 = 0.40. Use trial and error to find X2. FA 0 X 2 X 1 rA X Mole balance: V 2 Rearranging, we get X2 0.40 rA X 2 At X2 = 0.64, V FA 0 X2 0.008 0.40 rA X 0.008 2 Conversion = 0.64 P2-6 (e) From part (a), we know that X1 = 0.40. Use trial and error to find X2. X2 Mole balance: V PFR 72 FA 0 dX rA 0.40 X2 300 At X2 = 0.908, V = 300 x (area under the curve) => V = 300(0.24) = 72dm3 Conversion = 0.908. dX rA 0.40 P2-6 (f) See Polymath program P2-6-f.pol. P2-7 (a) V FS 0 X rS FS0 = 1000 g/hr At a conversion of 40% Therefore V 1 rS 0.15 0.15 (1000)(0.40) dm 3 hr g 60 dm 3 P2-7 (b) At a conversion of 80%, 1 rS 0.8 dm 3 hr g FS0 = 1000 g/hr Therefore V 0.8 (1000)(0.80) 640 dm 3 P2-7 (c) X VPFR FS 0 dX rS 0 From the plot of 1/-rS Calculate the area under the curve such that the area is equal to V/FS0 = 80 / 1000 = 0.08 X = 12% For the 80 dm3 CSTR, V 80 dm 3 FS 0 X rS X/-rs = 0.08. From guess and check we get X = 55% P2-7 (d) To achieve 80% conversion with a CSTR followed by a CSTR, the optimum arrangement is to have a CSTR with a volume to achieve a conversion of about 45%, or the conversion that corresponds to the minimum value of 1/-rs. Next is a PFR with the necessary volume to achieve the 80% conversion following the CSTR. This arrangement has the smallest reactor volume to achieve 80% conversion. For two CSTR’s in series, the optimum arrangement would still include a CSTR with the volume to achieve a conversion of about 45%, or the conversion that corresponds to the minimum value of 1/-rs, first. A second CSTR with a volume sufficient to reach 80% would follow the first CSTR. P2-7 (e) rs kC S CC and C C K M CS rs kC S 0.1 C S 0 C S K M CS 1 rs K M CS kC S 0.1 C S 0 C S 0.1 C S 0 CS 0.001 0.001 0.001 Let us first consider when CS is small. CS0 is a constant and if we group together the constants and simplify then 1 rs KM k1C S2 CS k 2 Cs since CS < KM 1 rs KM which is consistent with the shape of the graph when X is large (if CS is small X is k1C k 2 Cs 2 S large and as CS grows X decreases). Now consider when CS is large (X is small) As CS gets larger CC approaches 0: CC 0.1 C S 0 CS 0.001 and C S CS 0 If kC S CC then K M CS rs 1 rs K M CS kC S CC As CS grows larger, CS >> KM And 1 rs CS kC S CC 1 kCC And since CC is becoming very small and approaching 0 at X = 0, 1/-rs should be increasing with CS (or decreasing X). This is what is observed at small values of X. At intermediate levels of CS and X, these driving forces are competing and why the curve of 1/-rS has a minimum. P2-8 Irreversible gas phase reaction 2A + B 2C See Polymath program P2-8.pol. P2-8 (a) PFR volume necessary to achieve 50% conversion Mole Balance X2 V FA0 dX X 1 ( rA ) Volume = Geometric area under the curve of (FA0/-rA) vs X) V 1 400000 0.5 2 100000 0.5 V = 150000 m3 . P2-8 (b) CSTR Volume to achieve 50% conversion Mole Balance V V FA 0 X ( rA ) 0.5 100000 V = 50000m3 P2-8 (c) Volume of second CSTR added in series to achieve 80% conversion V2 FA0 ( X 2 X 1 ) ( rA ) V2 500000 (0.8 0.5) V2 = 150000m3 P2-8 (d) Volume of PFR added in series to first CSTR to achieve 80% conversion VPFR ( 1 400000 0.3) (100000 0.3) 2 VPFR = 90000m3 P2-8 (e) For CSTR, V = 60000 m3 (CSTR) Mole Balance V FA0 X ( rA ) 60000 ( 800000 X 500000 ) X X = 0.463 For PFR, V = 60000 m3 (PFR) Mole balance X V FA0 dX ( rA ) 0 X 60000 ( 800000 X 100000)dX 0 X = 0.134 P2-8(f) Real rates would not give that shape. The reactor volumes are absurdly large. P2-9 Problem 2-9 involves estimating the volume of three reactors from a picture. The door on the side of the building was used as a reference. It was assumed to be 8 ft high. The following estimates were made: CSTR h = 56ft d = 9 ft V = πr2h = π(4.5 ft)2(56 ft) = 3562 ft3 = 100,865 L PFR Length of one segment = 23 ft Length of entire reactor = (23 ft)(12)(11) = 3036 ft D = 1 ft V = πr2h = π(0.5 ft)2(3036 ft) = 2384 ft3 = 67,507 L Answers will vary slightly for each individual. P2-10 No solution necessary. P2-11 (a) The smallest amount of catalyst necessary to achieve 80 % conversion in a CSTR and PBR connected in series and containing equal amounts of catalyst can be calculated from the figure below. The lightly shaded area on the left denotes the CSTR while the darker shaded area denotes the PBR. This figure shows that the smallest amount of catalyst is used when the CSTR is upstream of the PBR. See Polymath program P2-11.pol. P2-11 (b) Calculate the necessary amount of catalyst to reach 80 % conversion using a single CSTR by determining the area of the shaded region in the figure below. The area of the rectangle is approximately 23.2 kg of catalyst. P2-11 (c) The CSTR catalyst weight necessary to achieve 40 % conversion can be obtained by calculating the area of the shaded rectangle shown in the figure below. The area of the rectangle is approximately 7.6 kg of catalyst. P2-11 (d) The catalyst weight necessary to achieve 80 % conversion in a PBR is found by calculating the area of the shaded region in the figure below. The necessary catalyst weight is approximately 22 kg. P2-11 (e) The amount of catalyst necessary to achieve 40 % conversion in a single PBR can be found from calculating the area of the shaded region in the graph below. The necessary catalyst weight is approximately 13 kg. P2-11 (f) P2-11 (g) For different (-rA) vs. (X) curves, reactors should be arranged so that the smallest amount of catalyst is needed to give the maximum conversion. One useful heuristic is that for curves with a negative slope, it is generally better to use a CSTR. Similarly, when a curve has a positive slope, it is generally better to use a PBR. P2-12 (a) Individualized Solution P2-12 (b) 1) In order to find the age of the baby hippo, we need to know the volume of the stomach. The metabolic rate, -rA, is the same for mother and baby, so if the baby hippo eats one half of what the mother eats then Fao (baby) = ½ Fao (mother). The Levenspiel Plot is shown: Autocatalytic Reaction 5 4.5 4 mao/-raM1 3.5 3 Mother 2.5 Baby 2 1.5 1 0.5 0 0 0.2 0.4 Conversion 0.6 0.8 Vbaby FaoX rA 1.36 *0.34 0.23m3 2 Since the volume of the stomach is proportional to the age of the baby hippo, and the volume of the baby’s stomach is half of an adult, then the baby hippo is half the age of a full grown hippo. Age 4.5 years 2 2.25 years 2) If Vmax and mao are both one half of the mother’s then 1 mA0mother 2 rAM 2 mAo rAM 2 and since rAM 2 rAM 2baby mAo rAM 2 vmax C A K M C A then 1 vmax C A 2 KM CA baby 1 rAM 2mother 2 1 mAo 2 1 rAM 2 2 mAo rAM 2 mother mother mAo will be identical for both the baby and mother. rAM 2 Assuming that like the stomach the intestine volume is proportional to age then the volume of the intestine would be 0.75 m3 and the final conversion would be 0.40 P2-12 (c) Vstomach = 0.2 m3 From the web module we see that if a polynomial is fit to the autocatalytic reaction we get: mA0 = 127X4 - 172.36X3 + 100.18X2 - 28.354X + 4.499 rAM 1 And since Vstomach = mA0 X, rAM 1 solve V= 127X5 - 172.36X4 + 100.18X3 - 28.354X2 + 4.499X = 0.2 m3 Xstomach = .067. For the intestine, the Levenspiel plot for the intestine is shown below. The outlet conversion is 0.178. Since the hippo needs 30% conversion to survive but only achieves 17.8%, the hippo cannot survive. P2-12 (d) PFR CSTR PFR: Outlet conversion of PFR = 0.111 CSTR: We must solve V = 0.46 = (X-0.111)(127X4 - 172.36X3 + 100.18X2 - 28.354X + 4.499) X=0.42 Since the hippo gets a conversion over 30% it will survive. P2-13 For a CSTR we have : V=X FA0 rA | X X f So the area under the FA 0 versus X curve for a CSTR is a rectangle but the height of rectangle rA corresponds to the value of FA 0 at X= Xf rA But in this case the value of FA 0 is taken at X= Xi and the area is calculated. rA Hence the proposed solution is wrong. CDP2-A (a) Over what range of conversions are the plug-flow reactor and CSTR volumes identical? We first plot the inverse of the reaction rate versus conversion. Mole balance equations for a CSTR and a PFR: CSTR: V FA 0 X rA PFR: V X dX 0 rA Until the conversion (X) reaches 0.5, the reaction rate is independent of conversion and the reactor volumes will be identical. i.e. VPFR 0.5 dX 0 rA FA0 0.5 dX rA 0 FA0 X rA VCSTR CDP2-A (b) What conversion will be achieved in a CSTR that has a volume of 90 L? For now, we will assume that conversion (X) will be less that 0.5. CSTR mole balance: V FA0 X rA v0 C A 0 X X rA V v0 C A 0 rA 3 5 m s 0.09m 3 3 mol 8 m .s 200 3 3 10 mol m 3 10 13 CDP2-A (c) This problem will be divided into two parts, as seen below: The PFR volume required in reaching X=0.5 (reaction rate is independent of conversion). V1 FA0 X rA v0 C A 0 X rA 1.5 1011 m 3 The PFR volume required to go from X=0.5 to X=0.7 (reaction rate depends on conversion). Finally, we add V2 to V1 and get: Vtot = V1 + V2 = 2.3 x1011 m3 CDP2-A (d) What CSTR reactor volume is required if effluent from the plug-flow reactor in part (c) is fed to a CSTR to raise the conversion to 90 % We notice that the new inverse of the reaction rate (1/-rA) is 7*108. We insert this new value into our CSTR mole balance equation: VCSTR FA0 X rA v0 C A 0 X rA 1.4 1011 m 3 CDP2-A (e) If the reaction is carried out in a constant-pressure batch reactor in which pure A is fed to the reactor, what length of time is necessary to achieve 40% conversion? Since there is no flow into or out of the system, mole balance can be written as: Mole Balance: rAV dN A dt Stoichiometry: N A N A0 (1 X ) Combine: rAV dX dt N A0 From the stoichiometry of the reaction we know that V = Vo(1+eX) and e is 1. We insert this into our mole balance equation and solve for time (t): rA V0 (1 X ) N A0 dt C A0 t 0 X 0 dX dt dX rA (1 X ) After integration, we have: t 1 C A0 ln(1 X ) rA Inserting the values for our variables: t = 2.02 x 1010 s That is 640 years. CDP2-A (f) Plot the rate of reaction and conversion as a function of PFR volume. The following graph plots the reaction rate (-rA) versus the PFR volume: Below is a plot of conversion versus the PFR volume. Notice how the relation is linear until the conversion exceeds 50%. The volume required for 99% conversion exceeds 4*1011 m3. CDP2-A (g) Critique the answers to this problem. The rate of reaction for this problem is extremely small, and the flow rate is quite large. To obtain the desired conversion, it would require a reactor of geological proportions (a CSTR or PFR approximately the size of the Los Angeles Basin), or as we saw in the case of the batch reactor, a very long time. CDP2-B Individualized solution CDP2-C (a) For an intermediate conversion of 0.3, Figure above shows that a PFR yields the smallest volume, since for the PFR we use the area under the curve. A minimum volume is also achieved by following the PFR with a CSTR. In this case the area considered would be the rectangle bounded by X =0.3 and X = 0.7 with a height equal to the CA0/-rA value at X = 0.7, which is less than the area under the curve. CDP2-C (b) CDP2-C (c) CDP2-C (d) For the PFR, CDP2-C (e) CDP2-D CDP2-D (a) CDP2-D (b) CDP2-D (c) CDP2-D (d) CDP2-D (e) CDP2-D (f) CDP2-D (g) CDP2-D (h) CDP2-E CDP2-F (a) Find the conversion for the CSTR and PFR connected in series. X -rA 1/(-rA) 0 0.2 5 0.1 0.0167 59.9 0.4 0.00488 204.9 0.7 0.00286 349.65 0.9 0.00204 490.19 CDP2-F (b) CDP2-F (c) CDP2-F (d) CDP2-F (e) CDP2-F (f) CDP2-F (g) Individualized solution The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 3-1 Solutions for Chapter 3 – Rate Laws P3-1 Individualized solution. P3-2 (a) Example 3-1 For, E = 60kJ/mol k 1.32 1016 exp T (K) For, E = 240kJ/mol 60000 J RT k (1/sec) 1/T k 1.32 1016 exp ln(k) T (K) 240000 J RT k (1/sec) 1/T ln(k) 310 1023100 0.003226 13.83918 310 4.78E-25 0.003226 -56.0003 315 1480488 0.003175 315 14.2087 2.1E-24 0.003175 -54.5222 320 2117757 0.003125 14.56667 320 8.77E-24 0.003125 -53.0903 325 2996152 0.003077 14.91363 325 3.51E-23 0.003077 -51.7025 330 4194548 330 1.35E-22 0.00303 15.25008 335 5813595 0.002985 15.57648 0.00303 -50.3567 335 4.98E-22 0.002985 -49.0511 3-2 P3-2 (b) No solution will be given P3-2 (c) A+ 1 1 B C 2 2 Rate law: rA rA 1 kC rB 1/2 kB 2 k A CA CB and kA rC 1/2 1 dm 3 12.5 s mol 1 dm 3 25 s mol 2 25CA CB 2 k B CA 2CB 1/2 kC CA 2CB 1/2 2 P3-3(a) Refer to Fig 3-3 The fraction of molecular collisions having energies less than or equal to 50 Kcal is given by the area under the curve, f(E,T)dE from EA = 0 to 50 Kcal. P3-3(b) The fraction of molecular collisions having energies between 10 and 20 Kcal is given by the area under the curve f(E,T) from EA = 10 to 20 Kcal. 3-3 P3-3(c) The fraction of molecular collisions having energies greater than the activation energy EA= 30 Kcal is given by the area under the curve f(E,T) from EA =30 to 50 Kcal. P3-4 (a) Note: This problem can have many solutions as data fitting can be done in many ways. Using Arrhenius Equation For Fire flies: T(in K) 294 1/T 0.003401 Flashes/ min 9 ln(flashe s/min) 2.197 298 0.003356 12.16 2.498 303 0.003300 16.2 2.785 Plotting ln (flashes/min) vs. 1/T, We get a straight line. See Polymath program P3-4-fireflies.pol. For Crickets: T(in K) 287.2 1/T 3 x10 3.482 chirps/ min 80 ln(chirps/ min) 4.382 293.3 300 3.409 3.333 126 200 4.836 5.298 Plotting ln (chirps/min) Vs 1/T, We get a straight line. Both, Fireflies and Crickets data follow the Arrhenius Model. ln y = A + B/T , and have the similar activation energy. See Polymath program P3-4-crickets.pol. P3-4 (b) For Honeybee: T(in K) V(cm/s) ln(V) 298 1/T 3 x10 3.356 0.7 -0.357 303 3.300 1.8 0.588 308 3.247 3 1.098 Plotting ln (V) vs. 1/T, almost straight line. 3-4 ln (V) = 44.6 – 1.33E4/T At T = 40oC (313K) At T = -5oC (268K) V = 6.4cm/s V = 0.005cm/s(But bee would not be alive at this temperature) See Polymath program P3-4-bees.pol. P3-4 (c) For Ants: T(in K) 1/T x10 283 3 V(cm/s) ln(V) 3.53 0.5 -0.69 293 3.41 2 0.69 303 3.30 3.4 1.22 311 3.21 6.5 1.87 Plotting ln (V) vs. 1/T, We get almost a straight line. See Polymath program P3-4-ants.pol. So activity of bees, ants, crickets and fireflies follow Arrhenius model. So activity increases with an increase in temperature. Activation energies for fireflies and crickets are almost the same. Insect Cricket Firefly Ant Honeybee Activation Energy 52150 54800 95570 141800 P3-4 (d) There is a limit to temperature for which data for any one of he insect can be extrapolate. Data which would be helpful is the maximum and the minimum temperature that these insects can endure before death. Therefore, even if extrapolation gives us a value that looks reasonable, at certain temperature it could be useless. P3-5 There are two competing effects that bring about the maximum in the corrosion rate: Temperature and HCN-H2SO4 concentration. The corrosion rate increases with increasing temperature and increasing concentration of HCN-H2SO4 complex. The temperature increases as we go from top to bottom of the column and consequently the rate of corrosion should increase. However, the HCN concentrations (and the HCN-H2SO4 complex) decrease as we go from top to bottom of the column. There is virtually no HCN in the bottom of the column. These two opposing factors results in the maximum of the corrosion rate somewhere around the middle of the column. 3-5 P3-6 Antidote did not dissolve from glass at low temperatures. P3-7 (a) If a reaction rate doubles for an increase in 10°C, at T = T1 let k = k1 and at T = T2 = T1+10, let k = k2 = 2k1. Then with k = Ae-E/RT in general, k1 k2 k1 e E 1 1 R T2 T1 E R or Ae E / RT1 and k2 ln k2 k1 1 T2 1 T1 Ae E / RT2 , or k2 k1 T1 T2 T1T2 ln Therefore: ln E R k2 k1 T1 T1 10 R T2 T1 T1 T1 10 ln 2 T1 T1 10 10 10 E R ln 2 which can be approximated by T 10 E 0.5 R ln 2 P3-7 (b) Equation 3-18 is k Ae E RT From the data, at T1 = 0°C, k1 k Dividing gives 2 k1 E R ln k2 k1 1 T2 1 T1 1.99 E e E 1 1 R T2 T1 Ae E / RT1 , and at T2 = 100°C, k2 , or RT1T2 k ln 2 T1 T2 k1 cal 273 K 373 K mol K .050 ln 100 K .001 7960 3-6 cal mol Ae E / RT2 A k1e E RT1 7960 10 3 min 1 exp 1.99 cal mol cal mol K 2100 min 1 273 K P3-7 (c) Individualized solution P3-8 From the given data k= rA(dm3/mol.s) T(K) rA/(4*1.5) 0.002 300 0.00033333 0.046 320 0.00766667 0.72 340 0.12 8.33 360 1.38833333 1/T ln (k) 0.003333 -8.00637 0.003125 -4.87087 0.002941 -2.12026 0.002778 0.328104 Plotting ln(k) vs (1/T), we have a straight line: Since, ln k = ln A - ( , therefore ln A = 41.99 and E/R = 14999 3-7 (a) Activation energy (E), E = 14999*8.314 =124700 J/mol = 124.7 kJ/mol (b) Frequency Factor (A), ln A = 41.99 A = 1.72X1018 (c) k = 1.72X1018 exp(- (1) Given T0 = 300K Therefore, putting T = 300K in (1), we get k(T0) = 3.33X10-4 Hence, k(T) = k(T0)exp[ P3-9 (a) From the web module we know that dX dt k (1 x) and that k is a function of temperature, but not a linear function. Therefore doubling the temperature will not necessarily double the reaction rate, and therefore halve the cooking time. P3-9 (b) When you boil the potato in water, the heat transfer coefficient is much larger, but the temperature can only be 100°C. When you bake the potato, the heat transfer coefficient is smaller, but the temperature can be more than double that of boiling water. P3-10 1) C2H6 → C2H4 + H2 Rate law: -rA = kC C2 H 6 2) C2H4 + 1/2O2 → C2H4O Rate law: -rA = kCC2 H 4 C 02 1/ 2 3) (CH3)3COOC(CH3)3 → C2H6 + 2CH3COCH3 A → B + 2C Rate law: -rA = k[CA – CBCC2/KC] 4) n-C4H10 ↔ I- C4H10 Rate law: -rA = k[ C nC4 H10 – C iC4 H10 /Kc] 5) CH3COOC2H5 + C4H9OH ↔ CH3COOC4H9 + C2H5OH A + B ↔ C + D Rate law: -rA = k[CACB – CCCD/KC] 3-8 P3-11 (a) 2A + B → C (1) (2) (3) (4) -rA = kCACB2 -rA = kCB -rA = k -rA = kCACB-1 P3-11 (b) 1/ 2 k1C H 2 C Br 2 Rate law: -rHBr = C HBr k2 C Br2 (1) H2 + Br2 → 2HBr (2) H2 + I2 → 2HI Rate law: -rA = k1CH 2 CI2 P3-12 a) we need to assume a form of the rate law for the reverse reaction that satisfies the equilibrium condition. If we assume the rate law for the reverse reaction (B->A) is = then: From Appendix C we know that for a reaction at equilibrium: KC At equilibrium, rnet 0, so: Solving for KC gives: 3-9 b) If we assume the rate law for the reverse reaction is then: From Appendix C we know that for a reaction at equilibrium: KC At equilibrium, rnet 0, so: Solving for KC gives: c) If we assume the rate law for the reverse reaction is then: 3-10 From Appendix C we know that for a reaction at equilibrium: KC At equilibrium, rnet 0, so: Solving for KC gives: P3-13 The rate at which the beetle can push a ball of dung is directly proportional to its rate constant, therefore -rA =c*k, where c is a constant related to the mass of the beetle and the dung and k is the rate constant k = A exp( From the data given -rA 6.5 13 18 T(K) 300 310 313 1/T 0.003333 0.003226 0.003195 ln k 1.871802 2.564949 2.890372 3-11 Refer to P3-8 (similar procedure) Therefore, A = 1.299X1011 E = 59195.68 J/mol k = 1.299X1011 exp(-7120/T) Now at T = 41.5 C = 314.5 K k = 19.12 cm/s Therefore, beetle can push dung at 19.12 cm/s at 41.5 C P3-14 Since the reaction is homogeneous, which means it involves only one phase. Therefore, So, option (4) is correct. P3-15 Assuming the reactions to be elementary: 2 Anthracene -> Dimer rA 2 k (C Anthracene CDimer ) KC where, Kc = k+/k- Similarly for the second reaction: 3-12 Norbornadiene Quadricyclane rNorbornadiene k (CNorbornadiene CQuadricyclane KC ) where, Kc = k+/k- P3-16 The mistakes are as follows: 1. For any reaction, the rate law cannot be written on the basis of the stoichiometric equation. It can only be found out using experimental data. 2. In the evaluation of the specific reaction rate constant at 100o C the gas constant that should have been used was 8.314 J K-1 mol -1. 3. In the same equation, the temperatures used should have been in K rather than oC. 4. The units for calculated k(at 100oC) are incorrect. 5. The dimension of the reaction rate obtained is incorrect. This is due to the fact that the rate law that has been taken is wrong. CDP3-A Polanyi equation: E = C – α(-ΔHR) We have to calculate E for the reaction CH3• + RBr CH3Br + R• Given: ΔHR = - 6 kcal/mol From the given data table, we get 6.8 = C – α (17.5) And, 6.0 = C – α (20) => C = 12.4 KJ/mol and α = 0.32 Using these values, and ΔHR = - 6 kcal/mol, we get E = 10.48 KJ/mol 3-13 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 4-1 Solutions for Chapter 4 –Stoichiometry P4-1 Individualized solution P4-2 (a) Example 4-1 Yes, water is already considered inert. P4-2 (b) Example 4-2 For 20% Conversion CD = same as example & CB = CAo (ѲB – XA/3) = 10 ( - ) = 2.33 mol/dm3 – ) = 0 mol/dm3 For 90 % Conversion CD = same as example & CB = CAo (ѲB – XA/3) = 10 ( The final concentration of glyceryl sterate is 0 instead of a negative concentration. Therefore 90 % of caustic soda is possible. P4-2 (c) Example 4-3 For the concentration of N2 to be constant, the volume of reactor must be constant. V = VO. Plot: 1 rA 0.5(1 0.14 X )2 (1 X )(0.54 0.5 X ) 1/(-ra) vs X 180 160 140 1/(-ra) 120 100 80 60 40 20 0 0 0.2 0.4 0.6 0.8 1 1.2 X The rate of reaction decreases drastically with increase in conversion at higher conversions. 4-2 P4-2 (d) Example 4-4 POLYMATH Report No Title 05-May-2009 Ordinary Differential Equations Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 epsilon -0.14 -0.14 -0.14 -0.14 2 FA0 1000. 1000. 1000. 1000. 3 k 9.7 9.7 9.7 9.7 4 K 930. 930. 930. 930. 5 KO2 38.5 38.5 38.5 38.5 6 KSO2 42.5 42.5 42.5 42.5 7 PO2 2.214 0.19639 2.214 0.1963901 8 PSO2 4.1 0.0115348 4.1 0.011535 9 PSO20 4.1 4.1 4.1 4.1 10 PSO3 0 0 4.754029 4.754029 11 rA -0.0017387 -0.0063092 5.915E-08 -1.659E-09 12 w 0 0 5.0E+05 5.0E+05 13 x 0 0 0.9975796 0.9975795 Differential equations 1 d(x)/d(w) = -rA/FA0 Explicit equations 1 FA0 = 1000 mol.hr-1 2 PSO20 = 4.1 3 K = 930 atm-1/2 4 KSO2 = 42.5 5 KO2 = 38.5 atm-1 6 k = 9.7 7 epsilon = -0.14 8 PSO3 = PSO20*x/(1+epsilon*x) 9 PO2 = PSO20*(1.08-x)/2/(1+epsilon*x) 10 PSO2 = PSO20*(1-x)/(1+epsilon*x) 11 rA = -k*(PSO2*PO2^0.5 - PSO3/K)/(1+(PO2*KO2)^0.5+PSO2*KSO2)^2 mol/hr.g.cat General 4-3 Total number of equations 12 Number of differential equations 1 Number of explicit equations 11 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 4-4 Therefore, catalyst weight required for 30% conversion is 1.611x105 g = 161.1 kg 4-5 Therefore, catalyst weight required for 60% conversion is 2.945x105 g = 294.5 kg Therefore, catalyst weight required for 99% conversion is 4.041x105 g = 404.1 kg P4-2 (e) Example 4-5 For a given conversion, concentration of B is lower in flow reactor than a constant volume batch reactor. Therefore the reverse reaction decreases. CT0 = constant and inerts are varied. N 2O4 2NO2 A ↔ 2B Equilibrium rate constant is given by: KC Stoichiometry: y A0 y A0 (2 1) CB,e 2 CA,e y A0 Constant volume Batch: CA N A0 (1 X) V0 CA0 (1 X) and CB 2N A 0 X V0 2CA 0 X Plug flow reactor: CA FA0 (1 X) v 0 (1 X) CA0 (1 X) and CB (1 X) 2FA0 X v 0 (1 X) 4-6 2CA0 X (1 X) CAO y AO PO RTO y AO 0.07176 mol /dm 3 Combining: For constant volume batch: KC CB,e 2 CA,e 2 4CAo X2 CAO (1 X) Xe KC (1 X e ) 4CA0 Xe K C (1 X e )(1 4C A0 For flow reactor: KC C B ,e 2 C A,e 2 4C Ao X2 C AO (1 X )(1 X) See Polymath program P4-2-e.pol. POLYMATH Results NLES Report (safenewt) Nonlinear equations [1] f(Xeb) = Xeb - (kc*(1-Xeb)/(4*Cao))^0.5 = 0 [2] f(Xef) = Xef - (kc*(1-Xef)*(1+eps*Xef)/(4*Cao))^0.5 = 0 Explicit equations [1] yao = 1 [2] kc = 0.1 [3] Cao = 0.07174*yao [4] eps = yao 4-7 Xe) Yinert Yao 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 0.95 0.956 Xeb Xef 1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.05 0.044 0.44 0.458 0.4777 0.5 0.525 0.556 0.5944 0.6435 0.71 0.8112 0.887 0.893 0.508 0.5217 0.537 0.5547 0.576 0.601 0.633 0.6743 0.732 0.8212 0.89 0.896 P4-3 Solution is in the decoding algorithm available separately from the author. P4-4 A y A0 (a) C B0 C A0 (b) C A C A0 CC C A0 0.1 X X 2 1 1 X 2 1 X 1 (c) C B (d) C B C A0 0.1 0.1 1 0.25 1 1 X 2 0.25 2 0.1 1 1 X 2 X 1 2 mol dm 3 1 X 1 1 1 B C 2 2 1 1 1 1 2 2 2 0.875 0.1 0.125 0.875 C A0 1 1 0.1 0.75 1 X 2 1 X 2 mol dm 3 4-8 C A0 0.086 0.0143 0.1 mol dm3 mol dm 3 mol dm 3 rA 4 (e) rC , rA 2 4 mol dm 3 min 2rC P4-5 (a) Liquid phase reaction, O CH2--OH CH2 - CH2 + H2O → CH2--OH A + B → C CAO = 16.13mol/dm3 CBO = 55.5 mol/dm3 Stoichiometric Table: Species Ethylene oxide Water Glycol Symbol A Initial CAO=16.13 mol/dm3 Change - CAOX B CBO= 55.5 mol/dm3, B =3.47 Remaining CA= CAO(1-X) = (1-X) lbmol/ft3 -CAOX CB = CAO( 0 CAOX =(3.47-X) lbmol/ft3 CC = CAOX = X lbmol/ft3 C Rate law: -rA = kCACB Therefore, 2 -rA = k C AO (1-X) ( At 300K E = 12500 cal/mol, k = 0.1dm3/mol.s CSTR = B -X) = k (16.13)2(1-X) (3.47-X) X = 0.9, 16.13 0.9 C AO X = 2 rA 0.1 16.13 1 0.9 3.47 0.9 2.186sec and, V = τ X FA0 = 2.186 X 200 liters = 437.2 liters At 350K, k2 = k exp((E/R)(1/T-1/T2))= 0.1exp((12500/1.987)(1/300-1/350)) = 19.99 dm3/mol.s Therefore, CSTR = 16.13 0.9 C AO X = 2 rA 19.99 16.13 1 0.9 3.47 0.9 and, V = τ X FA0 = 0.109 X 200 liters = 21.8 liters 4-9 0.109sec , B -X) P4-5 (b) Isothermal, isobaric gas-phase pyrolysis, C2H6 C2H4 + H2 A B + C Stoichiometric table: Species C2H6 C2H4 H2 symbol A B C Entering FAO 0 0 FTO=FAO Change -FAOX +FAOX +FAOX Leaving FA=FAO(1-X) FB=FAOX FC=FAOX FT=FAO(1+X) = yao = 1(1+1-1) = 1 v = vo(1+ X) => v = vo(1+X) P RT 1 6atm CAO = yAO CTO = yAO = = 0.067 kmol/m3 = 0.067 mol/dm3 3 0.082 m atm K .kmol 1100 K CA = FA v FAO (1 X ) vO (1 X ) C AO 1 X 1 X CB = FB v FAO ( X ) vO (1 X ) C AO X mol/dm3 1 X CC = FC v FAO ( X ) vO (1 X ) C AO X mol/dm3 1 X mol/dm3 Rate law: -rA = kCA= kCAO 1 X 1 X =0.067 k 1 X 1 X If the reaction is carried out in a constant volume batch reactor, =>( = 0) CA = CAO(1-X) mol/dm3 CB = CAO X mol/dm3 CC = CAO X mol/dm3 P4-5 (c) Isothermal, isobaric, catalytic gas phase oxidation, 1 O2 C2H4O 2 1 + B C 2 C2H4 + A 4-10 Stoichiometric table: B = FBO FAO y AO C AO CA 1 FAO 2 FAO CB FB v CC FC v Symbol A B Entering FAO FBO Change -FAOX C2H4O C 0 +FAOX 1 2 2 1 1 1 3 2 y AO CTO FA v Species C2H4 O2 y AO P RT FAO 1 X vO 1 X FAO B vO 1 X 2 X FAO X vO 1 X y AO FAO FTO - Leaving FA=FAO(1-X) 1 FB=FAO( B -X/2) FAOX 2 FAO FAO FBO FC=FAOX 2 3 0.33 2 3 6atm 0.082 atm.dm mol.K CAO 1 X 1 0.33 X 0.092 3 533K mol dm3 0.092 1 X 1 0.33 X 0.046 1 X 1 0.33 X 0.092 X 1 0.33 X If the reaction follow elementary rate law Rate law: rA kC AC 0.5 B rA 0.092 1 X k 1 0.33 X 0.046 1 X 1 0.33 X Change -FA0X -2FA0X FA0X Leaving FA=FA0(1-X) FB=FA0(θB-2X) Fc=FA0X P4-5 (d) Isothermal, isobaric, catalytic gas-phase reaction in a PBR C6H6 + 2H2 → C6H10 A + 2B → C Given: 0 50 dm 3 / min Stoichiometric Table: Species C6H6 H2 C6H10 Symbol A B C Entering FA0 FB0=2FA0 0 4-11 0.5 B C A0 CA CB CC FB 0 FA 0 2 FA 0 FA 0 2 P 1 RT 3 CT 0 y A0 FA 0 FT 0 y A0 FA 0 FA0 FB 0 1 3 6atm 1 0.0821 * (443K ) 3 0.055 dm3 atm mol K FA FA0 (1 X ) X) 0 (1 FB FA0 ( B 2 X ) X) 0 (1 FC FA0 X X) 0 (1 C A0 1 (1 2 1) 3 2 3 mol dm3 (1 X ) (1 23 X ) C A0 C A0 y A0 (2 2 X ) (1 23 X ) 2 * C A0 (1 X ) (1 23 X ) X 2 3 (1 X) Rate Law: NOTE: For gas-phase reactions, rate laws are sometimes written in terms of partial pressures instead of concentrations. The units of the rate constant, k, will differ depending on whether partial pressure or concentration units are used. See below for an example. rA ' kPA PB mol kgcat min 2 mol * atm * atm 2 3 kgcat min atm Notice that if you use concentrations in this rate law, the units will not work out. PA y A0 P ( y A0 C ) * RT rA kPA PB 2 2 C A RT kC AC B ( RT ) 3 4kC A0 3 (1 X ) 3 ( RT ) 3 (1 23 X ) 3 Design Equation for a fluidized CSTR: W W W FA0 X rA ' FA0 X (1 2 3 X )3 3 4kC A0 (1 X ) 3 ( RT ) 3 0 X (1 2 3 X )3 2 4kC A0 (1 X ) 3 ( RT ) 3 Evaluating the constants: k 53 mol at 300 K kgcat min atm3 At 170°C (443K), 4-12 k 443 k 300 EA 1 R T300 1 T443 J 1 mol 53 J 300 K 8.314 mol K 80000 1 443K 1663000 mol kgcat min atm Plugging in all the constants into the design equation: X = 0.8 3 W 3 2 50 dm min 0.8 (1 3 0.8) 3 mol mol 2 atm 4 1663000 kgat min (0.055 dm 0.8) 3 (0.0821 dm 443K ) 3 3 ) (1 mol K atm3 5.25 10 7 kgcat At 270°C (543K), k 543 k 300 EA 1 R T300 1 T543 J 1 mol 53 J 300 K 8.314 mol K 80000 1 543K 9079000 mol Plu kgcat min atm gging in all the constants into the design equation: X = 0.8 3 W 3 2 50 dm min 0.8 (1 3 0.8) 3 3 mol mol 2 atm 4 9079000 kgat min (0.055 dm 0.8) 3 (0.0821 dm 3 ) (1 mol K 543K ) atm3 5.22 10 8 kgcat P4-6 (a) Let A = ONCB B = NH3 A + 2B -rA C = Nibroanaline D = Ammonium Chloride C+D kC ACB P4-6 (b) Species A B C D Entering FA0 FB0 = ΘBFA0 =6.6/1.8 FA0 0 0 Change - FA0X -2 FA0X FA0X FA0X P4-6 (c) For batch system, CA=NA/V -rA = kNANB/V2 P4-6 (d) 4-13 Leaving FA0(1-X) FB= FA0(ΘB – 2X) FC= FA0X FD=FA0X -rA kC ACB FA NA V NA V0 N A0 1 X V0 FB NB V NB V0 N A0 V0 rA kC A2 0 1 X B CB 0 C A0 6.6 1.8 C A0 1.8 kmol m3 rA k 1.8 2 B B FA v FA v0 C A0 1 X 2 X , CB FB v0 C A0 C A0 1 X , C A 2X C A0 B B 2X 3.67 1 X 3.67 2 X P4-6 (e) 1) At X = 0 and T = 188°C = 461 K 2 A0 rA0 kC rA0 0.0202 m3 kmol 0.0017 1.8 3 kmol min m B 2 3.67 kmol m3 min 2) At X = 0 and T = 25C = 298K k k O exp E 1 R TO 1 T cal m 1 mol k 0.0017 exp cal kmol. min 461 1.987 mol.K m3 2.03 10 6 kmol. min 11273 3 1 298 -rAO = kCAOCBO = 2.41 X 10-5 kmol/m3min 3) k k0 exp E 1 R T0 1 T 4-14 0.0202 kmol m 3 min 2X k cal m 1 mol 0.0017 exp cal kmol min 461 K 1.987 mol K k 0.0152 11273 3 1 561 K m3 kmol min rA0 kC A0CB 0 rA 0.0152 m3 kmol 1.8 3 kmol min m rA 0.1806 kmol m3 min 6.6 kmol m3 P4-6 (f) rA = kCAO2(1-X)(θB-2X) At X = 0.90 and T = 188C = 461K 1) at T = 188 C = 461 K rA m3 0.0017 kmol. min 0.00103 kmol 1.8 3 m 2 1 0.9 3.67 2 0.9 kmol m 3 min 2) at X = 0.90 and T = 25C = 298K rA 2.03 10 1.23 10 6 6 m3 kmol. min kmol 1.8 3 m 2 1 0.9 3.67 2 0.9 kmol m 3 min 3) at X = 0.90 and T = 288C = 561K rA m3 0.0152 kmol. min 0.0092 kmol 1.8 3 m 2 1 0.9 3.67 2 0.9 kmol m 3 min P4-6 (g) FAO = 2 mol/min 1) For CSTR at 25oC -rA 1.23 10 6 kmol m 3 min 4-15 FAO 1 X rA X 0.9 V 2mol / min 0.1 mol 1.23 10 3 3 m min 2)At 288oC, -rA V 0.0092 162.60m 3 kmol m 3 min FAO 1 X rA X 0.9 2mol / min 0.1 mol 0.0092 3 m min 21.739m 3 P4-7 C6H12O6 + aO2 + bNH3 → c(C4.4H7.3N0.86O1.2) + dH2O + eCO2 To calculate the yields of biomass, you must first balance the reaction equation by finding the coefficients a, b, c, d, and e. This can be done with mass balances on each element involved in the reaction. Once all the coefficients are found, you can then calculate the yield coefficients by simply assuming the reaction proceeds to completion and calculating the ending mass of the cells. P4-7 (a) Apply mass balance For C 6 = 4.4c + e For N b = 0.86c For O For H 6 + 2a = 1.2c + d + 2e 12 + 3b = 7.3c + 2d Also for C, 6(2/3) = 4.4c which gives c = 0.909 Next we solve for e using the other carbon balance 6 = 4.4 (0.909) + e e=2 We can solve for b using the nitrogen balance b = 0.86c = 0.86* (0.909) b = 0.78 Next we use the hydrogen balance to solve for d 12 + 3b = 7.3c + 2d 12 + 3(0.78) = 7.3(0.909) + 2d 4-16 d = 3.85 Finally we solve for a using the oxygen balance 6 + 2a = 1.2c + d + 2e 6 + 2a = 1.2(0.909) + 3.85 + 2(2) a = 1.47 P4-7 (b) Assume 1 mole of glucose (180 g) reacts: Yc/s= mass of cells / mass of glucose = mass of cells / 180 g mass of cells = c*(molecular weight) = 0.909 mol* (91.34g/mol) mass of cells = 83.12 g Yc/s = 83.12 g / 180 g Yc/s = 0.46 Yc/o2 = mass of cells / mass of O2 If we assume 1 mole of glucose reacted, then 1.47 moles of O2 are needed and 83.12 g of cells are produced. mass of O2 = 1.47 mol * (32 g/mol) mass of O2 = 47.04 g Yc/o2 = 83.12 g /47.04 g Yc/o2 =1.77 P4-8 (a) Isothermal gas phase reaction. 1 N2 2 3 H2 2 NH 3 Making H2 as the basis of calculation: H2 1 N2 3 A 1 B 3 2 NH 3 3 2 C 3 Stoichiometric table: Species H2 N2 Symbol A B Initial FAO NH3 C 0 FBO= B FAO 4-17 change -FAOX -FAOX/3 Leaving FA=FAO(1-X) +2FAOX/3 FC=(2/3)FAOX FB=FAO( B -X/3) P4-8 (b) C AO 2 1 1 3 3 2 3 y AO 2 3 0.5 1 3 16.4atm 0.5 0.082 atm.dm mol.K = 0.2 mol/dm3 3 500 K CH 2 CA C AO 1 X 1 X 0.2 1 X X 1 3 CNH3 CC 2 C AO X 3 1 X 2 3 0.1mol / dm3 0.2 X X 1 3 0.1mol / dm3 P4-8 (c) kN2 = 40 dm3/mol.s (1) For Flow system: 1 rN 2 k N2 CN2 2 3 CH 2 1 40 C AO X 1 3 X 1 3 2 3 rN 2 1.6 2 3 2 2 1 X X 1 3 2 1 X X 1 3 (2) For batch system, constant volume. 4-18 1 rN2 k N2 CN2 CA NA V CA C A0 1 X CB NB V 3 2 CH 2 2 N A0 1 X V0 NA V0 N A0 B2 X 3 V0 X 3 C H 2O 1 1 rN2 40 C A0 X 3 1.6 1 X 1 3 2 1 2 1 X 2 3 1 X 3 2 2 P4-9 (a) Liquid phase reaction assume constant volume Rate Law (reversible reaction): rA k C AC B CC KC Stoichiometry: CA C A 0 1 X , CB C A0 1 X , CC C A0 X To find the equilibrium conversion, set -rA = 0, combine stoichiometry and the rate law, and solve for Xe. C AC B K C CC C A2 0 1 X e 2 X e2 2 Xe 0.80 KC C A0 X e 1 Xe 1 0 C A0 K C To find the equilibrium concentrations, substitute the equilibrium conversion into the stiochiometric relations. CA C A0 1 X CB C A0 1 X mol 1 0.80 dm3 mol 2 3 1 0.80 dm 2 mol dm3 mol 0.4 3 dm 0.4 4-19 CA C A0 X 2 mol mol *0.80 1.6 3 3 dm dm P4-9 (b) Stoichiometry: y A0 1 3 1 2 and CA NA V N A0 1 X V0 1 CC NC V 3 N A0 X V0 1 X C A0 X C A0 0 C 1 X 1 2X 3X 1 2X Combine and solve for Xe. K C C A0 3 1 Xe 3X e C A0 1 2Xe 1 2Xe KC 1 X e 1 2 X e 4 Xe 2 27CA2 0 X e3 27C A2 0 X e3 3 X e 1 0 KC 0.58 Equilibrium concentrations: C A0 P0 RT0 CA 0.305 CC 10 atm dm3 atm 400 K 0.082 mol K 1 0.58 1 2 0.58 3 0.58 0.305 1 2 0.58 0.059 0.246 0.305 mol dm3 mol dm3 mol dm3 P4-9 (c) Same reaction, rate law, and initial concentration as part (b) gas phase, batch reaction. Stoichiometry: CA NA V N A0 1 X V0 C A0 1 X 4-20 CC NC V 3 N A0 X V0 3C A0 X Combine and solve for Xe KC C A0 1 X e Xe 3 3CA0 X e 0.39 Equilibrium concentrations CA 0.305 1 0.39 CC 0.305 0.39 mol dm3 mol 0.36 3 dm 0.19 P4-9 (d) Gas phase reaction in a constant pressure, batch reactor Rate law (reversible reaction): rA CC3 KC k CA Stoichiometry: y A0 1 3 1 2 and CA NA V N A0 1 X V0 1 CC NC V 3 N A0 X V0 1 X 1 X C A0 X 0 C 1 2X 3C A0 X 1 2X Combine and solve for Xe: K C C A0 1 X e 1 2Xe Xe 3C A0 X e 1 2Xe 3 0.58 Equilibrium concentrations: CA 0.305 1 0.58 1 2 0.58 0.059 mol dm3 4-21 3 0.305 0.58 CC 0.246 1 2 0.58 mol dm3 P4-10 Given: Gas phase reaction A + B 8C in a batch reactor fitted with a piston such that V = 0.1P0 k 1.0 ft 3 2 lb mol 2 sec kC A2 CB rA NA0 = NB0 at t = 0 V0 = 0.15 ft3 T = 140°C = 600°R = Constant P4-10 (a) N A0 N A0 N B 0 y A0 0.5 8 1 1 6 y A0 3 Now V Therefore NA rA V0 P0 T P T0 1 10V02 1 10V V N A0 1 X 2 A kC CB kN A2 N B V3 X and T T0 1 , P0 10V0 , and P 10V X or V2 V02 1 NB N A0 kN A3 0 1 X V03 1 X B X X B 3 N A0 3 2 Therefore 4-22 N B0 N A0 y A0 P0 V0 RT 1 1 X y P k A0 0 RT rA rA 5.03*10 3 3 1 X 2 1 X 9 1 3X 3 3 2 lb mol ft 3 sec P4-10 (b) V2 V02 1 0.22 0.152 1 X X X 0.259 rA 8.63*10 10 lb mol ft 3 sec P4-11 (1) For any reaction ,we cannot write the rate law on the basis of the stochiometric equation. The rate law is to be obtained from the experimental data. It has been mentioned as an elementary reaction in the problem statement but in the proposed solution the rate law is based on the reaction equation that has been divided by stoichiometric coefficient of A. (2) The value of calculated is incorrect. = yA0δ = 0.6 (3+5-2-3) = 1.8 is the correct value. (3) The expression for CA and CB will therefore be, C A0 1 X CA 1 X C A0 1 CB 1 2 X 3 X (4) According to the system of units being used in the calculations, R = 0.0821 atm. Liter/ mol & Temperature = 700 K should be used. 4-23 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 5-1 Solutions for Chapter 5: Isothermal Reactor Design- Conversion P5-1 Individualized solution. P5-2 (a) Example 5-1 There would be no error! The initial liquid phase concentration remains the same. P5-2 (b) Example 5-2: For n equal sized CSTRs (volume Vi each) with equal feed FAi0 = FA0/n CSTR mole balance on any reactor: Since FAi0 = FA0/n rA= kCA= kCAO(1-X) (1) For single CSTR with volume nVI and feed rate FA0 CSTR mole balance: rA= kCA= kCAO(1-X) (2) From equation (1) and (2), Xi = X. Therefore, we can generalize that the conversion achieved in any one of the parallel reactors with volume V i and feed rate of FA0/n will be identical to the conversion achieved in one large CSTR of volume nVi and feed rate FA0. P5-2 (c) Example 5-3 For 50% conversion, X = 0.5 and k = 3.07 sec-1 at 1100 K (from Example 5-3) 5-2 FB = 200X106 / (365 X 24 X 3600 X 28) lbmol/sec = 0.226 lbmol/sec F 0.026 FAO = B 0.452lbmol / sec Also, C AO 0.00415lbmol / ft 3 X 0.5 Now, we have from the example V FA0 kC A0 1 ln 1 1 X X 0.452lbmol / sec 3.07sec 1 X 0.00415lbmol / ft 3 1 1 ln 1 1 0.5 1X 0.5 = 35.47 X 0.886 ft3 = 31.44 ft3 Now, n = 31.44 ft3/0.0205 ft2 X40 ft = 38.33 So, we see that for lower conversion and required flow rate the volume of the reactor is reduced. P5-2 (d) Example 5-4 New Dp = 3D0/4 Because the flow is turbulent o 1 Dp 1 2 y Now, 1 1 2 oL Po Dp 2 D p1 2 L Po 0.0775 1 2 1 0.75 0.1033 atm 2 X 0.103 X 60 ft ft 1 10atm 1 2 1 0.24 2 0 , so too much pressure drop P = 0 and the flow stops. P5-2 (e) Example 5-5 For P = 60atm, CAO = 0.0415 lbmol/ft3 ( C AO y AO PO RTO 60 ) 0.73 1980 5-3 Using equation E-4-3.6, for X = 0.8 We see that the only thing that changes is CA0 and it increases by a factor of 10, therby decreasing the volume by a factor of 10. 1 P V P5-2 (f) Example 5-6 For turbulent flow 2 1 and Dp 1 P0 DP1 DP 2 P01 P02 1 1 1 1 5 1 5 1 Therefore there is no change. P5-2 (g) Example 5-3, Using ASPEN, we get (Refer to Aspen Program P5-2g from polymath CD) (1) At 1000K, for the same PFR volume we get only 6.2% conversion. While at 1200K, we get a conversion of nearly 100%. This is because the value of reaction constant ‘k’ varies rapidly with reaction temperature. (2) Earlier for an activation energy of 82 kcal/mol we got approx. 81% conversion. For activation energy of 74 kcal/mol keeping the PFR volume the same we get a conversion of 71.1%. While for an activation energy of 90 kcal/mol we get a conversion of 89.93%. (3) On doubling both flow rate and pressure we find that the conversion remains the same. P5-2 (h) Individualized solution. P5-2 (i) Individualized solution. P5-3 Solution is in the decoding algorithm given with the modules. 5-4 P5-4 We have to find the time required to cook spaghetti in Cuzco, Peru. Location Ann Arbor Boulder Cuzco Elevation (km) 0.21 1.63 3.416 Pressure (mm Hg) 739 625 493 Boiling Point (°C) 99.2 94.6 88.3 Time (min) 15 17 ? Assume reaction is zero order with respect to spaghetti conversion: E rA dC A dt Ae RT k so that CA CC Ae E RT t A0 For complete conversion (i.e.: well cooked) CA = 0 at time t. Therefore E RT C A0 tAe C A0 A te E RT ln C A0 A ln k ln t E 1 R Tb Now, plot the natural log of the cooking time versus 1/Tb and get a linear relationship. Extrapolation to Tb = 88.3°C = 361.45 K yields t = 21 minutes. 5-5 P5-5 (a) The blades makes two equal volumes zones of 500gal each rather than one ‘big’ mixing zone of 1000gal. So, we get 0.57 as conversion instead of 0.5. 5-6 P5-5 (b) A CSTR is been created at the bend due to back mixing, so the effective arrangement is a PFR is in series with a CSTR. CSTR zone due to back mixing A→B k = 5 min-1 vo = 5 dm3/min. Xexpected = 0.632 Xactual = 0.618 X V FAO dX rA 0 vo 1 5 1 = ln ln k 1 X Expected 5 1 .632 1.0 Now, For PFR, VP For CSTR, Also, ln FAO ( X actual rA VC VP V 1 ………………………………….(1) 1 X1 VC V X1 ) X actual X 1 ……………(2) 1 X actual 1 ………………………………………..(3) Solving 1, 2 and 3 by using polymath, See Polymath program P5-5-b.pol. Calculated values of NLE variables Variable Value f(x) Initial Guess 1 Vc 0.3001282 -2.831E-15 1. 5-7 2 X1 0.503351 7.864E-11 0 Variable Value 1 V 1. 2 Vp 0.6998718 3 X2 0.618 Nonlinear equations 1 f(X1) = ln(1/(1-X1)) -Vp = 0 2 f(Vc) = (X2-X1)/(1-X2) - Vc = 0 Explicit equations 1 V=1 2 X2 = .618 3 Vp = V - Vc General Settings Total number of equations 5 Number of implicit equations 2 Number of explicit equations 3 Elapsed time 0.0000 sec Solution method SAFENEWT Max iterations 150 Tolerance F 0.0000001 Tolerance X 0.0000001 Tolerance min VC = 0.3 dm 0.0000001 3 ; VP = 0.7 dm3 ; X1 = 0.5 P5-5 (c) CAO = 2 mol/dm3 A B Assuming 1st order reaction, C AO X rA For CSTR, -rA = kCA = kCAO(1-X) => X 1 X k 0.4 0.6 X For PFR, V FA0 => X PFR 0.67 dX , k kC 1 X A0 0 1 exp( X dX 1 X 0 k ) =1-exp(-0.67) = 0.486 Now assuming 2nd order reaction, 5-8 For CSTR, Now, assuming 2nd order reaction, C AO X rA For CSTR, rA 2 kC A2 = kC AO 1 X => kC AO X 1 X 2 0.4 0.62 X 1 dX kC AO 0 1 X 2 For PFR, => X 1 1 1 kC AO 2 1.111 1 X kC AO 1 X 1 1 .526 2.111 So, while calculating PFR conversion they considered reaction to be 1st order. But actually it is a second order reaction. P5-5 (d) A graph between conversion and particle size is as follows: Originally we are at point A in graph, when particle size is decreased by 15%, we move to point C, which have same conversion as particle size at A. But when we decrease the particle size by 20%, we reach at point D, so a decrease in conversion is noticed. Also when we increase the particle size from position A, we reach at point B, again there is a decrease in the conversion. 5-9 P5-6 (a) (3) 50% (Liquid phase reactions do not depend on pressure) (b) (2) <50% (Low concentration if we lower the pressure) 2 kC A0 1 X rA (c) 1 X 2 , C A02 2 1 C A01 , low rate 2 (1) >0.234 2 rA kC A0 1 X rA ky 2 y2 y2 1 k true y 2 k true 2 k 0.234 0.234 0.234 y2 P5-7 (a) Ans. (1) X > 0.5 ~ 1 D Increase D, decrease , increase X. (b) Ans. (3) Xe = 0.75 Xe (c) KC 1 KC 3 1 3 Ans. (3) remain the same 5-10 0.75 KC CA C Ae C A0 1 X e y 1 X e C A0 X e y Xe Xe is not a function of . (d) Ans. (3) remain the same Xe is not a function of . (e) Ans. (4) insufficient information to tell Xe dp P5-8 (a) X V kC A2 0 1 X 2 10 5-11 dX dV X 1 X rA FA0 2 kC AO (1 X )2 FA0 kC A2 0V FA0 X=0.85 So, considering the above results, we will choose a CSTR. P5-8 (b) P5-8 (c) P5-8 (d) 1) CSTR and PFR are connected in series: 5-12 (200dm3 )(0.07dm3 / mol.min)(1mol / dm3 ) 2 (1 X ) 2 10mol / min X CSTR Solving the quadratic equation, XCSTR = 0.44 For PFR, FA0 dX dV rA (0.07dm3 / mol / min)C AO (1 X )(1 X )2 dV 10 mole / min dX X (0.07dm3 / mol / min)(1mol / dm3 )2 (800dm3 ) 10mole / min dX (1 X )3 0.44 X 0.736 2) when CSTR and PFR are connected in parallel, X CSTR (200dm3 )(0.07dm3 / mol.min)(1mol / dm3 ) 2 (1 X ) 2 5mol / min . XCSTR = 0.56 For PFR, X dX (1 X )2 0 (0.07dm3 / mol.min)(1mol / dm3 )2 (800dm3 ) 5mol / min XPFR = 0.92 Hence, final conversion X = 0.56 0.92 =0.74 2 P5-8 (e) To process the same amount of species A, the batch reactor must handle 5dm3 2M min 60 min hr 24h day 14400 mol day If the reactants are in the same concentrations as in the flow reactors, then V 14400 mol day 1dm3 mol 14400 dm3 day So the batch reactor must be able to process 14400 dm3 every 24 hours. 5-13 Now we find the time required to reach 90% conversion. Assume the reaction temperature is 300K. rAV N A0 dX dt kC A2 0 1 X V N A0 tR N N A0 X , and since A0 2 V VkC A0 1 X tR 1 X kC A0 1 X C A0 1 0.9 dm mol 0.1 4.2 *1 mol hr dm3 3 2.14hr Assume that it takes three hours to fill, empty, and heat to the reaction temperature. tf = 3 hours ttotal = tR + tf ttotal = 2.14hours + 3 hours = 5.14 hours. Therefore, we can run 4 batches in a day and the necessary reactor volume is 14400dm3 4 3600dm3 Referring to Table 1-1 and noting that 3600 dm3 is about 1000 gallons, we see that the price would be approximately $85,000 for the reactor. P5-8 (f) The points of the problem are: 1) To note the significant differences in processing times at different temperature (i.e. compare part (b) and (c)). 2) That the reaction is so fast at 77°C that a batch reactor is not appropriate. One minute to react and 180 to fill and empty. 3) Not to be confused by irrelevant information. It does not matter if the reactor is red or black. P5-9 PFR dX dV rA FA0 kCA0 1 X C A0 0 1 X 5-14 k 1 X X 0 1 X 1 0 X dX 1 X 1 k 1 ln 1 y A0 k 1 2 2s 11 1 1 1 1 1 1 ln 0.8 1 0.8 2 1.61 0.8 2 X 1 X 5 dm 3 s 1 k 0 10dm 3 k dV k 1.209 at 300K CSTR FA0 X V 0C A0 X rA 0X 1 1 X kC A0 1 1 2 X k1 X X 1 1 1 0.5 k 1 X1 X 1 X 1 0.8 1 0.5 0.8 2 0.2 2.8 ln ln k2 E 1 1 k1 R T1 T2 2.8 E 1 1 E 1.21 R 300 320 R 320 300 E R 300 320 20 ln 2.8 1.21 E 8010 5-15 20 , R 1.987 cal mol cal mol K P5-10 A kC A0 1 X X 0C A0 1 dX dV kV 3B 1 ln 0 1 X 1 3 1 2 y A0 kV V0 1 1 1 ln FA0 X 2 X1 rA2 V X 0C A0 X 2 V 1 X2 1 X2 kC A0 1 X 2 X1 1 1 X2 k 1 0.5 1 0.5 X 22 k 0.886 X2 1 X1 X2 X 2 X1 1 X 2 1 X2 k X1 X1 k 0 X 22 1.386X 2 1.386 0 X2 1.386X 2 1.386 2 4 1.386 2 X2 0.673 P5-11 (a) POLYMATH Report Ordinary Differential Equations 04-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 w 0 0 2000. 2000. 2 x 0 0 0.9978192 0.9978192 3 FBuO 50. 50. 50. 50. 4 PBuO 10. 10. 10. 10. 5 PBu 10. 0.0109159 10. 0.0109159 6 k 0.054 0.054 0.054 0.054 7 K 0.32 0.32 0.32 0.32 8 rBu -0.0306122 -0.0421872 -0.0005854 -0.0005854 5-16 Differential equations 1 d(x)/d(w) = -rBu / FBuO Kgcat-1 Explicit equations 1 FBuO = 50 Kmol.hr-1 2 PBuO = 10 atm 3 PBu = PBuO * (1 - x) / (1 + x) atm 4 k = 0.054 kmol.kgcat-1.hr-1.atm-1 5 K = 0.32 atm-1 6 rBu = -k * PBu / (1 + K * PBu) ^ 2 Kmol.kgcat-1.hr-1 General Total number of equations 7 Number of differential equations 1 Number of explicit equations 6 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 5-17 5-18 Hence, weight of catalyst required for 80% conversion is 1054.1 kg . P5-11 (b) Differential Mole Balance: FBuO = -rBuʹ PBu = PBuO Rate equation : Here, -rBuʹ = K*PBu For Fluidized CSTR : 5-19 Therefore, w = FBuo*X Given, X = 0.8 FBuO = 50 Kmol.hr-1 KBu = 0.32 atm-1 PBuO = 10 atm Therefore, putting the values in the above equation w = 50*0.8 = 1225 Kg Therefore, 1225 Kg of fluidized CSTR catalyst weight is required to achieve 80% conversion. P5-11 (c) With pressure drop parameter alpha = 0.0006 kg-1 POLYMATH Report Ordinary Differential Equations 04-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 w 0 0 1100. 1100. 2 x 0 0 0.7750365 0.7750365 3 y 1. 0.2689385 1. 0.2689385 4 FBuO 50. 50. 50. 50. 5 f 1. 1. 6.600157 6.600157 6 PBuO 10. 10. 10. 10. 7 PBu 10. 0.3408456 10. 0.3408456 8 k 0.054 0.054 0.054 0.054 9 K 0.32 0.32 0.32 0.32 10 rBu -0.0306122 -0.0421871 -0.0149635 -0.0149635 11 alpha 0.0006 0.0006 0.0006 0.0006 Differential equations 1 d(x)/d(w) = -rBu / FBuO 5-20 Kgcat-1 2 d(y)/d(w) = -alpha * (1 + x) / 2 / y Kgcat-1 Explicit equations 1 FBuO = 50 Kmol.hr-1 2 f = (1 + x) / y 3 PBuO = 10 atm 4 PBu = PBuO * (1 - x) / (1 + x) * y atm 5 k = 0.054 kmol.kgcat-1.hr-1.atm-1 6 K = 0.32 atm-1 7 rBu = -k * PBu / (1 + K * PBu) ^ 2 Kmol.kgcat-1.hr-1 8 alpha = 0.0006 Kg-1 General Total number of equations 10 Number of differential equations 2 Number of explicit equations 8 Elapsed time 1.157 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 5-21 So, we see the maximum rate in case with pressure drop is at catalyst weight equal to around 600 Kg. 5-22 To achieve 70% conversion, catalyst weight required is 932.3 kg . In case of (a), 915.5 kg of catalyst is required to achieve 70% conversion. 5-23 P5-11 (d) Individualized solution P5-11 (e) Individualized solution P5-12 (a) P5-12 (b) P5-12 (c) For α = 0.001dm-3 See Polymath program P5-12-c.pol. 5-24 POLYMATH Results Calculated values of the DEQ variables Variable v x y Co esp alfa C k r fo initial value 0 0 1 0.3 2 0.001 0.3 0.044 -0.0132 2.5 minimal value 0 0 0.1721111 0.3 2 0.001 0.0077768 0.044 -0.0132 2.5 maximal value 500 0.656431 1 0.3 2 0.001 0.3 0.044 -3.422E-04 2.5 Differential equations as entered by the user [1] d(x)/d(v) = -r/fo [2] d(y)/d(v) = -alfa*(1+esp*x)/(2*y) Explicit equations as entered by the user [1] Co = 0.3 [2] esp = 2 [3] alfa = 0.001 [4] C = Co*(1-x)*y/(1+esp*x) [5] k = 0.044 [6] r = -k*C [7] fo = 2.5 At V = 500, x = 0.66, y = 0.17 P5-12 (d) Individualized solution P5-12 (e) A B 2C 5-25 final value 500 0.656431 0.1721111 0.3 2 0.001 0.0077768 0.044 -3.422E-04 2.5 Using these equations in Polymath we get the volume to be 290 dm3. For a batch reactor. 5-26 P5-12 (f) A B 2C Using Polymath to solve the differential equation gives a volume of 290 dm3 See Polymath program P5-12-f.pol. PFR with pressure drop: Alter the Polymath equations from part (c). See Polymath program P5-12-f-pressure.pol. POLYMATH Results 5-27 Calculated values of the DEQ variables Variable v x y Kc alfa Cao k esp fo r initial value 0 0 1 0.025 0.001 0.3 0.044 2 2.5 -0.0132 minimal value 0 0 0.3181585 0.025 0.001 0.3 0.044 2 2.5 -0.0132 maximal value 500 0.5077714 1 0.025 0.001 0.3 0.044 2 2.5 -1.846E-04 ODE Report (STIFF) Differential equations as entered by the user [1] d(x)/d(v) = -r/fo [2] d(y)/d(v) = -alfa*(1+esp*x)/(2*y) Explicit equations as entered by the user [1] Kc = .025 [2] alfa = 0.001 [3] Cao = 0.3 [4] k = 0.044 [5] esp = 2 [6] fo = 2.5 [7] r = -(k*Cao/(1+esp*x))*(4*Cao^2*x^3/((1+esp*x)^2*Kc)) 5-28 final value 500 0.5077714 0.3181585 0.025 0.001 0.3 0.044 2 2.5 -1.846E-04 At V = 500 dm3 X = 0.507 and y = 0.381 P5-13 A To = 300K KCO (300K)= 3.0 V = 1000gal = 3785.4 dm3 FAO X rA V Mole balance: rA Rate law: Stoichiometry: C A V Now using: where B kO C and C AO 1 X FAO 2 kO C AO 1 X 2 V 1 X Z 2902.2dm3 , Z V Z z KC C BO X X2 KC 2 FAO kOC AO 2 k kO CB X Z z C B2 KC 2 A X2 KC 3785.4 0.62 0.4 X k ko exp X 1 X 2 E 1 R TO exp K CO exp 2 X KC 1 T H RX 1 R TO E 1 R T0 1 T f X 0 V and 1 T Solving using polymath to get a table of values of X Vs T. See Polymath program P5-13.pol. POLYMATH Results NLE Solution Variable X To Value 0.4229453 300 f(x) 3.638E-12 Ini Guess 0.5 5-29 0.42 3 Z z X 1 X 2 X2 KC T z V E R y Kco Hrx Kc 305.5 2902.2 3785.4 1.5E+04 2 1.5684405 3 -2.5E+04 1.4169064 NLE Report (safenewt) Nonlinear equations 0.43 0.42 [1] f(X) = (z/y)*X/((1-X)^2 - X^2/Kc) -V = 0 Explicit equations 0.41 [1] To = 300 [2] T = 305.5 [3] z = 2902.2 [4] V = 3785.4 [5] E = 15000 [6] R = 2 [7] y = exp(E/R*(1/To-1/T)) [8] Kco = 3 [9] Hrx = -25000 [10] Kc = Kco*exp(Hrx/R*(1/To-1/T)) X 0.4 0.39 0.38 0.37 0.36 295 300 305 310 Temperature T(in K) X 300 0.40 301 0.4075 303 0.4182 304 0.4213 305 0.4228 305.5 0.4229 305.9 0.4227 307 0.421 310 0.4072 315 0.3635 We get maximum X = 0.4229 at T = 305.5 K. P5-14 CH 3CO 2 O H 2O A B 5-30 2CH 3COOH 2C 315 320 Part 1 CSTR A B 3.3 10 3 dm3 s 0 C A0 1M, C B 51.2M 3 V 1 dm X= ? (1)Mole Balance: V (2)Rate Law: rA (3)Stoichiometry: FA0 X rA k CACB Liquid 0 Stoichiometric Table A B C FA0 FB0 BFA0 0 FA0 X FA FA0 1 X FA0 X FB FA0 2FA0 X FC Concentration CA CB FA FA0 1 X 0 0 FB FA0 0 51.2M B 1M B 0 C A0 1 X X C A0 B 51.2 Substitute the value of X into CB. 5-31 X B 2FA0 X X CB CA0 51.2 X CB0 (4)Combine k rA k C AC B0 k C B0 C A0 1 X dm3 k k C B0 1.95 10 4 V mol s FA0 X 0C A0 X rA kC A0 1 X 0 kC A0 1 X 51.2 mol dm 3 0.01 s 1 X k 1 X X k1 X k X 1 k (5)Evaluate V 1 dm3 0 3.3 10 3 dm3 s k X 303 s 3.03 3.03 1 3.03 0.75 Calculate the Conversion in a 0 3 3 3.3 10 dm s, CA0 1M CB 0 V 51.2M PFR 5-32 0.311 dm3 X= ? (1)Mole Balance: (2)Rate Law: (3)Stoichiometry: dX rA dV FA0 rA k CACB Liquid 0 CA C A0 1 X CB C B0 k rA k C B0 C A0 1 X kC A0 1 X (4)Combine dX rA kC A0 1 X dV FA0 0C A0 Separate variables and Integrate with limits V = 0 then X = 0 and V = V then X = X X dX 0 1 ln X V k 0 1 kV 1 X 0 X 1 e dV 0 k k (5)Evaluate 0.311 dm3 3.3 10 3 dm3 s k 0.94 X 0.61 5-33 94 s P5-15 Gaseous reactant in a tubular reactor: A B rA kC A k 0.0015min 1 at 80 F E 25, 000 MWA cal g mol MWB 58 lb lb mol P 132 psig 146.7 psia lb hr lb 58 lb mol 1000 FB X 0.90 MB Dt 1 inch (I.D.) L 10 ft T 260 F nt lb mol 17.21 hr 720 R FA0 FB X 1000 lb hr number of tubes lb mol hr 0.9 17.21 19.1 For a plug flow reactor: 0.9 nt Dt2 L 4 V FA0 dX rA 0 1 1 0 rA yA kC A0 1 X C A0 0.9 V yA 1.0 FA0 dX rA 0 0.9 FA0 dX kC A0 1 X 0 PA RT FA0 1 ln kC A0 1 0.9 0 P RT FA0 RT ln10 kP At T2 = 260°F = 720°R, with k1 = 0.0015 min-1 at T1 = 80°F = 540°R, E 1 R T1 k2 k1 exp k2 53.6 min 1 V 0.72 ft 3 V nt Dt2 L 4 0.0015exp 25000 1 1.104 540 1 720 lb mol hr ft 3 psia lb mol R 720 R 53.6 min 1 3219hr 1 FA0 RT ln10 kP V 1 T2 19.1 10.73 3219 hr 1 146.7 psia 5-34 ln10 lb mol hr nt 4V Dt2 L 4 0.72 ft 3 1 ft 12 2 13.2 10 ft Therefore 14 pipes are necessary. P5-16(a) A → B/2 Combining 2 VPFR kCA0 FA0 X 2 1 X 2 X 1 0 dX 2 1 ln 1 X C AO y AO CTO 2 2 X 1 X 1 X (for the integration, refer to Appendix A) from the Ideal Gas assumption. Substituting Eqn. (5), X = 0.8 and = –1/4 to Eqn. (4) yields, 2 2 VPFR ky AO CTO FAO 2( 1/ 4)(1 1/ 4) ln(1 0.8) ( 1/ 4)2 0.8 5-35 (1 1/ 4)2 0.8 1 0.8 2.9 ……….(6) 2 VPFR ky '2AO C 'TO F '2AO 2 2 CTO 8 VPFR ky AO 9 FAO 8 2.9 9 2.58 P5-16(b) Individualized solution. P5-17(a) A Given: The metal catalyzed isomerization rA B liquid phase reaction CB with Keq = 5.8 K eq k1 C A For a plug flow reactor with yA = 1.0, X1 = 0.55 Case 1: an identical plug flow reactor connected in series with the original reactor. B = 0. For a liquid phase reaction CA Since yA = 1.0, rA kC A0 X K eq 1 X For the first reactor, X1 V1 FA0 dX rA 0 X1 FA0 0 dX kC A0 1 X or X K eq 5-36 CA0 1 X and C B C A0 X X1 kC A0V1 FA0 X1 dX 0 kC A0V1 FA0 1 1 X K eq 1 1 1 1 K eq 1 ln 1 1 1 1 K eq ln 1 1 1 X K eq 0 1 X1 K eq 0.853ln .355 0.883 Take advantage of the fact that two PFR’s in series is the same as one PFR with the volume of the two combined. VF = V1 + V2 = 2V1 and at VF , X = X2 XF XF kC A0VF FA0 0 dX 1 1 1 1 X K eq kC A0VF FA0 2 kC A0V1 FA0 1 kC A0V1 FA0 2 0.883 1.766 2 1.766 1 1 1 5.8 ln 1 1 1 1 K eq 1 K eq 1 ln 1 1 ln 1 1 1 X K eq 0 1 X2 K eq 1 X2 5.8 X2 = 0.74 P5-17(b) Case 2: Products from 1st reactor are separated and pure A is fed to the second reactor, 5-37 The analysis for the first reactor is the same as for case 1. kC A0V1 FA0 1 1 K eq 1 ln 1 1 X1 K eq 1 By performing a material balance on the separator, FA0,2 = FA0(1-X1) Since pure A enters both the first and second reactor CA0,2 = CA0, CB0,2 = 0, CA = CA0 1 - X B=0 C B = C A0 X for the second reactor. X2 FA0 1 X dX FA0,2 rA 0 V2 kC A0V2 FA0 1 X 1 kC A0 1 1 1 K eq X2 0 ln 1 dX 1 X 1 X K eq 1 X2 K eq and since V1 = V2 kC A0V2 FA0 kC A0V1 FA0 or 1 1 1 K eq ln 1 1 1 1 1 X1 ln 1 1 1 K eq 1 X1 K eq 1 X2 K eq 1 5-38 1 1 X1 K eq 1 1 1 X1 1 X2 K eq 1 1 X2 1 1 X1 K eq 1 1 X1 1 1 0.356 0.45 1 1 K eq 1.174 FA0 FA0 1 X1 1 X 2 0.766 Overall conversion for this scheme: X X FA0 FA0,2 1 X 2 FA0 FA0 0.895 P5-18 Given: Meta- to ortho- and para- isomerization of xylene. M k1 P M k2 O O P (neglect) Pressure = 300 psig T = 750°F V = 1000 ft3 cat. Assume that the reactions are irreversible and first order. Then: rM k k1CM k 2 CM kCM k1 k2 0 Check to see what type of reactor is being used. Case 1: v0 2500 gal hr X 0.37 gal hr X 0.50 Case 2: v0 1667 Assume plug flow reactor conditions: FM 0 dX rM dV or 5-39 1 1 X1 1 X 2 X V FM 0 dX rM 0 X V X CM 0 v0 dX rM 0 v0 v0 ln 1 X k dX k 1 X 0 CM0, k, and V should be the same for Case 1 and Case 2. Therefore, kV Case1 v0 Case1 ln 1 X Case1 kV Case 2 v0 Case1 ln 1 X Case 2 gal ln 1 0.37 hr gal 1667 ln 1 0.50 hr 2500 gal hr gal 1155 hr 1155 The reactor appears to be plug flow since (kV)Case 1 = (kV)Case 2 As a check, assume the reactor is a CSTR. FM 0 X V CM 0 v0 X CM 0 X v0 rM rM V v0 X k 1 X or kV v0 X 1 X Again kV should be the same for both Case 1 and Case 2. kV Case1 kV Case 2 gal 0.37 hr 1 0.37 1468 gal 0.50 hr 1 0.50 1667 2500 v0 Case1 X Case1 1 X Case1 v0 Case 2 X Case 2 gal hr 1667 1 X Case 2 gal hr kV is not the same for Case 1 and Case 2 using the CSTR assumption, therefore the reactor must be modeled as a plug flow reactor. kV k gal hr gal 1155 gal hr 1.55 3 1000 ft cat. hr ft 3 cat 1155 For the new plant, with v0 = 5500 gal / hr, XF = 0.46, the required catalyst volume is: V v0 ln 1 X F k gal hr ln 1 0.46 gal 1.155 hr ft 3 cat 5500 2931 ft 3 cat This assumes that the same hydrodynamic conditions are present in the new reactor as in the old. 5-40 P5-19 A→ B in a tubular reactor Tube dimensions: L = 40 ft, D = 0.75 in. nt = 50 50 nt D 2 L 4 V FA0 0.75 12 4 lb hr lb 73 lb mol 2 40 6.14 ft 3 500 mA MWA 6.86 lb mol hr X V FA0 rA dX rA 0 kC A0 1 X 1 X V FA0 dX rA 0 X FA0 dX kC A0 1 X 0 y A0 P RT FA0 RT 1 ln or k ky A0 P 1 X with C A0 V kC A0 1 X X FA0 1 ln kC A0 1 X P RT FA0 RT 1 ln Vy A0 P 1 X Assume Arrhenius equation applies to the rate constant. At T1 = 600°R, k1 = 0.00152 At T2 = 760°R, k2 = 0.0740 Ae Ae E RT1 E RT2 5-41 k2 k1 ln E 1 R T2 exp k2 k1 E 1 R T2 1 T1 E T2 T1 R T1T2 1 T1 660 760 TT k 1 2 ln 2 T1 T2 k1 E R A k1 exp so k 100 ln 0.740 19,500 R 0.00152 E RT1 E 1 R T k1 exp 1 T1 From above we have k FA0 RT 1 ln Vy A0 P 1 X so FA0 RT 1 ln Vy A0 P 1 X E 1 R T k1 exp 1 T1 Dividing both sides by T gives: FA0 R 1 ln Vy A0 P 1 X 6.86 .00152 sec E 1 R T k1 exp lb mol hr 1 T1 T 10.73 sec 3600 hr psia ft 3 lb mol R 6.14 ft 3 exp ln 5 114.7 psia Evaluating and simplifying gives: exp 0.0308 R 1 1 T 19500 1 660 R T Solving for T gives: T = 738°R = 278°F 5-42 1 T 19500 T 1 660 R P5-20 Rate law: -rA= kCACB (1) Molar flow rate: FA0 = FB0 = Since FA0= FB0, therefore equimolar mixture. CA0 = CB0 = FA0/ = 1.51/5.33 = 0.283 lbmol/ft3 From (1), -rA= kCACB = kCA0(1-X)CB0(1-X) = kCA02 (1-X)2 (2) Now, for PFR V = FA0 (3) Putting -rA from (2) in (3) and then integrating, we get VkCA02/ FA0 = Now given, 50% conversion, therefore X = 0.5 So, VkCA02/ FA0 = =1 5.33*k*0.2832/1.51 = 1 k = 3.54 Now we have CSTR in series V = 100 gal = 13.37 ft3 Now, CA20 = CA0/2 = 0.1425 lbmol/ft3 , since we have 50% conversion if PFR FA20 = FA0/2 = 1.51/2 = 0.755 CSTR mole balance: V = FA20 So, 13.37 = 0.755 = FA20 = 13.37 = => X = 0.42 So, CA = 0.1425(1-0.42) = 0.083 So, overall conversion X = (CA0- CA)/CA0 = (0.283 – 0.083)/(0.283) = .70 5-43 X = 0.7 P5-21 Five things wrong with the solution are as follows : (i) The rate law is wrongly written (ii) The integration is wrongly done (iii) Value of Ɛ is wrongly calculated (iv)The equation for calculation of k has been reaaranged wrongly. (v) calculated value of k is therefore wrong correct solution For a first order reaction ; -rA = - 1 dN A V dt kC A By transforming into conversion units we have; -rA = C A0 dX A 1 A X A dt kC A0 (1 X A ) 1 AXA Separating and integrating we obtain ; ln(1 X A ) V ) AV0 ln(1 kt Now in this case ; Ɛ = yA0δ = 1(3-1) = 2 Substituting V V0 4 2 1 2 we have; -ln(1-0.5) = ln2 = kt => k = ln2/t = 0.693/2hr = 0.3465 hr-1 5-44 P5-22 Reversible isomerization reaction m-Xylene → p-Xylene Xe is the equilibrium conversion. rm Rate law: k Cm Cp ke At equilibrium, -rm = 0 => Cm Cp ke Cmo 1 X e Xe 1 Xe Ke 1 Ke 1 rm 1 1 Xe Xe kC A0 1 Cmo X e Ke Xe 1 Xe Xe 1 Xe X Xe P5-22 (a) For batch reactor, Mole balance: dX dt rmV N mO kC A0 X 1 C A0 Xe Xe Xe ln k Xe X V FAO vo k For PFR, PFR PFR dX rm dX 1 1 1 k 1 X Ke dX 1 1 1 X Ke Xe Xe ln k Xe X 5-45 P5-22 (b) For CSTR, V Fmo X rm X CSTR k 1 1 1 X Ke Putting the value of Ke, X k CSTR Xe Xe X P5-22 (c) Volume efficiency = PFR V CSTR 1 V Xe Xe ln k Xe X ln Xe X k Xe X Xe Xe X Xe X X Xe X X Xe 1 ln X X 1 Xe Xe Following is the plot of volume efficiency as a function of the ratio (X/Xe), See Polymath program P5-22-c.pol. 5-46 X ln Xe Xe X P5-23(a) 5-47 P5-23 (b) P5-23 (c) P5-23 (d) For turbulent flow 2 DP1 1 DP 2 Ac1 Ac 2 3 0.018kg 1 2 1 12 1.52 3 0.00316 kg 1 Pexit = P0(1- αW)0.5 = (20atm)(1-0.00316kg-1(50kg))1/2 = 18.35 atm ln 1 0.5 1 X2 X2 0.81 3/ 2 10 3 2 20atm 1 1 0.00316kg 1 50kg 1 atm kg 3 0.00316kg P5-24 Production of phosgene in a microreactor. CO + Cl2 COCl2 (Gas phase reaction) A + B C The euqtions that need to be solved are as follows : d(X)/d(W) = -rA/FA0 d(y)/d(W) = -α*(1+Ɛ *X)/(2*y) ( from 4.30) 5-48 FB0 = FA0; Fb = FB0-FA0*X; Fc = FA0*X See Polymath program P5-24.pol. POLYMATH Results Calculated values of the DEQ variables Variable W X y e FA0 FB0 Fa Fb v0 v Fc Ca Cb a k rA Cc initial value 0 0 1 -0.5 2.0E-05 2.0E-05 2.0E-05 2.0E-05 2.83E-07 2.83E-07 0 70.671378 70.671378 3.55E+05 0.004 -19.977775 0 minimal value 0 0 0.3649802 -0.5 2.0E-05 2.0E-05 4.32E-06 4.32E-06 2.83E-07 2.444E-07 0 9.1638708 9.1638708 3.55E+05 0.004 -19.977775 0 maximal value 3.5E-06 0.7839904 1 -0.5 2.0E-05 2.0E-05 2.0E-05 2.0E-05 2.83E-07 4.714E-07 1.568E-05 70.671378 70.671378 3.55E+05 0.004 -0.3359061 53.532416 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(W) = -rA/FA0 [2] d(y)/d(W) = -a*(1+e*X)/(2*y) Explicit equations as entered by the user [1] e = -.5 [3] FB0 = FA0 [5] Fb = FB0-FA0*X [7] v = v0*(1+e*X)/y [9] Ca = Fa/v [11] a = 3.55e5 [13] rA = -k*Ca*Cb [2] FA0 = 2e-5 [4] Fa = FA0*(1-X) [6] v0 = 2.83e-7 [8] Fc = FA0*X [10] Cb = Fb/v [12] k = .004 [14] Cc = Fc/v 5-49 final value 3.5E-06 0.7839904 0.3649802 -0.5 2.0E-05 2.0E-05 4.32E-06 4.32E-06 2.83E-07 4.714E-07 1.568E-05 9.1638708 9.1638708 3.55E+05 0.004 -0.3359061 33.259571 P5-24 (a) P5-24 (b) The outlet conversion of the reactor is 0.784 The yield is then MW*FA*X = 99 g/mol * 2 e-5 mol/s * 0.784 = .00155 g/s = 48.95 g/ year. Therefore 10,000 kg/year / 48.95 kg/ year = 204 reactors are needed. P5-24 (c) Assuming laminar flow, α ~ Dp-2, therefore 2 DP21 1 DP2 2 3.55 105 kg 1 4 14.2 105 kg 1 P5-24 (d) A lower conversion is reached due to equilibrium. Also, the reverse reaction begins to overtake the forward reaction near the exit of the reactor. P5-24 (e) Individualized solution 5-50 P5-24 (f) Individualized solution P5-24 (g) Individualized solution P5-25 No solution necessary P5-26 A B C D P0 P 1. Mole Balance – Use Differential Form dX dW rA FA 0 2. Rate Law – Psuedo Zero Order in B rA 3. Stoichiometry – Gas: kC A C 0B 0 1 kC A X T P0 , Isothermal, therefore T T0 P 5-51 T0 FA0 1 X P FA CA 0 1 X P0 CA 1 X y , y P P0 0 C A0 1 X y , where W 2y 1 X 1 1 1 1 1 2 y A0 dy dW C A0 0 then y 1 and X 0 Integrating y part (a) 1 W 12 Now since P/P0 >0.1 . So y= .1 for minimum value of W Now (1 – αW)1/2 = .1 => W = 99 kg 4. Combine rA kC A kC A0 1 X y kC A0 1 X 1 dX dW kC A0 1 X 1 FA0 1 W Separate Variables dX 1 X k 12 dW 0 when W = 0, X = 0 ln 1 1 X 2k 1 3 0 1 W 32 5-52 W 12 W 12 2 1.2 dm 3 g min 2k 3 0 ln 3 0.01 g 25 dm 3 min 1 3.2 1 1 1 X y 1 W 0 0 W 3.2 32 12 P0 P 1 y 5-53 W y 1/y X P 0 1 1 0 10 atm 1 1 1 0.47 2.5 0.99 1.01 0.11 5 0.975 1.02 0.21 15 0.92 1.08 0.5 25 0.87 1.16 0.67 50 0.71 1.41 0.87 75 0.5 2.0 0.94 90 0.32 3.16 0.955 99 0.1 10 0.96 X = 0.9 2.3 1 3.2 1 1 W 32 W .429 W = 57g for 5% W = 1.05g for last 5% (85 to 90%) W = 57 – 45 = 12 g Ratio = 12g = 11.4 1.05g Polymath dX dW rA prime FA0 dy dW alpha 2 y rA prime CA k CA C A0 1 Xy k 1.2 dm 3 g min alpha 0.01g 1 5-54 1 atm 5-55 5-56 P5-27 0, y 0 1 W 1 2 Mole Balance/Design Equation FA 0 dX dW rA Rate Law rA kC A 2 5-57 Stoichiometry CA C A0 1 X y Combining FA 0 dX dW FA 0 2 kC A0 1 X dX 2 kC A0 1 X FA 0 X 2 kC A0 1 X 10 2 1 2 W 2 y2 W dW 2 W2 100 99 2 101 2 19.8 dm 6 mol 2 min k 300 K 0.1 k 300 K 2000 101 k 400 K k 300 K exp E 1 R 300 19.8 exp 10,000 1 1.987 300 1311.179 dm 6 mol 2 min 1 400 1 400 P5-28 A rA B C kC A Case1: 10 dm3 PFR with 80% conversion at 300K. dV FA0 dX A rA C A0 dX A rA Here, = 10 dm3/5 dm3/sec = 2 sec & C A0 dX A 1 XA kC A0 1 XA y A0 1(1 1 1) 1 dX A 1 XA kC A0 1 XA 5-58 0.8 dX A 1 XA 1 XA 2k 0 Integrating, we get k = 1.21 sec-1 Case2: 10 dm3 CSTR with 80% conversion at 320K. V FA0 XA rA C A0 XA rA Here, = 10 dm3/5 dm3/sec = 2 sec & C A0 XA 1 XA kC A0 1 XA y A0 1(1 1 1) 1 XA 1 XA kC A0 1 XA XA 1 XA 1 XA 2k Putting XA=0.8, we get k = 2.8 sec-1 Now, k (T2 ) k (T1 ) exp k (T k (T Ea 1 ( R T1 320 K ) 300 K ) 1 ) T2 exp Ea 1 1 ( ) 1.986 300 320 Ea 2.8 1 1 exp ( ) 1.21 1.986 300 320 Ea 8000cal / mol P5-29 For the turbulent flow 0, y 0 1 W 1 2 5-59 Mole Balance/Design Equation FA 0 dX dW rA Rate Law rA kC A 2 Stoichiometry CA C A0 1 X y Combining FA0 dX dW kC A0 2 1 X FA0 dX 2 kC A0 1 X 2 FA0 X 2 kC A0 1 X 1 W 2 y2 W dW 2 W2 Combining ~ 2 DP1 1 DP 2 X 1 X 1 2 1 DP 9.975 10 3 kg 1 2 13.47 0.244 10 2 4.99 10 3 100 100 2 0.0802 100 24.95 X 4.99 10 3 kg 1 2 6.02 0.86 P5-30 Individualized solution 5-60 CDP5-B a) Polymath solution (Ans CDP5-B-a) b) 5-61 Polymath solution(Ans CDP5-B-b) c) Polymath solution(Ans CDP5-B-c) d) This part is almost same as part(b) with minor changes: V = 15000000 – 10000t vo = 80000 and vout = 70000 The reason the graph looks so different from(a) is that pure water is evaporated, but water with atrazine is coming in. Polymath code: 5-62 d(ca)/dt=cao*vo/v)-(ca(kv+vout)/v) ca(0)=4.5 # vo = 80000 # v = 15000000 - 10000*t k = 0.0025 # cao = 4.5 # vout = 70000 # t(0)=0 # t(f)=1000 Polymath solution(Ans CDP5-B-d) CDP5-C 5-63 CD5RD-1 No solution 5-64 CD5RD-2 5-65 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 6-1 Solutions for Chapter 6 : Isothermal Reactor Design- Molar Flow rates P6-1 Individualized solution. P6-2 (a) Example 6-1 For pressure doubled and temperature decrease CTO = 2*Po/RT and T = 688K See Polymath program P6-2-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable V Fa Fb Fc E T Cto Ft Ca k ra Fao rb vo rc X Tau rateA initial value 0 2.26E-04 0 0 2.4E+04 688 0.573773 2.26E-04 0.573773 213.40078 -70.254837 2.26E-04 70.254837 3.939E-04 35.127419 0 0 70.254837 minimal value 0 1.363E-05 0 0 2.4E+04 688 0.573773 2.26E-04 0.0236075 213.40078 -70.254837 2.26E-04 0.1189309 3.939E-04 0.0594654 0 0 0.1189309 maximal value 1.0E-04 2.26E-04 2.124E-04 1.062E-04 2.4E+04 688 0.573773 3.322E-04 0.573773 213.40078 -0.1189309 2.26E-04 70.254837 3.939E-04 35.127419 0.9395277 0.253044 70.254837 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(V) = ra [2] d(Fb)/d(V) = rb [3] d(Fc)/d(V) = rc 6-2 final value 1.0E-04 1.363E-05 2.124E-04 1.062E-04 2.4E+04 688 0.573773 3.322E-04 0.0236075 213.40078 -0.1189309 2.26E-04 0.1189309 3.939E-04 0.0594654 0.9395277 0.253044 0.1189309 Explicit equations as entered by the user [1] E = 24000 [2] T = 688 [3] Cto = 2*1641/8.314/T [4] Ft = Fa+Fb+Fc [5] Ca = Cto*Fa/Ft [6] k = 0.29*exp(E/1.987*(1/500-1/T)) [7] ra = -k*Ca^2 [8] Fao = 0.000226 [9] rb = -ra [10] vo = Fao/Cto [11] rc = -ra/2 [12] X = 1-Fa/Fao [13] Tau = V/vo [14] rateA = -ra P6-2 (b) Example 6-2 Individualized solution. P6-2 (c) Example 6-3 Using trial and error, we get maximum feed rate of B = 0.0251dm3/s to keep concentration of B 0.01mol/dm3. See Polymath program P6-2-c.pol. POLYMATH Results Calculated values of the DEQ variables Variable t ca cb cc cd k v00 cb0 initial value 0 0.05 0 0 0 0.22 0.0251 0.025 minimal value 0 0.0063485 0 0 0 0.22 0.0251 0.025 maximal value 500 0.05 0.009981 0.0078965 0.0078965 0.22 0.0251 0.025 6-3 final value 500 0.0063485 0.009981 0.0078965 0.0078965 0.22 0.0251 0.025 v0 5 5 ca0 0.05 0.05 rate 0 0 v 5 5 x 0 0 Differential equations as entered by the user [1] d(ca)/d(t) = -k*ca*cb-v00*ca/v [2] d(cb)/d(t) = -k*ca*cb+v00*(cb0-cb)/v [3] d(cc)/d(t) = k*ca*cb-v00*cc/v [4] d(cd)/d(t) = k*ca*cb-v00*cd/v 5 0.05 3.91E-05 17.55 0.5543321 Explicit equations as entered by the user [1] k = .22 [2] v00 = 0.0251 [3] cb0 = 0.025 [4] v0 = 5 [5] ca0 = 0.05 [6] rate = k*ca*cb [7] v = v0+v00*t [8] x = (ca0*v0-ca*v)/(ca0*v0) If the concentration of A is tripled the maximum feed rate becomes 0.064 dm3/s P6-2 (d through g) Individualized solution. P6-3 Solution is in the decoding algorithm given with the modules. P6-4 (a) A B 2C CA= CA0 CA0 = PA0/RT = k = 10-4exp[ Next we express the rate law as: 6-4 5 0.05 1.394E-05 17.55 0.5543321 rA k CA CBCC2 KC At equilibrium, C F k T0 A FT CT 0 FT 3 FB FC2 KC (1) = 0, Therefore, from (1), k[CA- ]=0 CA0(1-Xe) – CA0Xe*(2CA0Xe)2/Kc = 0 (1-Xe) - Xe*22* CA02* Xe2/ Kc = 0 (1-Xe) - Xe*22* 0.32* Xe2/ 0.025 = 0 (1-Xe) – 14.4Xe3 = 0 => Xe = 0.355 So, the equilibrium conversion obtained in a PFR is 35.5 %. P6-4 (b) dFB dV dFC dV rB RB rC Transport out the sides of the reactor: RB = kcCB = kB CT 0 FB FT Stoichiometery: -rA = rB =1/2 rC 6-5 POLYMATH Report No Title 06-May-2009 Ordinary Differential Equations Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Co 0.3 0.3 0.3 0.3 2 Fa 2.5 0.0323558 2.5 0.0323558 3 Fb 0 0 0.0197934 0.0002897 4 Fc 0 0 4.935288 4.935288 5 Ft 2.5 2.5 4.967934 4.967934 6 K 0.044 0.044 0.044 0.044 7 Kc 0.025 0.025 0.025 0.025 8 kc 4.8 4.8 4.8 4.8 9 ra -0.0132 -0.0132 -8.324E-05 -8.324E-05 10 Rb 0 0 0.0099094 8.398E-05 11 V 0 0 1500. 1500. 12 X 0 0 0.9870577 0.9870577 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = -ra - Rb 3 d(Fc)/d(V) = -2*ra Explicit equations 1 Ft = Fa+Fb+Fc 2 K = 0.044 3 kc = 4.8 min-1 4 Kc = 0.025 5 Co = 0.3 6 X = (2.5-Fa)/2.5 7 Rb = kc*Co*Fb/Ft 8 ra = - (K*Co/Ft)*(Fa- Co^2*Fb*Fc^2/(Kc*Ft^2)) General Total number of equations 11 Number of differential equations 3 Number of explicit equations 8 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 6-6 6-7 So, if the reactor volume is 800 dm3, exit conversion will be 0.92. 6-8 We see that volume required for 80% conversion is 467 dm3, therefore plotting the flow rates till 467 dm3 6-9 P6-5 (a) Assume constant volume batch reactor Mole balance: C A0 dX dt rA Rate law and stoichiometry: rA kC A kC A0 1 X 6-10 Specific reaction rate: k 25 C 0.0022 weeks 1 Combine: X dX kC A0 1 X 0 1 ln 1 X 52.2 weeks k 1 ln 1 X 0.0022 weeks 1 t C A0 X 0.108 CA C A0 1 X but since volume and molecular weight are constant the equation can be written as: mA mA0 1 X 6500 IU mA0 mA0 1 0.108 7287 IU C A0 C A *100 CA %OU 7287 6500 *100 12.1% 6500 P6-5 (b) 10,000,000 lbs/yr = 4.58 * 109 g/yr of cereal Serving size = 30g Number of servings per year = 4.58 * 109 / 30 =1.51 * 109 servings/yr Each serving uses an excess of 787 IU = 4.62 * 10-4 = 1.02 * 10-6 lb Total excess per year = (1.51 * 108 servings/yr) * (1.02 * 10-6 lbs/serving) = 154.11 lb/yr Total overuse cost = $100/lb * 154.11 lb/yr = $15411 / yr (trivial cost) P6-5 (c) If the nutrients are too expensive, it could be more economical to store the cereal at lower temperatures where nutrients degrade more slowly, therefore lowering the amount of overuse. The cost of this storage could prove to be the more expensive alternative. A cost analysis needs to be done to determine which situation would be optimal. P6-5 (d) k 40 C X t C A0 0.0048 weeks 1 dX kC A0 1 X 0 26weeks 6 months = 26 weeks 1 ln 1 X k 1 ln 1 X 0.0048 weeks 1 X 0.12 CA C A0 1 X but since volume and molecular weight are constant the equation can be written as: 6-11 mA mA0 1 X 6500 IU mA0 %OU mA0 1 0.12 7386 IU C A0 C A *100 CA 7386 6500 *100 13.6% 6500 P6-6 3 Suppose the volumetric flow rate could be increased to as much as 6,000 dm /h (9,000 mol/h) and the total time to fill, heat, empty and clean is 4.5 hours. What is the maximum number of moles of ethylene glycol (CH2OH)2 you can make in one 24 hour period? The feed rate of ethylene cholorhydrin will be adjusted so that the volume of fluid at the end of the reaction time will be 2500 dm3. Now suppose CO2 leaves the reactor as fast as it is formed. A B C D CO2 Mole Balance dN A rAV dt dN B FB0 dt dNC rC V dt N D NC rBV Overall Mass Balance Accumulation = In – Out dm ÝCO 2 0 m dt m V Assume constant density mÝCO 2 dV dt 0 The rate of formation of CO2 is equal to the rate of formation of ethylene glycol (C). mÝCO 2 dV dt CO 2 FCO 2 0 MWCO2 FCO 2 FCO 2 MWCO2 0 CO 2 MWCO2 6-12 Rate Law and Relative Rates rA kCA CB rB rA rC rA rCO 2 rA Stoichiometry NA V NB V CA CB dC A dt dC B dt dCC dt CD CC dN CO 2 dt FCO 2 CO 2 C A 0 rA V 0C B0 CO 2 CB 0 V V 0 rA CO 2 CC V 0 FCO 2 rAV rAV 6-13 P6-6(c) FA0 0.15 mol min vo Fao /Ca 3 9 mol hr 9 mol hr / 1.5 mol dm 3 6 dm 3 hr 3 1000 dm is needed to fill the reactor. At 6 dm /hr it will take 166.67 hours Now solving using the code form part (a) with the changed equations: See Polymath program 6-14 P6-7 C B0 0.25 mol dm3 V C A0 0.2 mol V0 dm3 VT VT D 2L 1.5m 4 4.42m 2 2.5m 4 3 4, 420 dm 3 We don’t know V0 or v0. First try equal number of moles of A and B added to react. NA C A0 V0 V0 NB C B0 V C B0 VT VT 4420 C A0 0.8 1.0 1 C B0 V0 2456 V 1964 V 0 k0 tR 3 0.000052 dm mol s 0.187 dm3 mol h For 1 batch tR = 24 – 3 = 21 VT 0 V0 21 (1) For one batch we see that only 198 moles of C are made so one batch will not work. (2) For two batches, we have a down time of 2 3 = 6 h and therefore each batch has a reaction time of 18h/2 = 9 h. We see that 106 moles of C are made in one batch therefore 2 106 = 212 moles/day are made in two batches. 6-15 P6-7 6-16 P6-7 P6-8 (a) A B 2C To plot the flow rates down the reactor we need the differential mole balance for the three species, noting that BOTH A and B diffuse through the membrane dFA dV dFB dV dFC dV rA RA rB RB rC Next we express the rate law: First-order reversible reaction rA k CA CBCC2 KC C F k T0 A FT CT 0 FT 3 FB FC2 KC 6-17 Transport out the sides of the reactor: RA = kACA = k ACT 0 FA FT RB = kBCB = kB CT 0 FB FT Stoichiometery: -rA = rB =1/2 rC Combine and solve in Polymath code: See Polymath program P6-9-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable v Fa Fb Fc Kc Ft Co K Kb ra Ka Ra Rb Fao X initial value 0 100 0 0 0.01 100 1 10 40 -10 1 1 0 100 0 minimal value 0 57.210025 0 0 0.01 100 1 10 40 -10 1 0.472568 0 100 0 maximal value 20 100 9.0599877 61.916043 0.01 122.2435 1 10 40 -0.542836 1 1 2.9904791 100 0.4278998 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(v) = ra - Ra [2] d(Fb)/d(v) = -ra - Rb [3] d(Fc)/d(v) = -2*ra 6-18 final value 20 57.210025 1.935926 61.916043 0.01 121.06199 1 10 40 -0.542836 1 0.472568 0.6396478 100 0.4278998 Explicit equations as entered by the user [1] Kc = 0.01 [2] Ft = Fa+ Fb+ Fc [3] Co = 1 [4] K = 10 [5] Kb = 40 [6] ra = - (K*Co/Ft)*(Fa- Co^2*Fb*Fc^2/(Kc*Ft^2)) [7] Ka = 1 [8] Ra = Ka*Co*Fa/Ft [9] Rb = Kb*Co*Fb/Ft P6-8 (b) The setup is the same as in part (a) except there is no transport out the sides of the reactor. See Polymath program P6-9-b.pol. POLYMATH Results Calculated values of the DEQ variables Variable v Fa Fb Fc Kc Ft Co K ra Fao X initial value 0 100 0 0 0.01 100 1 10 -10 100 0 minimal value 0 84.652698 0 0 0.01 100 1 10 -10 100 0 maximal value 20 100 15.347302 30.694604 0.01 130.6946 1 10 -3.598E-09 100 0.153473 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(v) = ra [2] d(Fb)/d(v) = -ra [3] d(Fc)/d(v) = -2*ra 6-19 final value 20 84.652698 15.347302 30.694604 0.01 130.6946 1 10 -3.598E-09 100 0.153473 Explicit equations as entered by the user [1] Kc = 0.01 [2] Ft = Fa+ Fb+ Fc [3] Co = 1 [4] K = 10 [5] ra = - (K*Co/Ft)*(Fa- Co^2*Fb*Fc^2/(Kc*Ft^2)) P6-8 (c) Conversion would be greater if C were diffusing out. P6-8 (d) Individualized solution P6-9 (a) CO + H 2O CO2 + H 2 A + B C + D Assuming catalyst distributed uniformly over the whole volume Mole balance: dFA dW Rate law: r RH 2 rA dFB dW r rB rC r rD dFC dW k C AC B K H2 CD 6-20 r CC CD K eq dFD dW r RH 2 Stoichiometry: C A CTO FA FT FT FA FB CB FC CTO FB FT CC CTO FC FT FD Solving in polymath: See Polymath program P6-10.pol. POLYMATH Results Calculated values of the DEQ variables Variable W Fa Fb Fc Fd Keq Ft Cto Ca Cb Kh Cc Cd Rh k r initial value 0 2 2 0 0 1.44 4 0.4 0.2 0.2 0.1 0 0 0 1.37 -0.0548 minimal value 0 0.7750721 0.7750721 0 0 1.44 3.3287437 0.4 0.0931369 0.0931369 0.1 0 0 0 1.37 -0.0548 maximal value 100 2 2 1.2249279 0.7429617 1.44 4 0.4 0.2 0.2 0.1 0.147194 0.0796999 0.00797 1.37 -0.002567 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(W) = r [2] d(Fb)/d(W) = r [3] d(Fc)/d(W) = -r [4] d(Fd)/d(W) = - r -Rh Explicit equations as entered by the user [1] Keq = 1.44 [2] Ft = Fa+Fb+Fc+Fd [3] Cto = 0.4 [4] Ca = Cto*Fa/Ft [5] Cb = Cto*Fb/Ft [6] Kh = 0.1 [7] Cc = Cto*Fc/Ft [8] Cd = Cto*Fd/Ft [9] Rh = Kh*Cd [10] k = 1.37 [11] r = -k*(Ca*Cb-Cc*Cd/Keq) For 85% conversion, W = weight of catalyst = 430 kg 6-21 final value 100 0.7750721 0.7750721 1.2249279 0.5536716 1.44 3.3287437 0.4 0.0931369 0.0931369 0.1 0.147194 0.0665322 0.0066532 1.37 -0.002567 CD CTO FD FT (b) In a PFR no hydrogen escapes and the equilibrium conversion is reached. K eq CC CD C AC B C A2 0 X 2 C A2 0 (1 X ) 2 X2 1 X 2 1.44 solve this for X, X = .5454 This is the maximum conversion that can be achieved in a normal PFR. (c) If feed rate is doubled, then the initial values of Fa and Fb are doubled. This results in a conversion of .459 P6-10 Individualized solution P6-11 (a) At equilibrium, r = 0 => C A C B CC C D KC V = V0 + vot CA N AO 1 X V C AO 1 X V VO C AO 1 X 1 vo t VO 6-22 C BO CB vO t C AO X VO 1 CC vo t VO C AO X CD 1 vo t VO v C AO 1 X C BO O t C AO X VO t VO C AO X2 vO C BO K C 1 X 2 X 200 * 7.72 X2 0.05 *10.93 1.08 1 X t C AO X KC X Solving in Polymath POLYMATH Report Nonlinear Equation 06-May-2009 Calculated values of NLE variables Variable Value f(x) Initial Guess 1 x 0 0 0.495 ( 0 < x < 0.99 ) Nonlinear equations 1 f(x) = 2825.25*(x^2/1.08/(1-x)+x) = 0 General Settings Total number of equations 1 Number of implicit equations 1 Number of explicit equations 0 Elapsed time 0.0000 sec Solution method SAFENEWT Max iterations 150 Tolerance F 0.0000001 Tolerance X 0.0000001 Tolerance min 0.0000001 6-23 If we solve in Excel X 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95 0.99 t (sec) 0 148.1466374 311.591358 493.0338235 695.8486111 924.3101852 1183.914286 1481.84765 1827.692593 2234.515909 2720.611111 3312.40216 4049.525 4994.264683 6250.42963 8004.875 10631.31111 15001.7287 23732.1 49902.28611 259188.435 6-24 P6-11 (b) See Polymath program P6-12-b.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb Cc Cd Kc k initial value 0 7.72 10.93 0 0 1.08 9.0E-05 minimal value 0 0.2074331 7.6422086 0 0 1.08 9.0E-05 maximal value 1.5E+04 7.72 10.93 3.2877914 3.2877914 1.08 9.0E-05 6-25 final value 1.5E+04 0.2074331 9.51217 1.41783 1.41783 1.08 9.0E-05 ra vo Vo V X -0.0075942 0.05 200 200 0 -0.0075942 0.05 200 200 0 -1.006E-05 0.05 200 950 0.9731304 -1.006E-05 0.05 200 950 0.9731304 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = ra - Ca*vo/V [2] d(Cb)/d(t) = ra - vo/V*(Cb- 10.93) [3] d(Cc)/d(t) = -ra - vo*Cc/V [4] d(Cd)/d(t) = -ra - vo*Cd/V Explicit equations as entered by the user [1] Kc = 1.08 [2] k = 0.00009 [3] ra = -k*(Ca*Cb - Cc*Cd/Kc) [4] vo = 0.05 [5] Vo = 200 [6] V = Vo + vo*t [7] X = 1 - Ca/7.72 Polymath solution P6-11 (c) Change the value of vo and CAO in the Polymath program to see the changes. P6-11 (d) As ethanol evaporates as fast as it forms: Now using part (b) remaining equations, Polymath code: CD = 0 See Polymath program P6-12-d.pol. 6-26 POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k ra vo Vo V X initial value 0 7.72 10.93 9.0E-05 -0.0075942 0.05 200 200 0 minimal value 0 0.0519348 6.9932872 9.0E-05 -0.0075942 0.05 200 200 0 maximal value 6000 7.72 10.93 9.0E-05 -3.69E-05 0.05 200 500 0.9932727 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = ra - Ca*vo/V [2] d(Cb)/d(t) = ra - vo/V*(Cb- 10.93) Explicit equations as entered by the user [1] k = 0.00009 [2] ra = -k*Ca*Cb [3] vo = 0.05 [4] Vo = 200 [5] V = Vo + vo*t [6] X = 1 - Ca/7.72 P6-11 (e) Individualized solution P6-11 (f) Individualized solution 6-27 final value 6000 0.0519348 7.8939348 9.0E-05 -3.69E-05 0.05 200 500 0.9932727 P6-12 CA0, CA0, CSTR A B CA0(1-X), (rejected) -rA = k[ CA – CB/Ke) -rA = k[ CA0(1-X)- CA0X/Ke) Given : k = 0.4 h-1 Ke = 4 V = 60 m3 CA0= 100 kg/m3 6-28 = 12 m3/hr FA0= 100*12 = 1200 kg/hr FA20= FA0 + CA0 = FA0 (1+ f) = 1200(1+ f) CSTR mole balance: = = Putting the values, we have = (1) Solving we get, X= Profit = Value or products – Operating Cost Profit = $2*CA0*X (1+f) - $50 (1+f) Profit = $ 600*(1+f)*(4X-1) (2) Now, solving equation (1) in excel and corresponding finding out the vale or profit from equation (2), we have f X Profit($) 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55 0.571429 0.56338 0.555556 0.547945 0.540541 0.533333 0.526316 0.519481 0.512821 0.506329 0.5 0.493827 771.4286 789.7183 806.6667 822.3288 836.7568 850 862.1053 873.1169 883.0769 892.0253 900 907.037 6-29 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95 1 0.487805 0.481928 0.47619 0.470588 0.465116 0.45977 0.454545 0.449438 0.444444 913.1707 918.4337 922.8571 926.4706 929.3023 931.3793 932.7273 933.3708 933.3333 0.9 0.91 0.92 0.93 0.94 0.95 0.96 0.97 0.98 0.99 1 0.454545 0.453515 0.452489 0.451467 0.45045 0.449438 0.44843 0.447427 0.446429 0.445434 0.444444 932.7273 932.9116 933.0679 933.1964 933.2973 933.3708 933.417 933.4362 933.4286 933.3942 933.3333 0.96 0.961 0.962 0.963 0.964 0.965 0.966 0.967 0.968 0.969 0.97 0.971 0.972 0.44843 0.44833 0.448229 0.448129 0.448029 0.447928 0.447828 0.447728 0.447628 0.447527 0.447427 0.447327 0.447227 0.447127 0.447027 0.446927 0.446828 0.446728 0.446628 0.446528 0.446429 933.417 933.4202 933.423 933.4256 933.428 933.43 933.4318 933.4333 933.4346 933.4355 933.4362 933.4367 933.4369 933.4368 933.4364 933.4358 933.4349 933.4337 933.4322 933.4305 933.4286 0.973 0.974 0.975 0.976 0.977 0.978 0.979 0.98 6-30 So we see the maximum profit ($933.4369) occurs for f=0.972 Corresponding conversion of A, X = 0.4472 P6-13 A + B -> C 6-31 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 t 0 0 200. 200. 2 Cc 2. 2. 3.893617 3.893617 3 Cb 2. 0.106383 2. 0.106383 4 Ca 2. 0.106383 2. 0.106383 5 k 0.0445 0.0445 0.0445 0.0445 6 Cao 2. 2. 2. 2. 7 ra -0.178 -0.178 -0.0005036 -0.0005036 8 rb -0.178 -0.178 -0.0005036 -0.0005036 9 X 0 0 0.9468085 0.9468085 10 rc 0.178 0.0005036 0.178 0.0005036 Differential equations 1 d(Cc)/d(t) = rc 2 d(Cb)/d(t) = rb 3 d(Ca)/d(t) = ra Explicit equations 1 k = 0.0445 6-32 2 Cao = 2 3 ra = -k * Ca * Cb 4 rb = ra 5 X = (Cao - Ca) / Cao 6 rc = -ra P6-14 The 4 mistakes are as follows: 1) rb = - k * Ca2 2) CA0 = 0.4 and not CTO 3) CTO = 0.8 4) The 5th equation should have been alpha FT 2 y FT 0 dy dW CDGA 6-1 (a) At equilibrium, r = 0 => C A C B CC C D KC V = V0 + vot CA N AO 1 X V C BO CB C AO 1 X V VO C AO 1 X 1 vo t VO vO t C AO X VO 1 vo t VO 6-33 CC CD C AO X 1 vo t VO v C AO 1 X C BO O t C AO X VO t VO C AO X2 vO C BO K C 1 X C AO X KC 2 X Now solving in polymath, See Polymath program CDGA6-1-a.pol. CDGA 6-1 (b) See Polymath program CDGA6-1-b.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb Cc Cd Kc k ra vo Vo V X initial value 0 7.72 10.93 0 0 1.08 9.0E-05 -0.0075942 0.05 200 200 0 minimal value 0 0.2074331 7.6422086 0 0 1.08 9.0E-05 -0.0075942 0.05 200 200 0 maximal value 1.5E+04 7.72 10.93 3.2877914 3.2877914 1.08 9.0E-05 -1.006E-05 0.05 200 950 0.9731304 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = ra - Ca*vo/V [2] d(Cb)/d(t) = ra - vo/V*(Cb- 10.93) [3] d(Cc)/d(t) = -ra - vo*Cc/V [4] d(Cd)/d(t) = -ra - vo*Cd/V Explicit equations as entered by the user [1] Kc = 1.08 [2] k = 0.00009 [3] ra = -k*(Ca*Cb - Cc*Cd/Kc) [4] vo = 0.05 [5] Vo = 200 6-34 final value 1.5E+04 0.2074331 9.51217 1.41783 1.41783 1.08 9.0E-05 -1.006E-05 0.05 200 950 0.9731304 [6] V = Vo + vo*t [7] X = 1 - Ca/7.72 Polymath solution CDGA 6-1 (c) Change the value of vo and CAO in the Polymath program to see the changes. CDGA 6-1 (d) As ethanol evaporates as fast as it forms: Now using part (b) remaining equations, Polymath code: CD = 0 See Polymath program CDGA6-1-d.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k ra vo Vo V X initial value 0 7.72 10.93 9.0E-05 -0.0075942 0.05 200 200 0 minimal value 0 0.0519348 6.9932872 9.0E-05 -0.0075942 0.05 200 200 0 maximal value 6000 7.72 10.93 9.0E-05 -3.69E-05 0.05 200 500 0.9932727 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = ra - Ca*vo/V [2] d(Cb)/d(t) = ra - vo/V*(Cb- 10.93) Explicit equations as entered by the user 6-35 final value 6000 0.0519348 7.8939348 9.0E-05 -3.69E-05 0.05 200 500 0.9932727 [1] k = 0.00009 [2] ra = -k*Ca*Cb [3] vo = 0.05 [4] Vo = 200 [5] V = Vo + vo*t [6] X = 1 - Ca/7.72 CDGA 6-1 (e) Individualized solution CDGA 6-1 (f) Individualized solution CDGA 6-2 (a) Mole balance on reactor 1: C A0 v A0 C A1v rA1V C A0 v0 C A1v rA1V 2 dN A1 with v A0 dt dN A1 dt 1 v0 2 Liquid phase reaction so V and v are constant. C A0 2 C A1 rA1 dC A1 dt Mole balance on reactor 2: C A1v0 C A 2 v0 C A1 C A2 rA 2 rA 2V dN A 2 dt dC A 2 dt 6-36 Mole balance for reactor 3 is similar to reactor 2: C A 2 v0 C A3v0 C A2 C A3 rA3V rA3 dN A3 dt dC A3 dt Rate law: rAi kC Ai CBi Stoichiometry For parts a, b, and c CAi = CBi so that rAi kC Ai2 Combine: C A0 2 C A1 C A1 kC A21 C A2 kC A2 2 C A2 C A3 kC A2 3 dC A1 dt dC A 2 dt dC A3 dt See Polymath program CDGA6-2-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca1 Ca2 Ca3 k Cao tau X initial value 0 0 0 0 0.025 2 10 1 minimal value 0 0 0 0 0.025 2 10 0.3890413 maximal value 100 0.8284264 0.7043757 0.6109587 0.025 2 10 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca1)/d(t) = (Cao/2 -Ca1)/tau -k*Ca1^2 [2] d(Ca2)/d(t) = (Ca1 - Ca2)/tau -k*Ca2^2 [3] d(Ca3)/d(t) = (Ca2 - Ca3)/tau -k*Ca3^2 6-37 final value 100 0.8284264 0.7043757 0.6109587 0.025 2 10 0.3890413 Explicit equations as entered by the user [1] k = 0.025 [2] Cao = 2 [3] tau = 10 [4] X = 1 - 2*Ca3/Cao From Polymath, the steady state conversion of A is approximately 0.39 CDGA 6-2 (b) 99% of the steady state concentration of A (the concentration of A leaving the third reactor) is: (0.99)(0.611) = 0.605 This occurs at t = CDGA 6-2 (c) The plot was generated from the Polymath program given above. CDGA 6-2 (d) We must reexamine the mole balance used in parts a-c. The flow rates have changed and so the mole balance on species A will change slightly. Because species B is added to two different reactors we will also need a mole balance for species B. Mole balance on reactor 1 species A: dN A1 with v A0 dt dN A1 C A1v rA1V dt C A0 v A0 C A1v rA1V 2C A0 v0 3 2 v0 and v0 3 Liquid phase reaction so V and v are constant. 6-38 200 15 C A0 2 C A1 rA1 dC A1 dt Mole balance on reactor 1 species B: dN B1 and vB 0 dt CB 0 vB 0 CB1v rB1V 1 v0 3 Stoichiometry has not changed so that –rAi = -rBi and it is a liquid phase reaction with V and v constant. CB 0 3 CB1 rA1 dCB1 dt Mole balance on reactor 2 species A: We are adding more of the feed of species B into this reactor such that v2 = v0 + vB0 = 20 C A1v0 C A 2 v2 C A1 1 C A2 rA2 2 rA 2V dN A 2 dt dC A2 where dt 1 V and v0 2 V v2 Mole balance on reactor 2 species B: dN B 2 dt CB1v0 CB 0 vB 0 CB 2 v rB 2V CB1 1 C B 0 vB 0 V CB 2 rA2 2 dCB 2 dt Mole balance for reactor 3 species A: C A 2 v2 C A3v2 C A2 C A3 2 2 rA3 rA3V dN A3 dt dC A3 dt Mole balance for reactor 3 species B: CB 2 v2 CB 3v2 CB 2 CB 3 2 2 rA3 rA3V dN B 3 dt dCB 3 dt 6-39 Rate law: rAi kC Ai CBi See Polymath program CDGA6-2-d.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca1 Ca2 Ca3 Cb1 Cb2 Cb3 k Cao tau X tau2 V vbo initial value 0 0 0 0 0 0 0 0.025 2 13.333333 1 10 200 5 minimal value 0 0 0 0 0 0 0 0.025 2 13.333333 0.3721856 10 200 5 maximal value 100 1.1484734 0.7281523 0.6278144 0.4843801 0.7349863 0.6390576 0.025 2 13.333333 1 10 200 5 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca1)/d(t) = (2*Cao/3 -Ca1)/tau -k*Ca1*Cb1 [2] d(Ca2)/d(t) = Ca1/tau - Ca2/tau2 -k*Ca2*Cb2 [3] d(Ca3)/d(t) = (Ca2 - Ca3)/tau2 -k*Ca3*Cb3 [4] d(Cb1)/d(t) = (1*Cao/3-Cb1)/tau-k*Ca1*Cb1 [5] d(Cb2)/d(t) = Cb1/tau+Cao*vbo/V-Cb2/tau2-k*Ca2*Cb2 [6] d(Cb3)/d(t) = (Cb2-Cb3)/tau2-k*Ca3*Cb3 Explicit equations as entered by the user [1] k = 0.025 [2] Cao = 2 [3] tau = 200/15 [4] X = 1 - 2*Ca3/Cao [5] tau2 = 10 [6] V = 200 [7] vbo = 5 Equilibrium conversion is 0.372. This conversion is reached at t = 85.3 minutes. 6-40 final value 100 1.1484734 0.7281523 0.6278144 0.4821755 0.7291677 0.6309679 0.025 2 13.333333 0.3721856 10 200 5 CDGA 6-2 (e) Individualized solution 6-41 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 7-1 Solutions for Chapter 7 – Collection and Analysis of Rate Data P7-1 (a) Individualized solution P7-1 (b) Individualized solution P7-1 (c) Individualized solution P7-1 (d) Individualized solution P7-2 (a) In Example 7-1, we have assumed CB as constant, but CB is varying and the error is due to the term and the maximum error occurs when this ratio is minimum. Error = 1 CB = CA0(Θ - X) Θ = 0.5/0.05 = 10 CB = CA0(10 - X) So, we have t(min) 0 50 100 150 200 250 300 CA X CB error(%) 0.05 0.038 0.0306 0. 256 0.0222 0.0195 0.0174 0 0.024 0.0388 0.0488 0.0556 0.061 0.0652 0.5 0.4988 0.49806 0.49756 0.49722 0.49695 0.49674 0 0.24 0.388 0.488 0.556 0.61 0.652 So, we have maximum error of 0.652%, hence k = 0.24 .652*0.24/100 k = 0.24 0.0015648 P7-2 (b) Example 7-3 because when α is set equal to 2, the best value of k must be found. P7-2 (c) Example 7-4 rate law: rCH 4 kPCO PH 2 7-2 Regressing the data r’(gmolCH4/gcat.min) 5.2e-3 13.2e-3 30e-3 4.95e-3 7.42e-3 5.25e-3 PCO (atm) 1 1.8 4.08 1 1 1 PH2 (atm) 1 1 1 0.1 0.5 4 See Polymath program P7-2-c.pol. POLYMATH Results Nonlinear regression (L-M) Model: r = k*(PCO^alfa)*(PH2^beta) Variable Ini guess Value k 0.1 0.0060979 alfa 1 1.1381455 beta 1 0.0103839 Precision R^2 = 0.9869709 R^2adj = 0.9782849 Rmsd = 4.176E-04 Variance = 2.093E-06 95% confidence 6.449E-04 0.0850634 0.1951217 Therefore order of reaction = 1.14 Again regressing the above data putting 1 POLYMATH Results Nonlinear regression (L-M) Model: r = k*(PCO^0.14)*(PH2) Variable Ini guess Value k 0.1 0.0040792 Precision R^2 = -0.8194508 R^2adj = -0.8194508 Rmsd = 0.0049354 Variance = 1.754E-04 95% confidence 0.0076284 Therefore, k = 0.004 (gmolCH4/(gcat.min.atm1.14)) P7-3 Solution is in the decoding algorithm given with the modules. P7-4 Individualized solution 7-3 P7-5 (a) P7-5 (b) First we fit a polynomial to the data. Using Polymath we use regression to find an expression for X(z) See Polymath program P7-5-b.pol. POLYMATH Results Polynomial Regression Report Model: X = a0 + a1*z + a2*z^2 + a3*z^3 + a4*z^4 + a5*z^5 + a6*z^6 Variable Value 95% confidence 7-4 a0 a1 a2 a3 a4 a5 a6 2.918E-14 0.0040267 -6.14E-05 7.767E-06 -5.0E-07 1.467E-08 -1.6E-10 0 0 0 0 0 0 0 General Order of polynomial = 6 Regression including free parameter Number of observations = 7 Statistics R^2 = R^2adj = Rmsd = Variance = 1 0 1.669E-10 1.0E+99 Next we differentiate our expression of X(z) to find dX/dz and knowing that dX ln ln a n ln 1 X dz n kC Ao Ac where, a FAo dX as a function of ln 1 X gives us similar vaules of slope and intercept dz Linear regression of ln as in the finite differences. POLYMATH Results Linear Regression Report Model: ln(dxdz) = a0 + a1*ln(1-X) Variable a0 a1 Value -5.531947 1.2824279 95% confidence 0.0241574 0.3446187 General Regression including free parameter Number of observations = 7 Statistics R^2 = R^2adj = Rmsd = Variance = 0.9482059 0.9378471 0.0044015 1.899E-04 n = 1.28 ln a = -5.53, a = 0.00396 7-5 k FAO a 45.7 106 moles / s 3.96 103 cm 4.0s 1 n 6 3 2 CAO AC 2.3 10 moles / cm 0.0196cm Hence rate law is, rA 4.0 C 1.28 A mol dm3 s P7-6 (a) Liquid phase irreversible reaction: A B + C ; CAO = 2 mole/dm3 C AO C A kC A C CA ln AO ln k ln C A Space time ( )min. CA(mol/dm3) ln(CA) 15 38 100 300 1200 1.5 1.25 1.0 0.75 0.5 0.40546511 0.22314355 0 -0.28768207 -0.69314718 ln((CAO-CA)/ ) -3.4011974 -3.9252682 -4.6051702 -5.4806389 -6.6846117 By using linear regression in polymath: See Polymath program P7-6-a.pol. POLYMATH Results Linear Regression Report Model: y = a0 + a1*lnCa C CA ln AO ln k ln C A Variable Value 95% confidence 7-6 a0 -4.6080579 0.0162119 a1 2.9998151 0.0411145 Statistics R^2 = 0.9999443 R^2adj = 0.9999258 Rmsd = 0.003883 Variance = 1.256E-04 Hence, slope 3 ln(k) = intercept = -4.6 therefore, k = 0.01 mole-2min-1. Rate law: dC A 0.01C A3 mol / dm3 min dt P7-6 (b) Individualized solution P7-6 (c) Individualized solution P7-7 (a) Constant voume batch reactor: Mole balance: A B +C dC A kC A dt Integrating with initial condition when t = 0 and CA = CAO for 1.0 t (1 ) C A(1 ) 1 (2)(1 ) C A(1 ) 1 C AO ……………substituting for initial concentration CAO = 2 mol/dm3. k (1 ) k (1 ) t (min.) 0 5 9 15 22 30 40 60 CA (mol/dm3) 2 1.6 1.35 1.1 0.87 0.70 0.53 0.35 See Polymath program P7-7-a.pol. POLYMATH Results Nonlinear regression (L-M) Model: t = (1/k)*((2^(1-alfa))-(Ca^(1-alfa)))/(1-alfa) Variable Ini guess Value 95% confidence k 0.1 0.0329798 3.628E-04 7-7 alfa 2 Precision R^2 = 0.9997773 R^2adj = 0.9997327 Rmsd = 0.1007934 Variance = 0.0995612 1.5151242 0.0433727 K= 0.03 (mol/dm3)-0.5.s-1 and 1.5 Hence , rate law is dC A 3 0.03C 1.5 A mol / dm .s dt P7-7 (b) Individualized solution P7-7 (c) Individualized solution P7-7 (d) Individualized solution P7-8 (a) Liquid phase reaction of methanol and triphenyl in a batch rector. CH3OH + (C6H5)3CCl (C6H5)3COCH3 + HCl A + B C + D Using second set of data, when CAO = 0.01 mol/dm3 and CBO = 0.1 mol/dm3 CA(mol/dm3) 0.1 0.0847 0.0735 0.0526 0.0357 t (h) 0 1 2 5 10 Rate law: rA kC Am C Bn n For table 2 data: CAO CBO => rA k ' C Am where k ' kCBO (1 m ) C A(1 m ) 1 (0.01)(1m ) C A(1m ) 1 C AO k' (1 m) k' (1 m) See Polymath program P7-8-a-1.pol. Using eqn E7-3.1, t POLYMATH Results Nonlinear regression (L-M) Model: t = (1/k)*((0.1^(1-m))-(Ca^(1-m)))/(1-m) Variable k m Ini guess 1 2 Value 1.815656 2.0027694 95% confidence 0.0109025 0.0021115 7-8 Nonlinear regression settings Max # iterations = 64 Precision R^2 R^2adj Rmsd Variance = 1 = 0.9999999 = 3.268E-04 = 8.902E-07 Therefore, m = 2 For first set of data, equal molar feed => CA = CB Hence, rate law becomes rA kC A2CBn kC A(2 n ) Observation table 2: for CA0 =0.01 and CB0 = 0.1 t (h) 0 0.278 1.389 2.78 8.33 16.66 t CA(mol/dm3) 1.0 0.95 0.816 0.707 0.50 0.37 (1 (2 n )) C A(1(2 n )) 1 (0.1)( 1n ) C A( 1n ) 1 C AO k (1 (2 n)) k (1 n)) See Polymath program P7-8-a-2.pol. POLYMATH Results Nonlinear regression (L-M) Model: t = (1^(-1-n)-Ca^(-1-n))/(k*(-1-n)) Variable n k Ini guess 3 2 Value 0.8319298 0.1695108 95% confidence 0.0913065 0.0092096 Nonlinear regression settings Max # iterations = 64 Precision R^2 R^2adj Rmsd Variance = 0.9999078 = 0.9998848 = 0.0233151 = 0.0048923 Therefore, n = 0.8 7-9 Hence rate law is: rA 0.17 C A2 CB0.8 mol dm3 h P7-8 (b) Individualized solution P7-9 (a) At t = 0, there is only (CH3)2O. At t = ∞, there is no(CH3)2O. Since for every mole of (CH3)2O consumed there are 3 moles of gas produced, the final pressure should be 3 times that of the initial pressure. P(∞) = 3P0 931 = 3P0 P0 ≈ 310 mm Hg P7-9 (b) Constant volume reactor at T = 504°C = 777 K Data for the decomposition of dimethylether in a gas phase: Time PT(mm Hg) 0 312 390 408 777 488 1195 562 (CH 3 ) 2 O CH 4 H 2 CO y A0 1 3 1 2 y A0 2 P V V0 0 1 X V0 because the volume is constant. P P P0 1 X at t = ∞, X = XAF = 1 N dX 1 dN A A0 rA V dt V0 dt Assume rA kC A (i.e. 1st order) C A C A0 1 X (V is constant) dX kC A0 1 X dt P P0 and X P0 Then: C A0 7-10 3155 799 931 Therefore: dX 1 dP dt P0 dt P P0 1 dP k k 1 1 P0 P P0 dt P0 P0 or dP k 1 P0 P dt P t dP P 1 P0 P 0 kdt 0 2 P0 P0 624 kt ln ln 936 P 3P0 P 1 P0 P Integrating gives: ln Therefore, if a plot of ln 624 versus time is linear, the reaction is first order. From the figure below, 936 P we can see that the plot is linear with a slope of 0.00048. Therefore the rate law is: rA 0.00048C A 1.6 y = 0.00048x - 0.02907 1.2 0.8 0.4 0 -0.4 0 1000 2000 3000 4000 P7-9 (c) Individualized solution P7-9 (d) The rate constant would increase with an increase in temperature. This would result in the pressure increasing faster and less time would be need to reach the end of the reaction. The opposite is true for colder temperatures. 7-11 P7-10 (a) Photochemical decay of bromine in bright sunlight: t (min) CA (ppm) 10 2.45 20 1.74 30 1.23 40 0.88 50 0.62 60 0.44 Mole balance: constant V dC A rA kC A dt dC ln A ln k ln C A dt Differentiation T (min) Δt (min) CA (ppm) ΔCA (ppm) C A ppm t min 10 20 10 2.45 30 10 1.74 40 10 1.23 50 10 0.88 60 10 0.62 -0.71 -0.51 -0.35 -0.26 -0.18 -0.071 -0.051 -0.035 -0.026 -0.018 7-12 10 0.44 After plotting and differentiating by equal area -dCA/dt ln(-dCA/dt) ln CA 0.082 -2.501 0.896 0.061 -2.797 0.554 0.042 -3.170 0.207 0.030 -3.507 -0.128 0.0215 -3.840 -0.478 0.014 -4.269 -0.821 Using linear regression: α = 1.0 ln k = -3.3864 k = 0.0344 min-1 P7-10 (b) dN A VrA FB 0 dt ppm mg at CA = 1 ppm rA 0.0344 0.0344 min l min mg min 1 g 3.7851l 1lbs lbs FB 25000 gal 0.0344 60 0.426 l min hr 1000 mg 1 gal 453.6 g hr P7-10 (c) Individualized solution P7-11 For the reaction, Oz + wall loss of O3 k1 Oz + alkene products k2 rO z Rate law: dCO z dt m n k 1CO z k 2CO C z Bu 7-13 Using polymath nonlinear regression we can find the values of m, n, k1 and k2 See Polymath program P7-11.pol. 7-14 P7-12 Given: Plot of percent decomposition of NO2 vs V/FA0 % Decomposition of NO 2 100 Assume that rA kC An X= For a CSTR V or FA0 X rA V X X FA0 rA kC An with n = 0, X k V FA0 X has a linear relationship with V as FA0 shown in the figure. 7-15 Therefore the reaction is zero order. P7-13 SiO2 6 HF H 2 SiF6 2 H 2O NS = moles of SiO 2 = A C ρS δ MWS AC = cross-sectional area ρS = silicon dioxide density MWS = molecular weight of silicon dioxide = 60.0 δ = depth of Si N F = moles of HF= w V 100 MWF w = weight percentage of HF in solution ρ = density of solution V = volume of solution MWF = molecular weight of HF = 20.0 Assume the rate law is rS kCF Mole balance: dN S rSV dt A d wV C S k V MWS dt 100V MWF kMWS d Vw dt 100 AC S MWF kMWS d w where V dt 100 AC S MWF d ln ln ln w dt d ln dt ln w -16.629 -15.425 -14.32 -13.816 -13.479 2.079 2.996 3.497 3.689 3.871 7-16 m d is in min dt where d and ln w we have: dt From linear regression between ln slope = α = 1.775 intercept = ln β = -20.462 or β = 1.2986 * 10-9 1.775 kMWS 1001.775 AC S MWF V AC 10*106 m 10m 2sides 1000 wafers 0.2 m2 MWS 60 S 2.32 g gmol g g 2.32*106 3 ml m (Handbook of Chemistry and Physics, 57th ed., p.B-155) g g 106 3 ml m g MWF 20 gmol 1 V 0.5 dm3 0.0005 m3 1.2986*109 1.775 6 g 10 3 9 m 1.2986*10 20 g gmol g k 60 gmol 0.0005 m3 g 1.775 0.2 m2 2.3*106 3 100 m 7-17 m3 k 3.224*10 gmol 0.775 7 Final concentration of HF min 1 5 2.316 0.2 0.107 5 weight fraction = 10.7% Initial concentration of HF = 0.2 (given) Mole balance for HF: weight fraction = 20% dN dN F 6 S dt dt dw w 6k V 100MWF dt 100 MWF V dw 1.775 6k w 100MWF 20 10.7 10.7 where α = 1.775 0.775 t dt 0 1 1 106 7 6 3.224*10 0.775 w0.775 20 20*100 0.775 t 1 1 1 0.775 2.389*104 t 0.775 0.775 10.7 20 t 331 min P7-14 See Polymath program P7-14.pol 7-18 P7-15 The following are the mistakes in the given solution, followed by the corrected solution:- AB+C For a batch Reactor, dC A rA kC A dt dC A kC A dt Taking ln both sides, ln( dC A ) ln k ln C A dt 7-19 (1) The value of △CA/△t cannot be calculated for t=0. It can only be calculated for t=1 onwards. (2) The values of △CA/△t calculated for t=1, 2, 3 etc. have been incorrectly calculated. t Ca ln Ca Delta t delta Ca/ delta t ln ( -delta Ca/ delta t) 0 1 0 1 0.5 -0.7 1 -0.5 -0.7 2 0.3 -1.2 1 -0.2 -1.61 3 0.2 -1.61 1 -0.1 -2.3 4 0.15 -1.9 1 -0.05 -3 (3) The graph has to be plotted for ln (-△CA/△t) vs. ln (CA) and not ‘t’. (4) So, the value of α from the graph = 1.88, not 0.5. (5) ln k = 0.64 from the graph, which gives k = 1.89 Therefore, we get dC A rA 1.89C1.88 A dt 7-20 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . 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All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 8-1 Solutions for Chapter 8 – Multiple Reactions P8-1 Individualized solution P8-2 (a) Example 8-1 For PFR (gas phase with no pressure drop or liquid phase), dC A d dC B d k1 k 2C A dC X d dCY d k 3C A2 k 2C A k1 k 3 C A2 In PFR with V = 1566 dm3 we get τ = V/v0 = 783 X = 0.958 , SB/XY (instanteneous) = 0.244, and SB/XY (overall) = 0.624 also at τ = 350, SB/XY (instanteneous) is at its maximum value of 0.84 See polymath problem P8-2-1.pol Calculated values of the DEQ variables Variable initial value tau 0 Ca 0.4 Cx 1.0E-07 Cb 0 Cy 1.0E-06 Cao 0.4 X 0 k1 1.0E-04 k2 0.0015 k3 0.008 Sbxy_over 0 Sbxy_inst 0.4347826 minimal value 0 0.0166165 1.0E-07 0 1.0E-06 0.4 0 1.0E-04 0.0015 0.008 0 0.2438609 maximal value 783 0.4 0.0783001 0.1472919 0.1577926 0.4 0.9584587 1.0E-04 0.0015 0.008 0.6437001 0.8385161 8-2 final value 783 0.0166165 0.0783001 0.1472919 0.1577926 0.4 0.9584587 1.0E-04 0.0015 0.008 0.6238731 0.2438609 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(tau) = -k1-k2*Ca-k3*Ca^2 [2] d(Cx)/d(tau) = k1 [3] d(Cb)/d(tau) = k2*Ca [4] d(Cy)/d(tau) = k3*Ca^2 Explicit equations as entered by the user [1] Cao = 0.4 [2] X = 1-Ca/Cao [3] k1 = 0.0001 [4] k2 = 0.0015 [5] k3 = 0.008 [6] Sbxy_overall = Cb/(Cx+Cy) [7] Sbxy_instant = k2*Ca/(k1+k3*Ca^2) Independent variable variable name : tau initial value : 0 final value : 783 (2) PFR - Pressure increased by a factor of 100. (a) Liquid phase: No change, as pressure does not change the liquid volume appreciably. (b) Gas Phase: Now CA0 = P/RT = 100 (P0_initial)/RT = 0.4 × 100 = 40 mol/dm3 Running with CA0 = 40 mol/dm3, we get: X = 0.998 , SB/XY (instanteneous) = 0.681, and SB/XY (overall) = 0.024 As a practice, students could also try similar problem with the CSTR. P8-2 (b) Example 8-2 (a) CSTR: intense agitation is needed, good temperature control. 8-3 (b) PFR: High conversion attainable, temperature control is hard – non-exothermic reactions, selectivity not an issue (c) Batch: High conversion required, expensive products (d) and (e) Semibatch: Highly exothermic reactions, selectivity i.e. to keep a reactant concentration low, to control the conversion of a reactant. (f) and (g) Tubular with side streams: selectivity i.e. to keep a reactant concentration high, to achieve higher conversion of a reactant. (h) Series of CSTR’s: To keep a reactant concentration high, easier temperature control than single CSTR. (i) PFR with recycle: Low conversion to reuse reactants, gas reactants, for highly exothermic reactions (j) CSTR with recycle: Low conversions are achieved to reuse reactants, temperature control, liquid reactants , for highly exothermic reactions (k) Membrane Reactor: yield i.e. series reactions that eliminate a desired product , used for thermodynamically limited reactions where the equilibrium shifts on left side. (l) Reactive Distillation: when one product is volatile and the other is not ; for thermodynamically limited gas phase reactions. P8-2 (c) Example 8-3 (1) For k1 = k2, we get CA k1 ' C AO exp and d d C B exp k1 ' dCB d ' Wopt CB 0 ' opt vo k1 k1C B k1C AO exp k1 ' k1C AO 0 , CB = 0 Optimum yield: ' ' d ' Now at dC B k1C AO ' exp k1C AO exp k1 ' k1 ' k1 ' exp 1 exp k1 ' k1 ' 1 k1 and X opt 1 e 1 =0.632 P8-2 (d) Example 8-4 According to the plot of CB versus T the maximum temperature is T = 310.52 0C. 8-4 CB k2 k1C A0 1 k1 1 POLYMATH Results See polymath problem P8-2-1.pol Calculated values of the DEQ variables Variable t T Cao tau k1o k2o E1 E2 R k1 k2 Cb initial value 0 300 5 0.5 0.4 0.01 10 20 0.001987 0.4 0.4 0.6944444 minimal value 0 300 5 0.5 0.4 0.01 10 20 0.001987 0.4 0.4 0.0052852 maximal value 100 400 5 0.5 0.4 0.01 10 20 0.001987 26.513034 1757.3524 0.8040226 ODE Report (RKF45) Differential equations as entered by the user [1] d(T)/d(t) = 1 Explicit equations as entered by the user [1] Cao = 5 [2] tau = .5 [3] k1o = .4 [4] k2o = .01 [5] E1 = 10 [6] E2 = 20 [7] R = .001987 [8] k1 = k1o*exp((-E1/R)*(1/T-1/300)) 8-5 final value 100 400 5 0.5 0.4 0.01 10 20 0.001987 26.513034 1757.3524 0.0052852 [9] k2 = k1o*exp((-E2/R)*(1/T-1/300)) [10] Cb = (tau*k1*Cao)/(tau*k2+1)/(tau*k1+1) P8-2 (e) Individualized solution P8-2 (f) Individualized solution P8-2 (g) Individualized solution P8-2 (h) Example 8-8 (1) Membrane Reactor PFR SD/U Original Problem 2.58 0.666 SD/U P8-2 h 1.01 0.208 Doubling the incoming flow rate of species B lowers the selectivity. (2) The selectivity becomes 6.52 when the first reaction is changed to A+2B D P8-2 (i) CDROM Example Original Case – CDROM example P8-2 i The reaction does not go as far to completion when the changes are made. The exiting concentration of D, E, and F are lower, and A, B, and C are higher. See Polymath program P8-2-i.pol. P8-2 (j) For equal molar feed in hydrogen and mesitylene. CHO = yHOCTO = (0.5)(0.032)lbmol/ft3 =0.016 lbmol/ft3 CMO = 0.016 lbmol/ft3 Using equations from example, solving in Polymath, we get 8-6 opt 0.38 hr. At 0.5 hr all of the H2 is reacted and only the decomposition of X takes place. XH CH CM CX ~ S X /T CD-ROM example 0.50 0.0105 0.0027 0.00507 0.2hr 0.596 This question 0.99 0.00016 0.0042 0.0077 0.38hr 1.865 See Polymath program P8-2-j.pol. POLYMATH Results Calculated values of the DEQ variables Variable tau CH CM CX k1 k2 r1M r2T r1H r2H r1X r2X initial value 0 0.016 0.016 0 55.2 30.2 -0.1117169 0 -0.1117169 0 0.1117169 0 minimal value 0 1.64E-06 0.0041405 0 55.2 30.2 -0.1117169 0 -0.1117169 -0.0159818 2.927E-04 -0.0159818 maximal value 0.43 0.016 0.016 0.0077216 55.2 30.2 -2.927E-04 0.0159818 -2.927E-04 0 0.1117169 0 ODE Report (RKF45) Differential equations as entered by the user [1] d(CH)/d(tau) = r1H+r2H [2] d(CM)/d(tau) = r1M [3] d(CX)/d(tau) = r1X+r2X Explicit equations as entered by the user [1] k1 = 55.2 [2] k2 = 30.2 [3] r1M = -k1*CM*(CH^.5) [4] r2T = k2*CX*(CH^.5) [5] r1H = r1M [6] r2H = -r2T [7] r1X = -r1M [8] r2X = -r2T ~ Increasing θH decreases τopt and S X/T. P8-2 (k) 8-7 final value 0.43 1.64E-06 0.0041405 0.0077207 55.2 30.2 -2.927E-04 2.986E-04 -2.927E-04 -2.986E-04 2.927E-04 -2.986E-04 From CD-ROM example Polymath code: See Polymath program P8-2-k.pol. POLYMATH Results NLES Solution Variable CH CM CX tau K1 K2 CHo CMo Value 4.783E-05 0.0134353 0.0023222 0.5 55.2 30.2 0.016 0.016 f(x) -4.889E-11 -1.047E-11 -9.771E-12 Ini Guess 1.0E-04 0.013 0.002 NLES Report (safenewt) Nonlinear equations [1] f(CH) = CH-CHo+K1*(CM*CH^.5+K2*CX*CH^.5)*tau = 0 [2] f(CM) = CM-CMo+K1*CM*CH^.5*tau = 0 [3] f(CX) = (K1*CM*CH^.5-K2*CX*CH^0.5)*tau-CX = 0 Explicit equations [1] tau = 0.5 [2] K1 = 55.2 [3] K2 = 30.2 [4] CHo = 0.016 [5] CMo = 0.016 A plot using different values of is given. For =0.5, the exit concentration are CH = 4.8 ×10-5 lbmol/ft3 CM =0.0134 lbmol/ft3 CX =0.00232 lbmol/ft3 The yield of xylene from mesitylene based on molar flow rates exiting the CSTR for YMX FX FMO CX FM C MO CM 0.00232 0.016 0.0134 0.89mole xylene produced mole mesitylene reacted The overall selectivity of xylene relative to toluene is: FX FT 8.3mole xylene produced mole toluene produced YMX CD-ROM example 0.0089 0.0029 0.0033 0.5 0.41 ~ S X /T CH CM CX This Question 4.8 x 10-5 0.0134 0.00232 0.5 0.89 8-8 =0.5: SX/T 0.7 8.3 P8-2 (l) At the beginning, the reactants that are used to create TF-VIIa and TF-VIIaX are in high concentration. As the two components are created, the reactant concentration drops and equilibrium forces the production to slow. At the same time the reactions that consume the two components begin to accelerate and the concentration of TF-VIIa and TF-VIIaX decrease. As those reactions reach equilibrium, the reactions that are still producing the two components are still going and the concentration rises again. Finally the reactions that consume the two components lower the concentration as the products of those reactions are used up in other reactions. P8-2 (m) Individualized solution P8-3 Solution is in the decoding algorithm given with the modules (ICM problem ) P8-4 (a) Assume that all the bites will deliver the standard volume of venom. This means that the initial concentration increases by 5e-9 M for every bite. After 11 bites, no amount of antivenom can keep the number of free sites above 66.7% of total sites. This means that the initial concentration of venom would be 5.5e-8 M. The best result occurs when a dose of antivenom such that the initial concentration of antivenom in the body is 5.7e-8 M, will result in a minimum of 66.48% free sites, which is below the allowable minimum. P8-4 (b) 8-9 The victim was bitten by a harmless snake and antivenom was injected. This means that the initial concentration of venom is 0. From the program below, we see that if an amount of antivenom such that the initial concentration in the blood is 7e-9 M, the patient will die. See Polymath program P8-4-b.pol. POLYMATH Results Calculated values of the DEQ variables Variable t fsv fs Cv Ca fsa Cp kv ksv ka kia Cso ksa kp kov koa kop g h m j initial value 0 0 1 0 7.0E-09 0 0 2.0E+08 6.0E+08 2.0E+08 1 5.0E-09 6.0E+08 1.2E+09 0 0.3 0.3 0 0 0 -2.1E-09 minimal value 0 0 0.6655661 0 4.503E-09 0 0 2.0E+08 6.0E+08 2.0E+08 1 5.0E-09 6.0E+08 1.2E+09 0 0.3 0.3 0 0 0 -2.1E-09 maximal value 0.5 0 1 0 7.0E-09 0.3344339 0 2.0E+08 6.0E+08 2.0E+08 1 5.0E-09 6.0E+08 1.2E+09 0 0.3 0.3 0 0 0 -1.351E-09 ODE Report (STIFF) Differential equations as entered by the user [1] d(fsv)/d(t) = kv * fs * Cv - ksv * fsv * Ca [2] d(fs)/d(t) = -kv*fs*Cv - ka * fs * Ca + kia * fsa + g [3] d(Cv)/d(t) = Cso * (-kv * fs * Cv - ksa * fsa * Cv) + h [4] d(Ca)/d(t) = Cso*(-ka * fs * Ca + kia * fsa) + j [5] d(fsa)/d(t) = ka * fs * Ca - kia * fsa - ksa * fsa * Cv [6] d(Cp)/d(t) = Cso * (ksv * fsv * Ca + ksa * fsa * Cv) + m Explicit equations as entered by the user [1] kv = 2e8 [2] ksv = 6e8 [3] ka = 2e8 [4] kia = 1 [5] Cso = 5e-9 [6] ksa = 6e8 8-10 final value 0.5 0 0.6655661 0 4.503E-09 0.3344339 0 2.0E+08 6.0E+08 2.0E+08 1 5.0E-09 6.0E+08 1.2E+09 0 0.3 0.3 0 0 0 -1.351E-09 [7] kp = 1.2e9 [8] kov = 0 [9] koa = 0.3 [10] kop = 0.3 [11] g = ksa * fsa * Cv + ksv * fsv * Ca [12] h = -kp * Cv * Ca - kov * Cv [13] m = kp * Cv * Ca - kop * Cp [14] j = -Cso * ksv * fsv * Ca - kp * Cv * Ca - koa * Ca P8-4 (c) The latest time after being bitten that antivenom can successfully be administerd is 27.49 minutes. See the cobra web module on the CDROM/website for a more detailed solution to this problem P8-4 (d) Individualized Solution P8-5 (a) Plot of CA, CD and CU as a function of time (t): See Polymath program P8-5-a.pol. POLYMATH Results Calculated values of the DEQ variables 8-11 Variable t Ca Cd Cu k1 k2 K1a K2a Cao X initial value 0 1 0 0 1 100 10 1.5 1 0 minimal value 0 0.0801802 0 0 1 100 10 1.5 1 0 maximal value 15 1 0.7995475 0.5302179 1 100 10 1.5 1 0.9198198 final value 15 0.0801802 0.7995475 0.1202723 1 100 10 1.5 1 0.9198198 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = -(k1*(Ca-Cd/K1a)+k2*(Ca-Cu/K2a)) [2] d(Cd)/d(t) = k1*(Ca-Cd/K1a) [3] d(Cu)/d(t) = k2*(Ca-Cu/K2a) Explicit equations as entered by the user [1] k1 = 1.0 [2] k2 = 100 [3] K1a = 10 [4] K2a = 1.5 [5] Cao = 1 [6] X = 1-Ca/Cao To maximize CD stop the reaction after a long time. The concentration of D only increases with time P8-5 (b) Conc. Of U is maximum at t = 0.31 min.(CA = 0.53) P8-5 (c) Equilibrium concentrations: CAe = 0.08 mol/dm3 CDe = 0.8 mol/dm3 CUe = 0.12 mol/dm3 8-12 P8-5 (d) See Polymath program P8-5-d.pol. POLYMATH Results NLES Solution Variable Ca Cd Cu Ca0 k1 k2 K1a K2a t Value 0.0862762 0.7843289 0.1293949 1 1 100 10 1.5 100 f(x) -3.844E-14 -2.631E-14 6.478E-14 Ini Guess 1 0 0 NLES Report (safenewt) Nonlinear equations [1] f(Ca) = Ca0-t*(k1*(Ca-Cd/K1a)+k2*(Ca-Cu/K2a))-Ca = 0 [2] f(Cd) = t*k1*(Ca-Cd/K1a)-Cd = 0 [3] f(Cu) = t*(k2*(Ca-Cu/K2a))-Cu = 0 1 min 10 min 100min CAexit 0.295 0.133 0.0862 CDexit 0.2684 0.666 0.784 CUexit 0.436 0.199 0.129 X 0.705 0.867 0.914 Explicit equations [1] Ca0 = 1 [2] k1 = 1 [3] k2 = 100 [4] K1a = 10 [5] K2a = 1.5 [6] t = 100 [7] X = 1-Ca/Ca0 P8-6 (a) A X rX 1/ 2 k1C A A B rB k 2C A rY 2 A Y k 3C A 1/ 2 k1 mol 0.004 dm 3 k2 0.3 min 1 k3 dm 3 0.25 mol. min Sketch SBX, SBY and SB/XY as a function of CA 8-13 min See Polymath program P8-6-a.pol. It shows the table of SBX, SBY and SB/XY in correspondence with values of CA . 1) SB/X = rB rX 2) SB/Y = rB rY 3) SB/XY = k 2C A k1C A1/ 2 k 2C A k 3C A 2 rB rX k2 C A1/ 2 k1 k2 k 3C A k 2C A rY k1C A1/ 2 k 3C A 2 8-14 P8-6 (b) Volume of first reactor can be found as follows We have to maximize SB/XY From the graph above, maximum value of SBXY = 10 occurs at CA* = 0.040 mol/dm3 So, a CSTR should be used with exit concentration CA* Also, CA0 = PA/RT = 0.162 mol/dm3 And rA => V v0 (C A0 C A* ) rA rX rB rY (k1C A1/ 2 k 3C A 2 ) k 2C A v0 (C A0 * 1/ 2 (k1 (C A ) C A* ) * k 3 (C A ) ) CB* 0.11 k 2C A * 2 P8-6 (c) Effluent concentrations: CB rB We know, τ = 9.24 min => Similarly: C X * 0.007 mol dm 3 and CB k 2C A CY * 0.0037 P8-6 (d) Conversion of A in the first reactor: C A0 CA C A0 X X 0.74 P8-6 (e) A CSTR followed by a PFR should be used. Required conversion = 0.99 => For PFR, Mole balance: dV dX F A0 rA 8-15 mol dm 3 mol dm 3 92.4dm 3 0.99 V 10 0.162 dX 1/ 2 0.74 ( k1C A k 2C A 2 92.8dm 3 k 3C A ) P8-6 (f) If we notice that E2 is the smallest of the activation energies, we get a higher selectivity at lower temperatures. However, the tradeoff is that the reaction rate of species B, and therefore production of B, decrease as temperature drops. So we have to compromise between high selectivity and production. To do this we need expressions for k1, k2, and k3 in terms of temperature. From the given data we know: ki Ei 1.98T Ai exp Since we have the constants given at T = 300 K, we can solve for Ai. A1 A2 A3 .004 1.49e12 20000 exp 1.98 300 .3 5.79e6 10000 exp 1.98 300 .25 1.798e21 30000 exp 1.98 300 Now we use a mole balance on species A V V FA0 FA rA v C A0 C A rA C A0 C A rA C A0 C A k1C k2C A k3C A2 0.5 A A mole balance on the other species gives us: Fi vCi Ci ri rV i 8-16 Cb versus temp 0.072 0.07 0.068 0.066 Cb 0.064 0.062 0.06 285 290 295 300 305 310 315 Using these equations we can make a Polymath program and by varying the temperature, we can find a maximum value for CB at T = 306 K. At this temperature the selectivity is only 5.9. This may result in too much of X and Y, but we know that the optimal temperature is not above 306 K. The optimal temperature will depend on the price of B and the cost of removing X and Y, but without actual data, we can only state for certain that the optimal temperature will be equal to or less than 306 K. See Polymath program P8-6-f.pol. POLYMATH Results NLE Solution Variable Ca T R k1 k2 Cao Cb k3 tau Cx Cy Sbxy Value 0.0170239 306 1.987 0.0077215 0.4168076 0.1 0.070957 0.6707505 10 0.0100747 0.0019439 5.9039386 f(x) 3.663E-10 Ini Guess 0.05 NLE Report (safenewt) Nonlinear equations [1] f(Ca) = (Cao-Ca)/(k1*Ca^.5+k2*Ca+k3*Ca^2)-10 = 0 Explicit equations [1] T = 306 8-17 [2] R = 1.987 [3] k1 = 1.49e12*exp(-20000/R/T) [4] k2 = 5790000*exp(-10000/R/T) [5] Cao = .1 [6] Cb = 10*k2*Ca [7] k3 = 1.798e21*exp(-30000/R/T) [8] tau = 10 [9] Cx = tau*k1*Ca^.5 [10] Cy = tau*k3*Ca^2 [11] Sbxy = Cb/(Cx+Cy) P8-6 (g) Concentration is proportional to pressure in a gas-phase system. Therefore: PA S B / XY ~ PA PA2 which would suggest that a low pressure would be ideal. But as before the tradeoff is lower production of B. A moderate pressure would probably be best. We know that : SB/XY = rB rX k 2C A rY k1C A1/ 2 k 3C A 2 Substituting PA = CA R T ; in the above co – relation we get rB SB/XY = rX rY k2 ( PA / RT ) k1 ( PA / RT )1/2 k3 ( PA / RT ) 2 See Polymath program P8-6-g.pol. Thus we find that the maximum is obtained at P= 1 atm . 8-18 P8-7 US legal limit: 0.8 g/l Sweden legal limit: 0.5 g/l A k1 B k2 C Where A is alcohol in the gastrointestinal tract and B is alcohol in the blood stream dC A k1C A dt dCB k1C A k2 dt k1 10 hr 1 k2 0.192 g L hr Two tall martinis = 80 g of ethanol Body fluid = 40 L C A0 80 g 40 L 2 g L Now we can put the equations into Polymath. See Polymath program P8-7.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k1 k2 initial value 0 2 0 10 0.192 minimal value 0 7.131E-44 0 10 0.192 maximal value 10 2 1.8901533 10 0.192 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = -k1*Ca [2] d(Cb)/d(t) = -k2+k1*Ca Explicit equations as entered by the user [1] k1 = 10 [2] k2 = 0.192 P8-7 (a) In the US the legal limit it 0.8 g/L. 8-19 final value 10 7.131E-44 0.08 10 0.192 This occurs at t = 6.3 hours.. P8-7 (b) In Sweden CB = 0.5 g/l , t = 7.8 hrs. P8-7 (c) In Russia CB = 0.0 g/l, t = 10.5 hrs P8-7 (d) For this situation we will use the original Polymath code and change the initial concentration of A to 1 g/L. Then run the Program for 0.5 hours. This will give us the concentration of A and B at the time the second martini is ingested. This means that 1 g/l will be added to the final concentration of A after a half an hour. At a half an hour CA = 0.00674 g/L and CB = 0.897 g/L. The Polymath code for after the second drink is shown below. See Polymath program P8-7-d.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k1 k2 initial value 0.5 1.0067379 0.8972621 10 0.192 minimal value 0.5 5.394E-42 0.08 10 0.192 maximal value 10 1.0067379 1.8069769 10 0.192 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = -k1*Ca [2] d(Cb)/d(t) = -k2+k1*Ca Explicit equations as entered by the user [1] k1 = 10 [2] k2 = 0.192 for the US t = 6.2 hours Sweden: t = 7.8 hours Russia: t =10.3 hours. P8-7 (e) 8-20 final value 10 5.394E-42 0.08 10 0.192 The mole balance on A changes if the drinks are consumed at a continuous rate for the first hour. 80 g of ethanol are consumed in an hour so the mass flow rate in is 80 g/hr. Since volume is not changing the rate of change in concentration due to the incoming ethanol is 2 g/L/hr. For the first hour the differential equation for CA becomes: dC A dt k1C A 2t after that it reverts back to the original equations. See Polymath program P8-7-e.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k1 k2 initial value 0 0 0 10 0.192 minimal value 0 0 -1.1120027 10 0.192 maximal value 11 0.1785514 0.7458176 10 0.192 final value 11 6.217E-45 -1.1120027 10 0.192 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = if(t<1)then(-k1*Ca+2*t)else(-k1*Ca) [2] d(Cb)/d(t) = -k2+k1*Ca Explicit equations as entered by the user [1] k1 = 10 [2] k2 = 0.192 US: CB never rises above 0.8 g/L so there is no time that it would be illegal. Sweden: t = 2.6 hours Russia: t = 5.2 hours P8-7 (f) 60 g of ethanol immediately CA = 1.5 g/L CB = 0.8 g/L at 0.0785 hours or 4.71 minutes. So the person has about 4 minutes and 40 seconds to get to their destination. P8-7 (g) A heavy person will have more body fluid and so the initial concentration of CA would be lower. This means a heavier person will reach the legal limit quicker. The opposite is true for a slimmer person. They will take longer to reach the legal limit, as their initial concentration will be higher. 8-21 P8-8 (a) See Polymath program P8-8-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cb k1 k2 k4 k3 initial value 0 6.25 0 0.15 0.6 0.2 0.1 minimal value 0 0.3111692 0 0.15 0.6 0.2 0.1 maximal value 4 6.25 0.5977495 0.15 0.6 0.2 0.1 ODE Report (RKF45) Differential equations as entered by the user [1] d(Ca)/d(t) = -k1*Ca-k2*Ca [2] d(Cb)/d(t) = k1*Ca-k3-k4*Cb Explicit equations as entered by the user [1] k1 = 0.15 [2] k2 = 0.6 [3] k4 = 0.2 [4] k3 = if(Cb<0)then (k1*Ca-k4*Cb) else (0.1) P8-8 (b) 8-22 final value 4 0.3111692 0.4057018 0.15 0.6 0.2 0.1 8-23 P8-8 (c) If one takes initially two doses of Tarzlon, it is not recommended to take another dose within the first six hours. Doing so will result in build up of the drug in the bloodstream that can cause harmful effects. P8-8 (d) If the drug is taken on a full stomach most of it will not reach the wall at all. The processed food can also drag the drug to the intestines and may limit its effectiveness. This effect can be seen in the adsorption constant k1 and elimination constant k2 values. If k1 decreases this means that the adsorption process is slow and if k2 increases means that the rate of elimination of Tarzlon increases. The next graph shows the concentration profiles for k1 = 0.10 h-1 and k2 = 0.8 h-1. Note that the maximum amount of the drug in the bloodstream is reduced by two. Concentration Profiles Ca (mg/dm3) Cb (mg/dm3) 0.6 CB (mg/dm3) CA (mg/dm3) 8 6 0.4 4 0.2 2 0 0 0 2 4 6 8 10 12 Time (h) Concentration profile for Tarzlon in the stomach (A) and bloodstream (B). The maximum amount of Tarzlon in the bloodstream is 0.3 mg/dm3. P8-9 (a) Reactor selection A B D rD r1 A r1 A 10 exp( 8000 K / T )C AC B A B U rU r2 A r2 A SDU = rD rU 10 exp( 8000 K / T )C A C B 1/ 2 100 exp( 1000 K / T )C A C B 1/ 2 100 exp( 1000 K / T )C A C B exp( 8000 K / T )C A 3/ 2 10 exp( 1000 K / T )C B At T = 300K 1/ 2 k1 = 2.62 x 10-11 & k2 = 3.57 SD/U 1/ 2 7.35 10 12 C A 1/ 2 CB At T = 1000K 8-24 1/ 2 3/ 2 -3 k1 = 3.35 x 10 & k2 =36.78 SD/U 9.2 10 5 C A CB 1/ 2 1/ 2 Hence In order to maximize SDU, use higher concentrations of A and lower concentrations of B. This can be achieved using: 1) A semibatch reactor in which B is fed slowly into a large amount of A 2) A tubular reactor with side streams of B continually fed into the reactor 3) A series of small CSTR’s with A fed only to the first reactor and small amounts of B fed to each reactor. Also, since ED > EU, so the specific reaction rate for D increases much more rapidly with temperature. Consequently, the reaction system should be operated at highest possible temperature to maximize SDU. 1 CB Note that the selectivity is extremely low, and the only way to increase it is to keep CA 2 10 6 and add B drop by drop. P8-9 (b) A B D and r1 A 100 exp( 1000 K / T )C AC B A B U and r2 A 106 exp( 8000K / T )C ACB SDU = rD rU 100 exp( 1000 K / T )C AC B 10 6 exp( 8000 K / T )C AC B exp( 1000 K / T ) 10 4 exp( 8000 K / T ) At T = 300K k1 = 3.57 & k2 = 2.623 SDU = 1.14 x106 At T = 1000K k1 = 36.78 & k2 = 3354.6 SDU = 0.103 Hence temperature should be kept as low as possible to maximize SDU, but at the same time care should be taken to have a significant reaction extent. P8-9 (c) A B D and r1 A 10 exp( 8000 K / T )C ACB B D r2 A 109 exp( 10, 000 K / T )CB CD U and 8-25 r1 A r2 A S DU 10 exp 8000 K / T C ACB 109 exp 10000 K / T CBCD exp S DU 8000 / T C A 8 10 exp 10000 / T CD Therefore the reaction should be run at a low temperature to maximize SDU, but not too low to limit the production of desired product. The reaction should also take place in high concentration of A and the concentration of D should be limited by removing through a membrane or reactive distillation. P8-9 (d) A D and D U1 and A U 2 and rD S D / U 1U 2 rU 1 rU 2 At T = 300K k1 = 1.18 x 10-14 & r1 A 4280 exp( 12000 K / T )C A r2 D 10,100 exp( 15000 K / T )C D r3 A 26 exp( 10800 K / T )C A 4280 exp( 12000 K / T )C A 10,100 exp( 15000 K / T )C D 10,100 exp( 15000 K / T )C D 26 exp( 10800 K / T )C A k2 = 1.94 X 10-18 & k3 = 6.03 x 10-15 If we keep CA > 1000CD S D / U 1U 2 1.18 10 14 C A 1.94 10 18 C D 1.94 10 18 C D 6.03 10 15 C A At T = 1000K k1 = 0.026 & 1.18 1.96 .603 k2 = 3.1 X 10-3 & k3 = 5.3 x 10-4 If we keep CA > 1000CD S D / U 1U 2 0.026C A 3.1 10 3 C D 3.1 10 3 C D 5.3 10 4 C A .026 .00053 49 Here, in order to lower U1 use low temperature and high concentration of A But low temperature and high concentration of A favours U2 So, it’s a optimization problem with the temperature and concentration of A as the variables . Membrane reactor in which D is diffusing out can be used. P8-9 (e) A B D and r1 A 10 9 exp( 10000 K / T )C A C B 8-26 D A B A B U S D /U rD rU and r2 D 20 exp( 2000 K / T )C D and r3 A 103 exp( 3000K / T )C AC B 10 9 exp( 10000 K / T )C AC B 20 exp( 2000 K / T )C D 10 3 exp( 3000 K / T )C A C B At T = 300K k1 = 3.34 x 10-6 & k2 = 0.025 & k3 = 0.045 The desired reaction lies very far to the left and CD is probably present at very low concentrations so that: S D /U 3.34 10 6 C A C B 0.025C D 0.045C A C B S D /U 0 At T = 1000K k1 = 45399.9 & 0.000334 4.5 0.000074 k2 = 2.7 & k3 = 49.7 If we assume that CACB > 0.001CD then, S D /U 45399.9C A C B 2.7C D 49.7C A C B 45399 49.7 913 Here we need a high temperature for a lower reverse reaction of D and lower formation of U Also we need to remove D as soon as it is formed so as to avoid the decomposition. P8-9 (f) A B D and r1 A 10 exp( 8000 K / T )C ACB A U and r2 A 26 exp( 10,800 K / T )C A U A and r3U 1000 exp( 15, 000 K / T )CU SD /U rD rU 10exp( 8000 K / T )C ACB 26exp( 10,800 K / T )C A 1000exp 15, 000 K / T CU We want high concentrations of B and U in the reactor. Also low temperatures will help keep the selectivity high. If we use pseudo equilibrium and set –rA = 0. rA 10 exp 8000 C AC B T 26 exp 10800 C A 1000 exp T 8-27 15000 CU T 0 10 exp CA CU CA CU 8000 CB T 26 exp 1000 exp 15000 T 10800 T 1 7000 26 4200 exp CB exp 100 T 1000 T P8-9 (g) A B D and r1 A 800 exp( 8000 K / T )C A0.5CB A B U1 and r2 B 10 exp( 300 K / T )C ACB D B U2 and r3 D 106 exp( 8000 K / T )CD CB 800 exp 8000 / T C A0.5CB 80 exp 10 exp 300 / T C ACB exp (1) S D / U1 8000 / T 300 / T C A0.5 At T = 300 S D / U1 2.098*10 10 0.368C A0.5 At T = 1000 S D / U1 29.43 0.7408C A0.5 To keep this selectivity high, low concentrations of A, and high temperatures should be used. S D /U 2 800 exp 8000 / T C A0.5CB 106 exp 8000 / T CD CB 800C A0.5 106 CD To keep this selectivity high, high concentrations of A and low concentrations of D should be used. Try to remove D with a membrane reactor or reactive distillation. The selectivity is not dependant on temperature. To keep optimize the reaction, run it at a low temperature to maximized SD/U1 in a membrane reactor that allows only D to diffuse out. (2) S D / U 1U 2 S D / U 1U 2 800 exp 10 exp 300 / T C ACB 106 exp 800 exp 10 exp 8000 / T C A0.5CB 8000 / T CD CB 8000 / T C A0.5 300 / T C A 106 exp 8000 / T CD 8-28 At T = 300 S D /U 1U 2 2.09*10 9 C A0.5 3.67C A 2.62*10 6 CD 0 At T = 1000 and very low concentrations of D S D /U 1U 2 0.268C A0.5 7.408C A 335CD .03617 C A0.5 If temperature is the only parameter that can be varied, then the highest temperature possible will result in the highest selectivity. Also removing D will help keep selectivity high. P8-10 (a) Species A : dCa dt rA ; -rA = k1 * Ca Species B: dCb dt rb rB = k1 * Ca – k2 * Cb Species C: dCc dt rc rC = k2*Cb See polymath program P8-10-a.pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 1.6 6.797E-18 1.6 6.797E-18 2 Cb 0 0 1.455486 0.6036996 3 Cc 0 0 0.9963004 0.9963004 4 k1 0.4 0.4 0.4 0.4 5 k2 0.01 0.01 0.01 0.01 8-29 6 ra -0.64 -0.64 -2.719E-18 -2.719E-18 7 rb 0.64 -0.0132415 0.64 -0.006037 8 rc 0 0 0.0145549 0.006037 9 t 0 0 100. 100. Differential equations 1 d(Cc)/d(t) = rc 2 d(Cb)/d(t) = rb 3 d(Ca)/d(t) = ra Explicit equations 1 k2 = 0.01 2 rc = k2*Cb 3 k1 = 0.4 4 ra = - k1*Ca 5 rb = k1*Ca - k2*Cb P8-10 (b) Now the rate laws will change ra = k1-1Cb – k1*Ca rb =k1*Ca – k1-1Cb – k2*Cb rc = k2*Cb See polymath program P8-10-b.pol Calculated values of DEQ variables 8-30 Variable Initial value Minimal value Maximal value Final value 1 Ca 1.6 0.3949584 1.6 0.3949584 2 Cb 0 0 0.8736951 0.5191343 3 Cc 0 0 0.6859073 0.6859073 4 k1 0.4 0.4 0.4 0.4 5 k1b 0.3 0.3 0.3 0.3 6 k2 0.01 0.01 0.01 0.01 7 ra -0.64 -0.64 -0.0022431 -0.0022431 8 rb 0.64 -0.0047669 0.64 -0.0029483 9 rc 0 0 0.008737 0.0051913 10 t 0 0 100. 100. Differential equations 1 d(Ca)/d(t) = ra 2 d(Cb)/d(t) = rb 3 d(Cc)/d(t) = rc Explicit equations 1 k1 = 0.4 2 k2 = 0.01 3 k1b = 0.3 4 ra = k1b*Cb - k1*Ca 5 rb = k1*Ca - k1b*Cb - k2*Cb 6 rc = k2*Cb 8-31 P8-10 (c) rC = k2*CB – k-2*Cc See polymath program P8-10-c.pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 1.6 0.4500092 1.6 0.4500092 2 Cb 0 0 0.8742432 0.5953978 3 Cc 0 0 0.554593 0.554593 4 k1 0.4 0.4 0.4 0.4 5 k1b 0.3 0.3 0.3 0.3 6 k2 0.01 0.01 0.01 0.01 7 k2c 0.005 0.005 0.005 0.005 8 ra -0.64 -0.64 -0.0013843 -0.0013843 9 rb 0.64 -0.0044688 0.64 -0.0017967 10 rc 0 0 0.0085186 0.003181 11 t 0 0 100. 100. Differential equations 1 d(Ca)/d(t) = ra 2 d(Cb)/d(t) = rb 3 d(Cc)/d(t) = rc Explicit equations 1 k1 = 0.4 2 k2 = 0.01 3 k1b = 0.3 4 k2c = 0.005 5 ra = k1b*Cb - k1*Ca 6 rb = k1*Ca - k1b*Cb - k2*Cb + k2c*Cc 7 rc = k2*Cb - k2c*Cc 8-32 P8-10 (d) When k1 > 100 and k2 < 0.1 the concentration of B immediately shoots up to 1.5 and then slowly comes back down , while CA drops off immediately and falls to zero . This is because the first reaction is very fast and the second reaction is slower with no reverse reactions. When k2 = 1 then the concentration of B spikes again and remains high, while very little of C is formed. This is because after B is formed it will not further get converted to C because the reverse reaction is fast. When k-2 = 0.25 , B shoots up , but does not stay as high because for the second reaction in the reverse direction is a slightly slower than seen before , but still faster than the reaction in the forward direction. P8-11 (a) Intermediates (primary K-phthalates) are formed from the dissociation of K-benzoate with a CdCl2 catalyst reacted with K-terephthalate in an autocatalytic reaction step: A k1 R S C AO P RT R k2 Series S k3 2S 110kPa kPa.dm3 8.314 683K mol.K Autocatalytic 0.02mol / dm3 Maximum in R occurs at t = 880 sec. See Polymath program P8-11-a.pol. POLYMATH Results Variable t A initial value 0 0.02 minimal value 0 0.003958 maximal value 1500 0.02 8-33 final value 1500 0.003958 R S k1 k2 k3 0.00159 0 0 0.00108 0.00119 0.00159 0.00159 0 0 0.00108 0.00119 0.00159 0.0069892 0.0100382 0.00108 0.00119 0.005868 0.0100382 0.00108 0.00119 ODE Report (RKF45) Differential equations as entered by the user [1] d(A)/d(t) = -k1*A [2] d(R)/d(t) = (k1*A)-(k2*R)-(k3*R*S) [3] d(S)/d(t) = (k2*R)-(k3*R*S) Explicit equations as entered by the user [1] k1 = 1.08e-3 [2] k2 = 1.19e-3 [3] k3 = 1.59e-3 P8-11 (b) 1) T = 703 K CAO = 0.019 mol/dm3 k1' k1' k1 exp E1 1 R T 1 T' (1.08 10 3 s 1 ) exp (42600cal / mol ) 1 (1.987cal / mol.K ) 683K 1 703K 2.64 10 3 s 1 Similarly, k2' 3.3 10 3 s 1 And, k3' 3.1 10 3 dm3 / mol.s Maxima in R occurs at around t =320 sec. See Polymath program P8-11-b1.pol. POLYMATH Results Calculated values of the DEQ variables Variable t A R S k1 k2 k3 initial value 0 0.019 0 0 0.00264 0.0033 0.0031 minimal value 0 3.622E-04 0 0 0.00264 0.0033 0.0031 maximal value 1500 0.019 0.0062169 0.0174625 0.00264 0.0033 0.0031 8-34 final value 1500 3.622E-04 8.856E-04 0.0174625 0.00264 0.0033 0.0031 ODE Report (RKF45) Differential equations as entered by the user [1] d(A)/d(t) = -k1*A [2] d(R)/d(t) = (k1*A)-(k2*R)-(k3*R*S) [3] d(S)/d(t) = (k2*R)-(k3*R*S) Explicit equations as entered by the user [1] k1 = 2.64e-3 [2] k2 = 3.3e-3 [3] k3 = 3.1e-3 2) T = 663 K CAO = 0.19 mol/dm3 (42600cal / mol ) 1 (1.987cal / mol.K ) 683K k1' (1.08 10 3 s 1 ) exp k2' 0.4 10 3 s 1 k3' 0.78 10 3 dm3 / mol.s 1 663K 0.42 10 3 s 1 See Polymath program P8-11-b2.pol. POLYMATH Results Calculated values of the DEQ variables Variable t A R S k1 k2 k3 initial value 0 0.019 0 0 4.2E-04 4.0E-04 7.8E-04 minimal value 0 2.849E-04 0 0 4.2E-04 4.0E-04 7.8E-04 maximal value 10000 0.019 0.0071414 0.016889 4.2E-04 4.0E-04 7.8E-04 final value 10000 2.849E-04 0.0012573 0.016889 4.2E-04 4.0E-04 7.8E-04 ODE Report (RKF45) Differential equations as entered by the user [1] d(A)/d(t) = -k1*A [2] d(R)/d(t) = (k1*A)-(k2*R)-(k3*R*S) [3] d(S)/d(t) = (k2*R)-(k3*R*S) Explicit equations as entered by the user [1] k1 = 0.42e-3 [2] k2 = 0.4e-3 [3] k3 = 0.78e-3 Independent variable variable name : t initial value : 0 final value : 10000 Maxima in R occurs around t = 2500 sec. P8-11 (c) Use the Polymath program from part (a) and change the limits of integration to 0 to 1200. We get: CAexit = 0.0055 mol/dm3 CRexit = 0.0066 mol/dm3 8-35 CSexit = 0.0078 mol/dm3 P8-12 (a) P8-12 (b) P8-12 (c) P8-12 (d) P8-12 (e) P8-12 (f) P8-12 (g) P8-12 (h) Mole balance: C AO CA rA CC rC CD rD 8-36 Rate law: Solving in polymath: rA k1 A C A 1 k 2 D C A CC2 3 rC 1 k1 A C A 3 2 k 2 D C A CC2 3 rD k 2 D C A CC2 4 k 3 E CC C D 3 CA 0.0069 M C B k 3 E CC C D 0.96M CC SB/D = rB/rD = 247 SB/C = 1.88 See Polymath program P8-12-h.pol. POLYMATH Results NLES Solution Variable Ca Cb Cc Cd Ce kd ka rb ra ke rc rd re tau Cao Value 0.0068715 0.9620058 0.5097027 0.0038925 0.2380808 3 7 0.0160334 -0.0498855 2 0.008495 6.488E-05 0.003968 60 3 f(x) -2.904E-10 -1.332E-15 -1.67E-08 -2.391E-08 1.728E-08 0.51M C D Ini Guess 3 0 0 0 0 NLES Report (safenewt) Nonlinear equations [1] f(Ca) = Cao-Ca+ra*tau = 0 [2] f(Cb) = Cb - rb*tau = 0 [3] f(Cc) = Cc-rc*tau = 0 [4] f(Cd) = Cd-rd*tau = 0 [5] f(Ce) = Ce - re*tau = 0 Explicit equations [1] kd = 3 [2] ka = 7 [3] rb = ka*Ca/3 [4] ra = -(ka*Ca+kd/3*Ca*Cc^2) [5] ke = 2 [6] rc = ka*Ca/3 - 2/3*kd*Ca*Cc^2 - ke*Cd*Cc [7] rd = kd*Ca*Cc^2 - 4/3*ke*Cd*Cc 8-37 0.004M [8] re = ke*Cd*Cc [9] tau = 60 [10] Cao = 3 P8-12 (i) For PFR and gas phase: dFC dV Mole balance: dFA dV rA dFB rB dV 1 k 2 D C A CC2 3 Rate law: rA k1 A C A rB 1 k1 A C A 3 rC 1 k1 A C A 3 2 k 2 D C A CC2 3 rD k 2 D C A CC2 4 k 3 E CC C D 3 rE k 3E CC C D Stoichiometry: C A CTO FA y FT FT FA FB dy dV FT 2 y FTO FC rC dFD dV rD CD CTO dFE dV K 3 E CC C D CC CTO FD FE FC y FT FD y FT Plot of CB and CC are overlapping. See Polymath program P8-12-i.pol. POLYMATH Results Calculated values of the DEQ variables Variable V Fa Fb Fc Fd Fe y Ft Cto Cc ka kd ke Ca initial value 0 20 0 0 0 0 1 20 0.2 0 7 3 2 0.2 minimal value 0 9.147E-04 0 0 0 0 0.9964621 13.330407 0.2 0 7 3 2 1.367E-05 maximal value 100 20 6.6638171 6.6442656 0.0201258 0.0043322 1 20 0.2 0.0993605 7 3 2 0.2 8-38 final value 100 9.147E-04 6.6638171 6.6442167 0.0171261 0.0043322 0.9964621 13.330407 0.2 0.0993325 7 3 2 1.367E-05 rE rb ra Cd Fto rc rd re alfa X 0.4666667 -1.4 0 20 0.4666667 0 0 1.0E-04 0 3.191E-05 -1.4 0 20 -1.923E-05 -7.012E-05 0 1.0E-04 0 0.4666667 -9.586E-05 3.0E-04 20 0.4666667 8.653E-04 5.908E-05 1.0E-04 0.9999543 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(V) = ra [2] d(Fb)/d(V) = rb [3] d(Fc)/d(V) = rc [4] d(Fd)/d(V) = rd [5] d(Fe)/d(V) = re [6] d(y)/d(V) = -alfa*Ft/(2*y*Fto) Explicit equations as entered by the user [1] Ft = Fa+Fb+Fc+Fd+Fe [2] Cto = 0.2 [3] Cc = Cto*Fc/Ft*y [4] ka = 7 [5] kd = 3 [6] ke = 2 [7] Ca = Cto*Fa/Ft*y [8] rb = ka*Ca/3 [9] ra = -(ka*Ca+kd/3*Ca*Cc^2) [10] Cd = Cto*Fd/Ft*y [11] Fto = 0.2*100 [12] rc = ka*Ca/3 - 2/3*kd*Ca*Cc^2 - ke*Cd*Cc [13] rd = kd*Ca*Cc^2 - 4/3*ke*Cd*Cc [14] re = ke*Cd*Cc [15] alfa = 0.0001 [16] X = 1-Fa/20 8-39 3.191E-05 -9.586E-05 2.56E-04 20 -1.923E-05 -6.742E-05 5.087E-05 1.0E-04 0.9999543 P8-12 (j) Changes in equation from part (i): dFC dV rC RC RC k diffuse C C k diffuse 2 min 1 See Polymath program P8-12-j.pol. P8-13(a) 8-40 See Polymath program P8-13-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 1.5 0.3100061 1.5 0.3100061 2 Cb 2. 0.3384816 2. 0.3384816 3 Cc 0 0 0.1970387 0.105508 4 Cd 0 0 0.6751281 0.6516263 5 Ce 0 0 0.1801018 0.1801018 6 Cf 0 0 0.3621412 0.3621412 7 kd1 0.25 0.25 0.25 0.25 8 ke2 0.1 0.1 0.1 0.1 9 kf3 5. 5. 5. 5. 10 ra -1.5 -1.5 -0.0694818 -0.0694818 11 rb -3. -3. -0.0365984 -0.0365984 12 rc 1.5 -0.0490138 1.5 -0.0085994 13 rd 1.5 -0.0128609 1.5 -0.0126825 14 rd1 1.5 0.0088793 1.5 0.0088793 15 re 0 0 0.0523329 0.0202008 16 re2 0 0 0.0523329 0.0202008 17 rf 0 0 0.2571468 0.0188398 18 rf3 0 0 0.2571468 0.0188398 19 V 0 0 50. 50. 20 vo 10. 10. 10. 10. Differential equations 1 d(Ca)/d(V) = ra/vo 2 d(Cb)/d(V) = rb/vo 3 d(Cc)/d(V) = rc/vo 4 d(Cd)/d(V) = rd/vo 5 d(Ce)/d(V) = re/vo 6 d(Cf)/d(V) = rf/vo Explicit equations 1 vo = 10 2 kf3 = 5 8-41 3 ke2 = .1 4 kd1 = 0.25 5 rf3 = kf3*Cb*Cc^2 6 rd1 = kd1*Ca*Cb^2 7 re2 = ke2*Ca*Cd 8 rf = rf3 9 re = re2 10 rd = rd1-2*re2+rf3 11 ra = -rd1-3*re2 12 rb = -2*rd1-rf3 13 rc = rd1+re2-2*rf3 P8-13 (b) 8-42 P8-13 (c) 8-43 8-44 8-45 P8-13 (d) As θB increases the outlet concentration of species D and F increase, while the outlet concentrations of species A, C, and E decrease. When θB is large, reactions 1 and 3 are favored and when it is small the rate of reaction 2 will increase. P8-13 (e) When the appropriate changes to the Polymath code from part (a) are made we get the following. POLYMATH Results Calculated values of the DEQ variables Variable V Fa Fb Fc Fd Fe Ff vo Ft Cto kd1 ke2 kf3 Cc Cd initial value 0 20 20 0 0 0 0 100 40 0.4 0.25 0.1 5 0 0 minimal value 0 18.946536 18.145647 0 0 0 0 100 38.931546 0.4 0.25 0.1 5 0 0 maximal value 500 20 20 0.9342961 0.8454829 0.0445942 0.0149897 100 40 0.4 0.25 0.1 5 0.0095994 0.0086869 8-46 final value 500 18.946536 18.145647 0.9342961 0.8454829 0.0445942 0.0149897 100 38.931546 0.4 0.25 0.1 5 0.0095994 0.0086869 Cb Ca rd1 re2 rf3 re rf rd ra rb rc Scd Sef 0.2 0.2 0.002 0 0 0 0 0.002 -0.002 -0.004 0.002 1 0 0.1864364 0.1946651 0.0016916 0 0 0 0 0.0014393 -0.0021989 -0.004 0.0016889 1 0 0.2 0.2 0.002 1.691E-04 8.59E-05 1.691E-04 8.59E-05 0.002 -0.002 -0.003469 0.002 1.1734311 83.266916 ODE Report (RKF45) Differential equations as entered by the user [1] d(Fa)/d(V) = ra [2] d(Fb)/d(V) = rb [3] d(Fc)/d(V) = rc [4] d(Fd)/d(V) = rd [5] d(Fe)/d(V) = re [6] d(Ff)/d(V) = rf Explicit equations as entered by the user [1] vo = 100 [2] Ft = Fa+Fb+Fc+Fd+Fe+Ff [3] Cto = .4 [4] kd1 = 0.25 [5] ke2 = .1 [6] kf3 = 5 [7] Cc = Cto*Fc/Ft [8] Cd = Cto*Fd/Ft [9] Cb = Cto*Fb/Ft [10] Ca = Cto*Fa/Ft [11] rd1 = kd1*Ca*Cb^2 [12] re2 = ke2*Ca*Cd [13] rf3 = kf3*Cb*Cc^2 [14] re = re2 [15] rf = rf3 [16] rd = rd1-2*re2+rf3 [17] ra = -rd1-3*re2 [18] rb = -2*rd1-rf3 [19] rc = rd1+re2-2*rf3 [20] Scd = rc/(rd+.0000000001) [21] Sef = re/(rf+.00000000001) 8-47 0.1864364 0.1946651 0.0016916 1.691E-04 8.59E-05 1.691E-04 8.59E-05 0.0014393 -0.0021989 -0.003469 0.0016889 1.1734311 1.9686327 P8-13 (f) The only change from part (e) is: dFD dV rD kcD CD dFB dV rB FB 0 where VT = 500 dm3 and FB0 = 20 mol/min VT P8-13 (g) The only change from part (e) is: 8-48 P8-14 (a) Equations: Rate law: -rA = k1CACB1/2 + k2CA2 rB = rA rC= k1CACB1/2 - k3CC + k4CD rD = k2CA2 – k4CD rE = k3CC rG = k3CC rG = k4CD Mole Balance: See polymath problem P8-14-a.pol Maximum values can be found out from this table : Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 8-49 1 Ca 0.098 0.0064314 0.098 0.0064314 2 Cb 0.049 0.0032157 0.049 0.0032157 3 Cc 0 0 0.0138769 0.0004265 4 Cd 0 0 0.0001148 6.459E-07 5 Ce 0 0 0.0642751 0.0642751 6 Cg 0 0 0.0083756 0.0083756 7 Cto 0.147 0.147 0.147 0.147 8 Cw 0 0 0.0642751 0.0642751 9 Fa 10. 0.9041349 10. 0.9041349 10 Fb 5. 0.4520674 5. 0.4520674 11 Fc 0 0 1.463177 0.0599575 12 Fd 0 0 0.0116183 9.08E-05 13 Fe 0 0 9.035817 9.035817 14 Fg 0 0 1.177438 1.177438 15 Ft 15. 14.87618 20.66532 20.66532 16 Fw 0 0 9.035817 9.035817 17 k1 0.014 0.014 0.014 0.014 18 k2 0.007 0.007 0.007 0.007 19 k3 0.014 0.014 0.014 0.014 20 k4 0.45 0.45 0.45 0.45 21 ra -0.0003709 -0.0003709 -5.395E-06 -5.395E-06 22 rb -0.0001855 -0.0001855 -2.698E-06 -2.698E-06 23 rc 0.0003037 -3.328E-05 0.0003037 -5.744E-07 24 rd 6.723E-05 -8.355E-07 6.723E-05 -1.1E-09 25 re 0 0 0.0001943 5.971E-06 26 rg 0 0 5.166E-05 2.906E-07 27 rw 0 0 0.0001943 5.971E-06 28 Sae 0 0 25.89133 0.1000612 29 Scd 0 0 660.3424 660.3424 30 Sdg 0 0 0.0501992 7.711E-05 31 V 0 0 2.0E+05 2.0E+05 32 Yc 0 0 0.2299208 0.0663148 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(Fe)/d(V) = re 8-50 6 d(Fw)/d(V) = rw 7 d(Fg)/d(V) = rg Explicit equations 1 Cto = 0.147 2 k1 = 0.014 3 Ft = Fa+Fb+Fc+Fd+Fe+Fw+Fg 4 k2 = 0.007 5 Cb = Cto*(Fb/Ft) 6 k3 = 0.014 7 k4 = 0.45 8 Ca = Cto*(Fa/Ft) 9 Cc = Cto*(Fc/Ft) 10 ra = -(k1*Ca*(Cb)^0.5 + k2*(Ca)^2) 11 rb = ra/2 12 re = k3*Cc 13 Cd = Cto*(Fd/Ft) 14 Ce = Cto*(Fe/Ft) 15 Cg = Cto*(Fg/Ft) 16 Cw = Cto*(Fw/Ft) 17 rg = k4*Cd 18 rw = k3*Cc 19 rd = k2*(Ca)^2-k4*Cd 20 rc = k1*Ca*(Cb)^0.5 - k3*Cc+k4*Cd 21 Yc = Fc/Fa 22 Scd = if (V>0.0001)then (Fc/Fd) else (0) 23 Sae = if (V>0.0001)then (Fa/Fe) else (0) 24 Sdg = if (V>0.0001)then (Fd/Fg) else (0) 8-51 8-52 8-53 8-54 P8-14(b) Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 0.098 0.0951293 0.098 0.0951293 2 Cb 0.049 0.0475647 0.049 0.0475647 3 Cc 0 0 0.0032152 0.0032152 4 Cd 0 0 0.0001412 0.0001411 5 Ce 0 0 0.0002229 0.0002229 6 Cg 0 0 0.0005038 0.0005038 7 Cto 0.147 0.147 0.147 0.147 8 Cw 0 0 0.0002229 0.0002229 9 Fa 10. 9.63739 10. 9.63739 10 Fb 5. 4.818695 5. 4.818695 11 Fc 0 0 0.3257277 0.3257277 12 Fd 0 0 0.0143026 0.014299 13 Fe 0 0 0.0225834 0.0225834 14 Fg 0 0 0.0510394 0.0510394 15 Ft 15. 14.89232 15. 14.89232 16 Fw 0 0 0.0225834 0.0225834 17 k1 0.014 0.014 0.014 0.014 18 k2 0.007 0.007 0.007 0.007 19 k3 0.014 0.014 0.014 0.014 20 k4 0.45 0.45 0.45 0.45 21 ra -0.0003709 -0.0003709 -0.0003538 -0.0003538 22 rb -0.0001855 -0.0001855 -0.0001769 -0.0001769 23 rc 0.0003037 0.0003037 0.000336 0.000309 8-55 24 rd 6.723E-05 -1.674E-07 6.723E-05 -1.674E-07 25 re 0 0 4.501E-05 4.501E-05 26 rg 0 0 6.352E-05 6.351E-05 27 rw 0 0 4.501E-05 4.501E-05 28 Sae 0 0 7.875E+05 426.7466 29 Scd 0 0 22.77975 22.77975 30 Sce 0 0 594.3536 14.42332 31 Sdg 0 0 18.10358 0.2801563 32 V 0 0 1000. 1000. 33 Yc 0 0 0.0337983 0.0337983 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(Fe)/d(V) = re 6 d(Fw)/d(V) = rw 7 d(Fg)/d(V) = rg Explicit equations 1 Cto = 0.147 2 k1 = 0.014 3 Ft = Fa+Fb+Fc+Fd+Fe+Fw+Fg 4 k2 = 0.007 5 Cb = Cto*(Fb/Ft) 6 k3 = 0.014 7 k4 = 0.45 8 Ca = Cto*(Fa/Ft) 9 Cc = Cto*(Fc/Ft) 10 ra = -(k1*Ca*(Cb)^0.5 + k2*(Ca)^2) 11 rb = ra/2 12 re = k3*Cc 13 Cd = Cto*(Fd/Ft) 14 Ce = Cto*(Fe/Ft) 15 Cg = Cto*(Fg/Ft) 16 Cw = Cto*(Fw/Ft) 17 rg = k4*Cd 18 rw = k3*Cc 8-56 19 rd = k2*(Ca)^2-k4*Cd 20 rc = k1*Ca*(Cb)^0.5 - k3*Cc+k4*Cd 21 Yc = Fc/Fa 22 Scd = if (V>0.0001)then (Fc/Fd) else (0) 23 Sae = if (V>0.0001)then (Fa/Fe) else (0) 24 Sdg = if (V>0.0001)then (Fd/Fg) else (0) 25 Sce = if (V>0.0001)then (Fc/Fe) else (0) Then taking different values of FA0 and FB0, we find the following data: FA0 FB0 Θ= FA0/FB0 YC SC/E 0.01 1 5 10 100 1000 5 5 5 5 5 5 SD/G SC/D 0.002 0.2 1 2 20 200 0.139038 4.424789 0.070678 3.48E+04 0.111343 5.379092 0.088876 321.5455 0.057955 9.342066 0.168248 52.61217 0.033798 14.42332 0.280156 22.77975 0.001968 107.1563 2.87001 1.931864 5.99E-05 1001.268 30.05269 0.413009 50 100 150 200 250 0.16 0.14 0.12 0.1 0.08 Yc 0.06 0.04 0.02 0 -50 -0.02 0 ΘO2 8-57 1200 1000 800 SC/E 600 400 200 0 -50 0 50 100 150 200 250 150 200 250 ΘO2 35 30 25 20 SD/G 15 10 5 0 -50 -5 0 50 100 ΘO2 8-58 25 20 15 SD/G 10 5 0 -500 0 500 -5 1000 1500 2000 2500 ΘO2 P8-14(c) Now we have a pressure drop parameter α = 0.002, so we modify our polymath program as follows: Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 0.002 0.002 0.002 0.002 2 Ca 0.098 0.0041647 0.098 0.0041647 3 Cb 0.049 0.0020823 0.049 0.0020823 4 Cc 0 0 0.0004581 3.917E-05 5 Cd 0 0 5.56E-05 3.278E-06 6 Ce 0 0 8.655E-06 9.533E-07 7 Cg 0 0 3.75E-05 3.755E-06 8 Cto 0.147 0.147 0.147 0.147 9 Cw 0 0 8.655E-06 9.533E-07 10 Fa 10. 9.896873 10. 9.896873 11 Fb 5. 4.948437 5. 4.948437 12 Fc 0 0 0.0930717 0.0930717 13 Fd 0 0 0.0082669 0.0077896 14 Fe 0 0 0.0022655 0.0022655 15 Fg 0 0 0.0089238 0.0089238 16 Ft 15. 14.95962 15. 14.95963 17 Ft0 15. 15. 15. 15. 18 Fw 0 0 0.0022655 0.0022655 19 k1 0.014 0.014 0.014 0.014 20 k2 0.007 0.007 0.007 0.007 21 k3 0.014 0.014 0.014 0.014 8-59 22 k4 0.45 0.45 0.45 0.45 23 ra -0.0003709 -0.0003709 -2.782E-06 -2.782E-06 24 rb -0.0001855 -0.0001855 -1.391E-06 -1.391E-06 25 rc 0.0003037 3.587E-06 0.0003037 3.587E-06 26 rd 6.723E-05 -4.638E-06 6.723E-05 -1.354E-06 27 re 0 0 6.413E-06 5.483E-07 28 rg 0 0 2.502E-05 1.475E-06 29 rw 0 0 6.413E-06 5.483E-07 30 Sae 0 0 3.344E+06 4368.521 31 Scd 0 0 11.94813 11.94813 32 Sce 0 0 1218.255 41.08224 33 Sdg 0 0 37.46977 0.8729093 34 V 0 0 500. 500. 35 y 1. 0.0428242 1. 0.0428242 36 Yc 0 0 0.0094042 0.0094042 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(Fe)/d(V) = re 6 d(Fw)/d(V) = rw 7 d(Fg)/d(V) = rg 8 d(y)/d(V) = -alpha/2/y*(Ft/Ft0) Explicit equations 1 alpha = 0.002 2 Ft0 = 15 3 Cto = 0.147 4 k1 = 0.014 5 Ft = Fa+Fb+Fc+Fd+Fe+Fw+Fg 6 k2 = 0.007 7 Cb = Cto*(Fb/Ft)*y 8 k3 = 0.014 9 k4 = 0.45 10 Ca = Cto*(Fa/Ft)*y 11 Cc = Cto*(Fc/Ft)*y 12 ra = -(k1*Ca*(Cb)^0.5 + k2*(Ca)^2) 8-60 13 rb = ra/2 14 re = k3*Cc 15 Cd = Cto*(Fd/Ft)*y 16 Ce = Cto*(Fe/Ft)*y 17 Cg = Cto*(Fg/Ft)*y 18 Cw = Cto*(Fw/Ft)*y 19 rg = k4*Cd 20 rw = k3*Cc 21 rd = k2*(Ca)^2-k4*Cd 22 rc = k1*Ca*(Cb)^0.5 - k3*Cc+k4*Cd 23 Yc = Fc/Fa 24 Scd = if (V>0.0001)then (Fc/Fd) else (0) 25 Sae = if (V>0.0001)then (Fa/Fe) else (0) 26 Sdg = if (V>0.0001)then (Fd/Fg) else (0) 27 Sce = if (V>0.0001)then (Fc/Fe) else (0) 8-61 8-62 8-63 P8-14(d) Since C(Formic acid) is our desired product, so temperature corresponding to the maximum yield of C should be recommended. 8-64 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 0.098 3.689E-08 0.098 3.689E-08 2 Cb 0.049 1.844E-08 0.049 1.844E-08 3 Cc 0 0 0.0150519 1.497E-12 4 Cd 0 0 0.0089776 1.018E-10 5 Ce 0 0 0.0496431 0.0496431 6 Cg 0 0 0.0477138 0.0477138 7 Cto 0.147 0.147 0.147 0.147 8 Cw 0 0 0.0496431 0.0496431 9 Fa 10. 7.43E-06 10. 7.43E-06 10 Fb 5. 3.715E-06 5. 3.715E-06 11 Fc 0 0 1.854 3.016E-10 12 Fd 0 0 1.030757 2.05E-08 13 Fe 0 0 9.999993 9.999993 14 Fg 0 0 9.611354 9.611354 15 Ft 15. 14.91758 29.61135 29.61135 16 Fw 0 0 9.999993 9.999993 17 k1 0.014 0.014 30.64368 30.64368 18 k10 0.014 0.014 0.014 0.014 19 k2 0.007 0.007 7.341E+07 7.341E+07 20 k20 0.007 0.007 0.007 0.007 21 k3 0.014 0.014 6.707E+04 6.707E+04 22 k30 0.014 0.014 0.014 0.014 23 k4 0.45 0.45 984.9755 984.9755 24 k40 0.45 0.45 0.45 0.45 25 ra -0.0003709 -0.0625305 -1.0E-07 -1.0E-07 26 rb -0.0001855 -0.0312653 -5.002E-08 -5.002E-08 27 rc 0.0003037 -0.0238556 0.0236439 -5.93E-12 28 rd 6.723E-05 -0.0093009 0.0120515 -3.804E-10 29 re 0 0 0.0773459 1.004E-07 30 rg 0 0 0.0627128 1.003E-07 31 rw 0 0 0.0773459 1.004E-07 32 Sae 0 0 5.205E+05 7.43E-07 33 Scd 0 0 3.394658 0.0147083 34 Sdg 0 0 18.42613 2.133E-09 35 T 300. 300. 550. 550. 36 V 0 0 1000. 1000. 37 Yc 0 0 0.4483122 4.059E-05 8-65 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(Fe)/d(V) = re 6 d(Fw)/d(V) = rw 7 d(Fg)/d(V) = rg 8 d(T)/d(V) = 0.25 Explicit equations 1 k20 = 0.007 2 k10 = 0.014 3 k1 = k10*exp((10000/1.97)*(1/300-1/T)) 4 k2 = k20*exp((30000/1.97)*(1/300-1/T)) 5 k30 = 0.014 6 k3 = k30*exp((20000/1.97)*(1/300-1/T)) 7 k40 = 0.45 8 Ft = Fa+Fb+Fc+Fd+Fe+Fw+Fg 9 Cto = 0.147 10 Ca = Cto*(Fa/Ft) 11 Cb = Cto*(Fb/Ft) 12 Cc = Cto*(Fc/Ft) 13 Cd = Cto*(Fd/Ft) 14 Ce = Cto*(Fe/Ft) 15 Cg = Cto*(Fg/Ft) 16 ra = -(k1*Ca*(Cb)^0.5 + k2*(Ca)^2) 17 rb = ra/2 18 re = k3*Cc 19 k4 = k40*exp((10000/1.97)*(1/300-1/T)) 20 Cw = Cto*(Fw/Ft) 21 rg = k4*Cd 22 rw = k3*Cc 23 rd = k2*(Ca)^2-k4*Cd 24 rc = k1*Ca*(Cb)^0.5 - k3*Cc+k4*Cd 25 Yc = Fc/Fa 26 Scd = if (V>0.0001)then (Fc/Fd) else (0) 27 Sae = if (V>0.0001)then (Fa/Fe) else (0) 8-66 28 Sdg = if (V>0.0001)then (Fd/Fg) else (0) Temperature corresponding to maximum yield = 367.8 K P8-15 (1) C2H4 + 1/2O2 → C2H4O E + 1/2O → D (2) E C2H4 + 3O2 → 2CO2 + 2H2O + 3O → 2U1 + 2U2 8-67 FIO 0.82 FTO 0.007626 P8-15 (a) Selectivity of D over CO2 S FD FU 1 See Polymath program P8-15-a.pol. POLYMATH Results Variable W Fe Fo Fd Fu1 Fu2 Finert Ft K1 K2 Pto Pe Po k1 k2 X S r1e r2e initial value 0 5.58E-04 0.001116 0 1.0E-07 0 0.007626 0.0093001 6.5 4.33 2 0.1199987 0.2399974 0.15 0.088 0 0 -0.0024829 -0.0029803 minimal value 0 1.752E-10 4.066E-05 0 1.0E-07 0 0.007626 0.0091804 6.5 4.33 2 3.817E-08 0.008858 0.15 0.088 0 0 -0.0024829 -0.0029803 maximal value 2 5.58E-04 0.001116 2.395E-04 6.372E-04 6.371E-04 0.007626 0.0093001 6.5 4.33 2 0.1199987 0.2399974 0.15 0.088 0.9999997 0.4101512 -3.692E-10 -8.136E-10 Differential equations as entered by the user [1] d(Fe)/d(W) = r1e+r2e [2] d(Fo)/d(W) = 1/2*r1e + 3*r2e [3] d(Fd)/d(W) = -r1e [4] d(Fu1)/d(W) = -2*r2e [5] d(Fu2)/d(W) = -2*r2e Explicit equations as entered by the user [1] Finert = 0.007626 [2] Ft = Fe+Fo+Fd+Fu1+Fu2+Finert [3] K1 = 6.5 [4] K2 = 4.33 [5] Pto = 2 [6] Pe = Pto*Fe/Ft [7] Po = (Pto*Fo/Ft) [8] k1 = 0.15 [9] k2 = 0.088 [10] X = 1 - Fe/0.000558 [11] S = Fd/Fu1 [12] r1e = -k1*Pe*Po^0.58/(1+K1*Pe)^2 [13] r2e = -k2*Pe*Po^0.3/(1+K2*Pe)^2 8-68 final value 2 1.752E-10 4.066E-05 2.395E-04 6.372E-04 6.371E-04 0.007626 0.0091804 6.5 4.33 2 3.817E-08 0.008858 0.15 0.088 0.9999997 0.3758225 -3.692E-10 -8.136E-10 X = 0.999 and S = 0.376(mol of ethylene oxide)/(mole of carbon dioxide) P8-15(b) Changes in equation from part (a): dFO dW RO 1 r1E 3r 2 E RO and FO o 2 0.12 0.0093 0.001116 mol W 2 kg.s From Polymath program: 0 X = 0.71 S = 0.04 (mol of ethylene oxide)/(mole of carbon dioxide) P8-15 (c) Changes in equation from part (a): dFE dW r1E r 2 E RE and FE o RE 0.06 0.0093 W 0.000558 mol 2 kg.s From Polymath program: 0 X = 0.96 S = 0.41(mol of ethylene oxide)/(mole of carbon dioxide) P8-15 (d) No solution will be given. P8-16 The reactions are 1. C + W 6 H2 + 6CO 2. L + W 13 H2 + 10 CO Rate laws are : - r1C = k1C CC CW -r2L = k2L CL Cw2 CT0 = P0/RT = ( 1 atm )/(0.082)(1473) = 0.00828 mol/dm3 FC0 = 0.00411 mol/s FL0 = 0.0185 mol/s FW0 = 0.02 mol/s P8-16 (a) See polymath program P 8-16(a) Calculated values of DEQ variables 8-69 Variable Initial value Minimal value Maximal value Final value 1 ConvC 0 0 0.8337198 0.8337198 2 ConvL 0 0 0.7379696 0.7379696 3 Ct0 0.0082791 0.0082791 0.0082791 0.0082791 4 Fc 0.0041152 0.0006843 0.0041152 0.0006843 5 Fc0 0.0041152 0.0041152 0.0041152 0.0041152 6 Fco 0 0 0.0342518 0.0342518 7 Fh 0 0 0.0383516 0.0383516 8 Fl 0.0018519 0.0004852 0.0018519 0.0004852 9 Fl0 0.0018519 0.0018519 0.0018519 0.0018519 10 Ft 0.0259671 0.0259671 0.0807757 0.0807757 11 Fw 0.02 0.0070028 0.02 0.0070028 12 k1c 3.0E+04 3.0E+04 3.0E+04 3.0E+04 13 k2l 1.4E+07 1.4E+07 1.4E+07 1.4E+07 14 Mc 0.6666673 0.1108536 0.6666673 0.1108536 15 Mco 0 0 0.9590499 0.9590499 16 Mh 0 0 0.0767032 0.0767032 17 Ml 0.333333 0.0873434 0.333333 0.0873434 18 Mw 0.36 0.1260502 0.36 0.1260502 19 P 1. 1. 1. 1. 20 R 0.082 0.082 0.082 0.082 21 r1c -0.2509955 -0.2509955 -0.0015102 -0.0015102 22 r2l -0.3361048 -0.3361048 -0.0003587 -0.0003587 23 T 1473. 1473. 1473. 1473. 24 V 0 0 0.417 0.417 Differential equations 1 d(Fc)/d(V) = r1c 2 d(Fl)/d(V) = r2l 3 d(Fw)/d(V) = r1c+7*r2l 4 d(Fh)/d(V) = -6*r1c-13*r2l 5 d(Fco)/d(V) = -6*r1c-10*r2l Explicit equations 1 T = 1473 2 R = 0.082 3 P=1 4 k2l = 14000000 5 k1c = 30000 8-70 6 Ft = Fc+Fl+Fw+Fh+Fco 7 Ct0 = P/(R*T) 8 Fc0 = 0.00411523 9 Fl0 = 0.00185185 10 Mc = Fc*162 11 Ml = Fl*180 12 Mh = Fh*2 13 Mco = Fco*28 14 Mw = Fw*18 15 r1c = -k1c*(Ct0*(Fc)/(Ft))*(Ct0*(Fw)/(Ft)) 16 r2l = -k2l*(Ct0*(Fl)/(Ft))*((Ct0*(Fw)/(Ft))^2) 17 ConvC = (Fc0-Fc)/Fc0 18 ConvL = (Fl0-Fl)/Fl0 Plot of Fc vs V 8-71 Plot of Fl vs V Plot of Fw vs V 8-72 Plot of Fh vs V plot of Fco vs V (b) W is the key reactant YC = (-dCC/-dCW) = -r1C/(-r1C -7*r2L) 8-73 The modification is made in the polymath code for Prob 8.16(a) The plot of YC versus V is as follows ; For poltting YW versus volume ; since W is our key reactant then, Yw = -dW/(-dW) = 1 Now YL = -dL/(-dW) = -r2L/(-r1C – 7*r2L) The plot is as follows : 8-74 Overall selectivity SCO / H 2 = NCO = exit molar flow rate of CO/exit molar flow rate of H2 = N H2 CCO |exit /CH2 | exit at any point in the reactor. P8-16 (c) Individualized solution P8-17 (a) The reactions are (i) L + 3 W 3 H2 + 3 CO + char (ii) Ch + 4 W 10 H2 + 7CO 8-75 rate laws at 1200 0C are : -r1L = k1LCLCw2 -r2CH = k2ChCchCw2 ; k1L = 3721 (dm3/mol)2/sec ; k2CH = 1000 ( dm3/mol)2/sec Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 ConL 0 0 0.99 0.99 2 Ct0 0.2 0.2 0.2 0.2 3 Fch 0 0 0.0076175 0.0047293 4 Fco 0 0 0.089117 0.089117 5 Fh 0 0 0.1115957 0.1115957 6 Fl 0.0123457 0.0001235 0.0123457 0.0001235 7 Fl0 0.0123457 0.0123457 0.0123457 0.0123457 8 Ft 0.1240226 0.1240226 0.2506041 0.2506041 9 Fw 0.1116769 0.0450387 0.1116769 0.0450387 10 k1l 3721.73 3721.73 3721.73 3721.73 11 k2ch 1000. 1000. 1000. 1000. 12 r1l -2.403113 -2.403113 -0.0004738 -0.0004738 13 r2ch 0 -0.0992252 0 -0.0048763 14 V 0 0 0.417002 0.417002 Differential equations 1 d(Fl)/d(V) = r1l 2 d(Fch)/d(V) = r2ch-r1l 3 d(Fw)/d(V) = 3*r1l+4*r2ch 4 d(Fh)/d(V) = -3*r1l-10*r2ch 5 d(Fco)/d(V) = -3*r1l-7*r2ch Explicit equations 1 k2ch = 1000 2 k1l = 3721.73 3 Ft = Fch+Fl+Fw+Fh+Fco 4 Ct0 = 0.2 5 r1l = -k1l*(Ct0*(Fl)/(Ft))*((Ct0*(Fw)/(Ft))^2) 8-76 6 r2ch = -k2ch*(Ct0*(Fch)/(Ft))*((Ct0*(Fw)/(Ft))^2) 7 Fl0 = 0.012345679 8 ConL = (Fl0-Fl)/(Fl0) 8-77 P8-17 (b) (c) SCO/Ch Let S1 = S~CO/Ch = Fco/Fch The plot is as follows- 8-78 Considering W as the principle reacting species; Yw = 1 and Yl = (rl)/(rw) = (r1l)/(3*r1l + 4*r2ch) the plot is as follows: (d) The molar flow rate for char is maximum at about V= 0.02085 dm3. 8-79 P8-18 (a) Isothermal gas phase reaction in a membrane reactor packed with catalyst. A r1'C B C k1C C A AD r2' D k2 D C A 2C + D 2E r3' E k3 E CC2 CD C AO P RT CB CC K1C 24.6atm 0.082dm atm / mol.K (500 K ) 3 0.6mol / dm3 Fa(0) = 10 mol/min Fb(0) = Fc(0) = Fd(0) = Fe(0) = 0 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alfa 0.008 0.008 0.008 0.008 2 Ca 0.6 0.0029024 0.6 0.0029024 3 Cb 0 0 0.1525032 0.0075281 4 Cc 0 0 0.1425644 0.0541764 5 Cd 0 0 0.0254033 0.0036956 6 Ce 0 0 0.274725 0.235079 7 Cto 0.6 0.6 0.6 0.6 8 Fa 10. 0.0702103 10. 0.0702103 9 Fb 0 0 3.391481 0.1821054 10 Fc 0 0 3.16936 1.310531 11 Fd 0 0 0.5564071 0.0893965 12 Fe 0 0 5.686575 5.686575 13 Ft 10. 7.338818 12.8179 7.338818 14 Fto 10. 10. 10. 10. 15 k1c 2. 2. 2. 2. 16 K1c 0.2 0.2 0.2 0.2 17 k2d 0.4 0.4 0.4 0.4 18 k3e 400. 400. 400. 400. 8-80 19 kb 1. 1. 1. 1. 20 r1c 1.2 0.0017264 1.2 0.0017264 21 r2d 0.24 0.001161 0.24 0.001161 22 r3e 0 0 0.200243 0.0043387 23 ra -1.44 -1.44 -0.0028874 -0.0028874 24 rb 1.2 0.0017264 1.2 0.0017264 25 rc 1.2 -0.0492057 1.2 -0.0026123 26 rd 0.24 -0.0164816 0.24 -0.0010084 27 re 0 0 0.200243 0.0043387 28 W 0 0 100. 100. 29 y 1. 0.5056359 1. 0.5056359 Differential equations 1 d(Fa)/d(W) = ra 2 d(Fb)/d(W) = rb-(kb*Cb) 3 d(Fc)/d(W) = rc 4 d(Fd)/d(W) = rd 5 d(Fe)/d(W) = re 6 d(y)/d(W) = -alfa*Ft/(2*Fto*y) Explicit equations 1 k2d = 0.4 2 K1c = 0.2 3 Ft = Fa+Fb+Fc+Fd+Fe 4 Cto = 0.6 5 Cb = Cto*(Fb/Ft)*y 6 Ca = Cto*(Fa/Ft)*y 7 Cd = Cto*(Fd/Ft)*y 8 Cc = Cto*(Fc/Ft)*y 9 kb = 1 10 k1c = 2 8-81 11 r2d = k2d*Ca 12 k3e = 400 13 r1c = k1c*(Ca-(Cb*Cc/K1c)) 14 ra = -r1c-r2d 15 r3e = k3e*(Cc^2)*Cd 16 rd = r2d-(r3e/2) 17 rb = r1c 18 rc = r1c-r3e 19 re = r3e 20 Ce = Cto*(Fe/Ft)*y 21 alfa = 0.008 22 Fto = 10 P8-18 (b) Species B, C, D, and E all go though a maximum. The concentration of species are affected by two factors: reaction and pressure drop. We can look at species B for example: Species B: 8-82 Production by reaction 1 => tends to increase concentration of B Pressure drop => tends to decrease concentration of B At W<10, concentration of B rises because the production of B by reaction outweighs the dilution of B by pressure drop. Further down the reactor, the concentration of B drops because the effect of pressure drop outweighs the production of B by reaction. Species E: The reasoning for species E is similar to species B. Species C and D: Species C and D are produced in reactions 1 and 2, respectively. However, species C and D are also reactants in reaction 3; this contributes to their decline at later times (in addition to the pressure drop). P8-18 (c) Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alfa 0.008 0.008 0.008 0.008 2 Ca 0.6 0.0024106 0.6 0.0024106 3 Cb 0 0 0.2447833 0.0593839 4 Cc 0 0 0.1181101 0.0028718 5 Cd 0 0 0.0408517 0.0119119 6 Ce 0 0 0.1034882 0.0252849 7 Cto 0.6 0.6 0.6 0.6 8 Fa 10. 0.2791706 10. 0.2791706 9 Fb 0 0 6.877205 6.877205 10 Fc 0 0 2.623093 0.3325842 11 Fd 0 0 1.379513 1.379513 12 Fe 0 0 2.928221 2.928221 13 Ft 10. 10. 13.00145 11.79669 14 Fto 10. 10. 10. 10. 15 k1c 2. 2. 2. 2. 16 K1c 0.2 0.2 0.2 0.2 8-83 17 k2d 0.4 0.4 0.4 0.4 18 k3e 400. 400. 400. 400. 19 kb 1. 1. 1. 1. 20 r1c 1.2 0.0031158 1.2 0.0031158 21 r2d 0.24 0.0009642 0.24 0.0009642 22 r3e 0 0 0.1548711 3.93E-05 23 ra -1.44 -1.44 -0.0040801 -0.0040801 24 rb 1.2 0.0031158 1.2 0.0031158 25 rc 1.2 0.001223 1.2 0.0030765 26 rd 0.24 0.0009446 0.24 0.0009446 27 re 0 0 0.1548711 3.93E-05 28 W 0 0 100. 100. 29 y 1. 0.169772 1. 0.169772 Differential equations 1 d(Fa)/d(W) = ra 2 d(Fb)/d(W) = rb 3 d(Fc)/d(W) = rc-(kb*Cc) 4 d(Fd)/d(W) = rd 5 d(Fe)/d(W) = re 6 d(y)/d(W) = -alfa*Ft/(2*Fto*y) Explicit equations 1 k2d = 0.4 2 K1c = 0.2 3 Ft = Fa+Fb+Fc+Fd+Fe 4 Cto = 0.6 5 Cb = Cto*(Fb/Ft)*y 6 Ca = Cto*(Fa/Ft)*y 7 Cd = Cto*(Fd/Ft)*y 8 Cc = Cto*(Fc/Ft)*y 8-84 9 kb = 1 10 k1c = 2 11 r2d = k2d*Ca 12 k3e = 400 13 r1c = k1c*(Ca-(Cb*Cc/K1c)) 14 ra = -r1c-r2d 15 r3e = k3e*(Cc^2)*Cd 16 rd = r2d-(r3e/2) 17 rb = r1c 18 rc = r1c-r3e 19 re = r3e 20 Ce = Cto*(Fe/Ft)*y 21 alfa = 0.008 22 Fto = 10 Major Differences: 8-85 (1) When C diffuses out instead of B, the concentration of C is lower and the concentration of B is higher. (2) The concentration of D is higher because reaction 3 is slower (C is a reactant in reaction 3) (3) The concentration of E is lower because of the same reasoning as (2). P8-18 (d) Individualized Solution P8-20 The reactions are : k3 2A A k1 D B C Volume of PFR = 100 dm3 flow rate =υ = 10 dm3/min C0 = 3 mol / m3 K1 = 0.05 min K3 = 0.015 (dm3/mol)/min Kc = 0.5 dm3 /mol The mistakes in the solution are as follows : k1 (i) k1 is the rate constant for the reaction for A B C . But the rate constants for (ii) (iii) the reactions have been reversed. The molar flow rates have not been used when rate laws are written in the code. The rate law expression for various species (A,B,C,D) is incorrect . The mistakes are corrected hereby; The rate laws are written as follows; rC = rB = k1(CA – (1/KC )CCCB) = 0.05 *(CA – CB*CC/0.5) rA = - k3*CA – k1(CA – (1/KC )CCCB) = - 0.05 *(CA – CA*CC/0.5) - 0.015*CA rD = 1/2 *k3*CA = 0.0075 Now for plotting the concentrations with the volume we need the performance equation for PFR; Thus 8-86 -rA *dV = dFA dFA/dV = -rA dCa/dV = -1/υ *rA This being a gaseous reaction the volumetric flow rate will change with volume as we proceed in the PFR, Assuming the extent of reactions to be XA1 and XA2 for the reactions 1 and 2 ; then υ =υ0 *(1 + εA1XA1 +εA2XA2 ) the performance equations will be ; dXa/dV = CA0 * 0 (1 1 A1 X A1 A2 X A2 ) * Ca0*(k 3*(1 Xa) k1((1 Xa) (1/ KC )* B * C *(1 Xa1)*(1 Xa2)) Here , Xa = Xa1 + Xa2 Similarly performance equations for other species in the reactor can be written and the equations will have to be solved simultaneously for getting the plots. 8-87 CDGA8-1 8-88 8-89 8-90 8-91 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. 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All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 9-1 Solutions for Chapter 9 – Reaction Mechanisms, Pathways, Bioreactions and Bioreactors P9-1 Individualized Solution P9-2 (a) Example 9-1 The graph of Io/I will remain same if CS2 concentration changes. If concentration of M increases the slope of line will decrease. P9-2 (b) Example 9-2 The inhibitor shows competitive inhibition. P9-2 (c) Example 9-3 1)Now Curea = 0.001mol/dm3 and t = 10 min = 600 sec. t kM 1 ln VMAX 1 X 600 sec Curea X VMAX 0.0266mol / dm 3 1 ln 3 1 X 0.000266mol / s.dm 0.001mol / dm 3 X 0.000266mol / s.dm 3 Solving, we get X = 0.9974. t 461.7 sec 2) For CSTR, C urea X rurea rurea rurea Curea X 9-2 VMAX Curea K M Curea 0.000266mol / s.dm 3 0.1mol / dm 3 1 X 0.0266mol / dm 3 0.1mol / dm 3 1 X Solving, we get X = 0.675 See Polymath program P9-2-c.pol. POLYMATH Results NLE Solution Variable Value f(x) Ini Guess X 0.6751896 -8.062E-10 0.5 NLE Report (safenewt) Nonlinear equations [1] f(X) = 0.0000266*(1-X)/(0.0266+0.1*(1-X))-0.1*X/461.7 = 0 3) For PFR, CO dC urea r Cures and C urea kM 1 ln VMAX 1 X Curea X VMAX C urea0 1 X Same as batch reactor, but t replaced by X = 0.8 P9-2 (d) Example 9-4 YS / P YP / S YS / C P CS CP 1 238.7 245 5.03 2.14 1 2.18 YS / P 1 YC P / S 2.18 g / g 0.46 g / g 1 0.075 0.46 1.87 g / g Yes there is disparity as substrate is also used in maintenance. P9-2 (e) Example 9-5 See Polymath program P9-2-e.pol. Part (1) Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 24 24 Cc 2.0E-04 1.276E-04 0.002742 0.002742 9-3 0.1mol / dm 3 X 461.7 sec Cs Cp rd Ysc Ypc Ks m umax rsm kobs rg vo Cso Vo V mp 5.0E-04 5.0E-04 4.5794959 4.5794959 0 0 0.0159354 0.0159354 2.0E-06 1.277E-06 2.742E-05 2.742E-05 12.5 12.5 12.5 12.5 5.6 5.6 5.6 5.6 1.7 1.7 1.7 1.7 0.03 0.03 0.03 0.03 0.33 0.33 0.33 0.33 6.0E-06 3.83E-06 8.226E-05 8.226E-05 0.33 0.3299706 0.33 0.3299706 1.941E-08 1.941E-08 6.598E-04 6.598E-04 0.5 0.5 0.5 0.5 5 5 5 5 1 1 1 1 1 1 13 13 0 0 0.20716 0.20716 ODE Report (RKF45) Differential equations as entered by the user [1] d(Cc)/d(t) = rg-rd-vo*Cc/V [2] d(Cs)/d(t) = Ysc*(-rg)-rsm+(Cso-Cs)*vo/V [3] d(Cp)/d(t) = rg*Ypc-vo*Cp/V Explicit equations as entered by the user [1] rd = Cc*.01 [2] Ysc = 1/.08 [3] Ypc = 5.6 [4] Ks = 1.7 [5] m = .03 [6] umax = .33 [7] rsm = m*Cc [8] kobs = (umax*(1-Cp/93)^.52) [9] rg = kobs*Cc*Cs/(Ks+Cs) [10] vo = 0.5 [11] Cso = 5 [12] Vo = 1 [13] V = Vo+vo*t [14] mp = Cp*V Comments [2] d(Cs)/d(t) = Ysc*(-rg)-rsm+(Cso-Cs)*vo/V Cso is concentration of substrate in feed stream, NOT initial concentration of substrate in reactor [17] mp = Cp*V mass of product in grams 9-4 Part (2) Change the cell growth rate law: rg CC C S k obs 2 KS CS CS KI All other equations are the same as in part (1). 9-5 Notice that uncompetitive inhibition by the substrate causes the concentration of cells to decrease with time, whereas without uncompetitive inhibition, the concentration of cells increased with time. Consequently, the concentration of product is very low compared to the case without uncompetitive inhibition. Part (3) Change the observed reaction rate constant: k obs max 1 CP 10000 0.52 All other equations are the same as in part (1). CP Since CP is so small, the factor 1 * CP 0.52 1 whether CP* = 93 g/dm3 or CP* = 10,000 g/dm3. Thus the plots for this part are approximately the same as the plots in part (1). P9-2 (f) Example on CDROM For t = 0 to t = 0.35 sec, PSSH is not valid as steady state not reached. And at low temperature PSSH results show greatest disparity. See Polymath program P9-2-f.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 12 12 C1 0.1 2.109E-04 0.1 2.109E-04 C2 0 0 1.311E-09 1.311E-09 C6 0 0 3.602E-09 3.602E-09 C4 0 0 2.665E-07 1.276E-08 C7 0 0 0.0979179 0.0979179 C3 0 0 0.0012475 0.0012475 9-6 C5 C8 CP5 CP1 k5 T k1 k2 k4 k3 0 0 0.0979179 0.0979179 0 0 6.237E-04 6.237E-04 0 0 0.0979123 0.0979123 0.1 2.166E-04 0.1 2.166E-04 3.98E+09 3.98E+09 3.98E+09 3.98E+09 1000 1000 1000 1000 0.0014964 0.0014964 0.0014964 0.0014964 2.283E+06 2.283E+06 2.283E+06 2.283E+06 9.53E+08 9.53E+08 9.53E+08 9.53E+08 5.71E+04 5.71E+04 5.71E+04 5.71E+04 ODE Report (STIFF) Differential equations as entered by the user [1] d(C1)/d(t) = -k1*C1-k2*C1*C2-k4*C1*C6 [2] d(C2)/d(t) = 2*k1*C1-k2*C1*C2 [3] d(C6)/d(t) = k3*C4-k4*C6*C1 [4] d(C4)/d(t) = k2*C1*C2-k3*C4+k4*C6*C1-k5*C4^2 [5] d(C7)/d(t) = k4*C1*C6 [6] d(C3)/d(t) = k2*C1*C2 [7] d(C5)/d(t) = k3*C4 [8] d(C8)/d(t) = 0.5*k5*C4^2 [9] d(CP5)/d(t) = k3*(2*k1/k5)^0.5*CP1^0.5 [10] d(CP1)/d(t) = -k1*CP1-2*k1*CP1(k3*(2*k1/k5)^0.5)*(CP1^0.5) P9-2 (g) Individualized solution P9-3 Burning: 9-7 9-8 9-9 P9-4 k1 CH 3 CHO CH 3 CH 3 CH 3CHO k2 CHO CH 3CHO k3 2CH 3 rAC k4 r1 r1 CHO CH 3 CO CH 4 r2 k 2 C AC CCH3 CH 3 2CO H 2 r3 k 3CCHO C AC r4 C2 H 6 r2 r3 k1C AC k 2 C AC CCH3 C AC k1 k 2 CCH3 k 3C AC CCHO k 3CCHO Active intermediates: CH 3 , CHO rCHO r1 r3 k1C AC C AC k1 CCHO rCH3 0 k 3C AC CCHO k 3CCHO 0 0 k1 k3 r1 r2 r2 r3 2r4 k1C AC k1C AC k3C AC CCHO 0 2k4CCH3 2 0 Plugging in expression for C CHO : 9-10 k 4 CCH3 2 k1C AC 2k4CCH3 2 k1C AC 0 k1C AC k4 CCH3 Now, substitute expressions for CH 3 and CHO into equation for rAC C AC k1 k 2 CCH3 k 3CCHO C AC k1 k2 k1C AC k4 k1C AC 2 k2 C AC k1k4 k1 P9-4 (b) When k2 C AC k1k4 1, rAC k2 3 k1 C AC 2 k4 3 kC AC 2 9-11 rAC : P9-4 (c) CH3CHO k1 k4 C2H6 CH3• CHO• k2 k3 CH4 CO H2 P9-5 (a) 9-12 P9-5 (b) k1 Cl2 2Cl * k2 k3 Cl * CO COCl * k4 k5 COCl * Cl2 rCOCl* COCl 2 Cl * 0 k3 Cl * CO k4 k5 Cl2 k5 k3 CO Cl * Cl2 k5 COCl * Cl2 rCl k5 COCl * Cl2 k3 Cl * CO COCl * rCOCl2 k4 COCl * 0 k1 Cl2 k2 Cl * k4 k5 Cl2 2 k3 Cl * CO add rCOCl to rCl rCl rCOCl Cl * Cl * 2 0 0 k1 Cl2 k2 Cl 2 k1 Cl2 k2 k1 Cl2 k2 9-13 k4 COCl * k5 COCl * Cl2 k1 k5 k3 CO Cl2 k2 k4 k5 Cl2 rCOCl2 k4 0.5 Cl2 k5 k3 k1 k2 k4 1/ 2 3 CO Cl2 2 k5 Cl2 k5 Cl2 rCOCl2 3 k11/ 2 k3 k5 CO Cl2 2 k21/ 2 k4 P9-5 (c) The proposed mechanism for this reaction is: Through this mechanism, it may be deduced that the net rate of formation of HBr (product) is given by: where the concentrations of the intermediates may be determined by invoking the steady state approximation, i.e.: and: i.e. from (ii) + (i) we obtain: 9-14 i.e.: which substituted back in (i) gives: i.e.: i.e.: or: dividing 'top' and 'bottom' by k`b : Thus, the net rate of formation of HBr may be written solely in terms of reactants, 9-15 i.e.: which simplifies to: as predicted by the empirical rate law: where: 9-16 P9-6(a) 9-17 P9-6(b) Low temperatures with anti-oxidant 9-18 P9-6(c) If the radicals are formed at a constant rate, then the differential equation for the concentration of the radicals becomes: d I dt k0 and I ki I RH 0 k0 k i RH The substitution in the differential equation for R· also changes. Now the equation is: d R dt ki I RH k P1 R O2 and solving and substituting gives: R k P 2 RO 2 k0 RH 0 k P 2 RO 2 k P1 O2 RH Now we have to look at the balance for RO2·. d RO 2 dt k P1 R O2 k P 2 RO 2 RH k t RO 2 and if we substitute in our expression for *R·+ we get 0 k0 RO 2 k t RO 2 2 0 which we can solve for [RO2·+. k0 kt Now we are ready to look at the equation for the motor oil. 9-19 2 0 d RH dt ki I RH k P 2 RO 2 RH and making the necessary substitutions, the rate law for the degradation of the motor oil is: d RH dt r RH k0 kP 2 k0 RH kt P9-6(d) Without antioxidants With antioxidants P9-6 (e) Individualized solution P9-7 (a) 9-20 P9-7 (b) P9-7 (c) P9-7 (d) See Polymath program P9-7-d.pol. 9-21 Everyone becomes ill rather quickly, and the rate at which an ill person recovers to a healthy person is much slower than the rate at which a healthy person becomes ill. Eventually everyone is ill and people start dying. P9-7 (e) Individualized solution P9-7 (f) Individualized solution P9-8 (a) E S k1 E.S E.S k2 E S E.S k3 P E P E k4 E.S By applying PSSH for the complex [E.S], we have k1 [ E ][S ] k 2 [ E.S ] k 3 [ E.S ] k 4 [ P][E ] k1 [ S ] k 4 [ P ] [E] k 2 k3 [ E.S ] rP 0 rS k 3 [ E.S ] k 4 [ P][E ] k 3 k1 [ E ][S ] k 3 k 4 [ P][E ] k 4 [ P][E ] k 2 k3 k 3 k1 [ E ][S ] k 3 k 4 [ P][E ] k 2 k 4 [ P][E ] k 3 k 4 [ P][E ] k 2 k3 k 3 k1 [ S ] k 2 k 4 [ P ] [E] k 2 k3 9-22 k1 k 3 [ s ] k2 [ P] [E] k1 k 2 k2k4 k3 Since E is not consumed, we have where [ ET ] is a constant [ ET ] [ E ] [ E.S ] k1 [ S ] k 4 [ P ] [E] k 2 k3 [ ET ] [ E ] k2 k3 k1 [ S ] k 4 [ P ] [E] k 2 k3 So, k1 k 3 [ S ] rP k2 k3 [ P] [ ET ] ke k1k 3 k2k4 where k e k1 [ S ] k 4 [ P ] P9-8 (b) E k1 S E S E P E S k3 E P E P k5 P 0 k3 E S E P k3 E S k 4 k5 k1 E S k4 E P k2 E S ET k4 S E S k3 E S k4 k5 k5 E P k3 E S since E is not consumed: ET E E E rE S rE S k2 E S E E S k4 E P E S E P or E E ET E S ET 1 E S E P k3 k4 k5 Insert this into the equation for rE·S and solve for the concentration of the intermediate: E S k1 S E T 1 rP k5 E P k3 k4 k1 S k2 k3 k 4 k3 k 4 k5 k5 k 3 k5 E S k4 k5 9-23 rP k1k3 k5 S ET k4 k5 k1 S k2 k4 k3 k3k5 P9-8 (c) k1 E S1 k2 E S1 S2 E S1 k3 E S1S2 k4 k5 E S1S2 P E (1) rE S1 0 k1 E S1 (2) rE S1S2 0 k3 E S S2 k2 E S k3 E S S2 k4 E S1S2 k4 E S1S2 k5 E S1S2 k2 E S k5 E S1S2 If we add these two rates we get: (3) rE S1 rE S1S2 0 k1 E S k3 E S S2 From equation (2) we get E S1S2 k4 k5 Plug this into equation 3 and we get: k1 E S1 k3 S 2 k2 k 4 k5 E S1 E S1S2 k3 S2 k1 E S1 k4 k5 rP k5 E S1S2 ET E ET E 1 E S k1k3 E S1 S2 k1k2 k5 S1 S2 k2 k4 k2 k4 k5 k2 k3 S2 k3 S2 k4 k5 k2 E k2 k5 k3 S2 E S1S2 k1 S1 k3 S 2 k2 k 4 k5 k1k3 S1 S 2 k2 k4 k5 k 2 k3 S 2 9-24 k1k2 k5 S1 S2 rP ET k1 S1 k3 S2 k2 k4 k5 k 2 k 4 k 2 k5 k3 S 2 1 k1k3 S1 S2 k2 k4 k5 k2 k3 S2 P9-8 (d) k3 k1 E S E S k2 k4 E P E P k5 rE S 0 k1 E S E S rE P k1 S E k2 k3 rP rP k5 E P k5 k3 E S k4 E P k1k3 S E k1k3 S k2 k5 E P k4 E P k2 k3 k4 E P E k3 E ET E ET E 1 E S k1 S E P E k4 E P k2 k3 k5 k1 S k4 P k2 k5 k3 k1k3 S ET rP k1 S k2 k3 k2 k3 1 rP k3 E S k4 E P ET rP k2 E S 0 k4 E P E P rP P k4 P k5 k3 S ET k2 k3 k1 S k4 k2 k3 k1k5 P Vmax S KM S KP P 9-25 P9-8 (e) No solution will be given P9-8 (f) No solution will be given P9-9 (a) The enzyme catalyzed reaction of the decomposition of hydrogen peroxide. For a batch reactor: 9-26 P9-9 (b) P9-9 (c) Individualized solution P9-9 (d) Individualized solution 9-27 P9-10 (a) P9-10 (b) 9-28 9-29 X CS 0 CS CS 0 50 2.1 .958 50 P9-10 (c) rS kCS ET 1 K1Cs K 2CS2 If ET is reduced by 33%, -rS will also decrease by 33%. From the original plot, we see that if the curve –rS is decreased by 33%, the straight line from the CSTR calculation will cross the curve only once at approximately CS = 40 mmol/L X CS 0 CS CS 0 50 40 50 0.2 P9-10 (d) Individualized solution P9-10 (e) Individualized solution P9-11 (a) 9-30 P9-11 (b) 9-31 P9-11 (c) Individualized solution P9-11 (d) Individualized solution P9-12 For No Inhibition, using regression, Equation model: 1 rs a0 = 0.008 a0 a1 1 S a1 = 0.0266 For Maltose, Equation model: 1 rs a0 a1 1 S 9-32 a0 = 0.0098 a1 = 0.33 For α-dextran, 1 rs Equation model: a0 = 0.008 a0 a1 1 S a1 = 0.0377 Maltose show non-competitive inhibition as slope and intercept, both changing compared to no inhibition case. α-dextran show competitive inhibition as intercept same but slope increases compared to no inhibition case. P9-13 (a) rS rEHS rP k EHS EHS rP rP K M EH kK M EH S S EH 2 K2 H EH EH K1 H E E ET ET EH K1 H E EH EH K1 H EH 2 EH K2 H EH ET EH 1 1 K1 H K2 H Now plug the value of (EH) into rP 9-33 rS rP kK M EH kK M ET K1 H S 1 K1 H S K1 K 2 H 2 At very low concentrations of H+ (high pH) rS approaches 0 and at very high concentrations of H+ (low pH) rS also approaches 0. Only at moderate concentrations of H+ (and therefore pH) is the rate much greater than zero. This explains the shape of the figure. P9-13 (b) Individualized solution P9-13 (c) Individualized solution P9-14 (a) Case1: Without drug inhibition:Reactions: 1. GLP-1(7-36) Stimulates insulin releases ( Rate constant k1) (a) 2. GLP-1(7-36) + DPP-4 GLP-1(9-36) (Rate constant k2) (a) (b) Rates of reaction (assuming 1st order) are given by: -rGLP-1 = dCa = k1*Ca+ k2*Ca*Cb dt - rDPP-4 = dCb = k2*Ca*Cb dt Sub to: - (Assumed values) at t=0, Ca0 = Cb0 =1 gmol/liter Now, For a 1st order reaction, half life period (t 1/2) = ln (2)/ rate constant Therefore, assuming the half life period of GLP-1(7-36) to be very short (i.e. 10 sec), we get k1 = ln (2)/ 10 (sec-1) k1 = 0.0693 sec-1 9-34 Similarly, given that half life of GLP-1(9-36) is 0.5 to 1 min (i.e. average 0.75 min or 45 sec), we get k2 = ln (2)/ 45 (sec-1) k2 = 0.0154 sec-1 Solving the differential equations using POLYMATH, we get See Polymath program P9-14-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 1. 0.0002638 1. 0.0002638 2 Cb 1. 0.831363 1. 0.831363 3 k1 0.0693 0.0693 0.0693 0.0693 4 k2 0.0154 0.0154 0.0154 0.0154 5 t 0 0 100. 100. 6 X 0.0847 2.166E-05 0.0847 2.166E-05 Differential equations 1 d(Cb)/d(t) = -k2*Ca*Cb 2 d(Ca)/d(t) = -k1*Ca-k2*Ca*Cb Explicit equations 1 k2 = 0.0154 2 k1 = 0.0693 3 X = k1*Ca+k2*Ca*Cb 9-35 Here, we get the rate of reaction (-rGLP-1) value at t = 10 sec to be 0.035973 (gmol/ liter sec). Case2: With drug inhibition Reactions: 1. GLP-1(7-36) + Drug Stimulates insulin releases (Rate constant k1) (a) (e) 2. GLP-1(7-36) + DPP-4 GLP-1(9-36) (Rate constant k2) (a) (b) 3. Drug + DPP-4 E.DPP-4 (Inactive) (Rate constant k3) (e) (b) Rates of reaction are given by: - Sub to: - (Assumed values) 9-36 -rGLP-1 = dCa = k1*Ca*Ce + k2*Ca*Cb dt - rDPP-4 = dCb = k2*Ca*Cb + k3*Ce*Cb dt - rDrug = dCe = k1*Ca*Ce + k3*Ce*Cb dt at t=0, Ca0 = Cb0 =Ce0=1 gmol/liter Now, as derived earlier k1 = 0.0693 sec-1 k2 = 0.0154 sec-1 k3 = rate constant for drug inhibition (to be varied) Taking, k3 = 0.0693, 0.03465, 0.0231, 0.0173, 0.0154, 0.01390, 0.01155, 0.0099, 0.00866, 0.0077, 0.00693 respectively and solving the 3 differential equations using POLYMATH: Example: For k3 = 0.03465 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 1. 0.1451749 1. 0.1451749 2 Cb 1. 0.3512064 1. 0.3512064 3 Ce 1. 0.0232788 1. 0.0232788 4 k1 0.0693 0.0693 0.0693 0.0693 5 k2 0.0154 0.0154 0.0154 0.0154 6 k3 0.03465 0.03465 0.03465 0.03465 7 t 0 0 100. 100. 8 X 0.0847 0.0010194 0.0847 0.0010194 Differential equations 9-37 1 d(Cb)/d(t) = -k3*Ce*Cb-k2*Ca*Cb 2 d(Ce)/d(t) = -k1*Ca*Ce-k3*Ce*Cb 3 d(Ca)/d(t) = -k1*Ca*Ce-k2*Ca*Cb Explicit equations 1 k3 = 0.03465 2 k2 = 0.0154 3 k1 = 0.0693 4 X = k1*Ca*Ce+k2*Ca*Cb Here, we get the rate of reaction (-rGLP-1) value at t = 10 sec to be 0.0234211 (gmol/ liter sec). Similarly, we obtain the rate of reaction (-rGLP-1) value at t = 10 sec, for all values of k3: 9-38 Rate of reaction without Rate constant for inhibition (-rGLP-1) at t=10 Rate of reaction(-rGLP-1) at inhibition( k3) sec t=10sec Ratio ( t= 10 sec) 0.0693 0.035973 0.0198914 1.808469992 0.03465 0.035973 0.0234211 1.535922736 0.0231 0.035973 0.0249 1.444698795 0.0173 0.035973 0.0257217 1.398546752 0.0154 0.035973 0.026 1.383576923 0.0139 0.035973 0.0262283 1.371533801 0.01155 0.035973 0.0265907 1.352841407 0.0099 0.035973 0.0268515 1.339701693 0.00866 0.035973 0.0270509 1.329826364 0.0077 0.035973 0.0272075 1.322172195 0.00693 0.035973 0.0273344 1.316034008 Plotting the ratio of reaction of –rGLP (without inhibition) to the rate – rGLP (with inhibition) as a function of drug inhibition constant k3, we get 9-39 P9-14 (b) The performance equation for mixed reactor is given by:- V vCAo XA rA (1) Where, V = Volume of the reactor, v = volumetric flow rate of the reactant XA = Conversion of the reactant, -rA = rate of reaction in term of conversion CAo = Initial concentration of the reactant, τ = Residence time = (V/ v) As derived earlier, in case of drug inhibition the rate of disappearance of GLP-1(7-36) is given by:-rA = k1*Ca*Ce + k2* Ca* Cb Let the conversion be XA, Therefore we get, -rA = k1*CAo (1- XA)* CAo (M1 - XA) + k2* CAo (1- XA)* CAo (M2 - XA) --------- (2) Where, M1 = (CEo / CAo) & M2 = (CBo / CAo) Putting, equation (2) in (1), we get V = vCAo k1CAo 2 1 X A M1 V = v k1CAo 1 X A M1 τ = k1C XA XA k2 CAo 2 1 XA M2 XA XA k2 C Ao 1 X A M2 XA k2 C Ao 1 X A M2 XA XA Ao 1 XA M1 XA P9-15 -rs = (μmax*Cs*Cc)/(Km+Cs) 9-40 XA μmax= 1hr-1 Km = 0.25 gm/dm3 Yc/s = 0.5g/g (a) Cc0 = 0.1g/dm3 Cs0 = 20 g/dm3 Cc=Cc0 + Yc/s(Cs0-Cs) See polymath problem P9-15-a.pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cc 0.1 0.1 10.1 10.1 2 Cc0 0.1 0.1 0.1 0.1 3 Cs 20. 6.301E-11 20. 6.301E-11 4 Cs0 20. 20. 20. 20. 5 Km 0.25 0.25 0.25 0.25 6 rc 0.0493827 1.273E-09 4.043487 1.273E-09 7 rs -0.0987654 -8.086974 -2.546E-09 -2.546E-09 8 t 0 0 10. 10. 9 umax 1. 1. 1. 1. 0.5 0.5 0.5 0.5 10 Ycs Differential equations 1 d(Cs)/d(t) = rs Explicit equations 1 Cc0 = 0.1 2 Ycs = 0.5 3 Cs0 = 20 4 umax = 1 5 Cc = Cc0+Ycs*(Cs0-Cs) 6 Km = 0.25 7 rs = -umax*Cs*Cc/(Km+Cs) 8 rc = -rs*Ycs 9-41 Plot of Cc and Cs versus time Plot of rs and rc with time (b) Change the polymath code to include rg = μmax*(1-Cc/C∞)*Cc C∞= 1 g/dm3 9-42 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cc 0.1 0.1 0.5751209 0.5751209 2 Cc0 0.1 0.1 0.1 0.1 3 Cinf 1. 1. 1. 1. 4 Cs 20. 19.04976 20. 19.04976 5 Cs0 20. 20. 20. 20. 6 Km 0.25 0.25 0.25 0.25 7 rc 0.0225 0.0225 0.0624999 0.0610892 8 rg 0.09 0.09 0.2499995 0.2443569 9 rs -0.045 -0.1249997 -0.045 -0.1221784 10 t 0 0 10. 10. 11 umax 1. 1. 1. 1. 12 Ycs 0.5 0.5 0.5 0.5 Differential equations 1 d(Cs)/d(t) = rs Explicit equations 1 Cc0 = 0.1 2 Ycs = 0.5 3 Cs0 = 20 4 umax = 1 5 Cinf = 1 6 Cc = Cc0+Ycs*(Cs0-Cs) 7 Km = 0.25 8 rg = umax * (1-Cc/Cinf) * Cc 9 rs = -Ycs*rg 10 rc = -rs*Ycs 9-43 Plot of Cc with time (c) Cs0 = 20g/dm3 Cc0 = 0 The dilution rate at which wash-out occurs will be by setting Cc=0 in equation; Cc = Ycs*(Cs0 – (DKs)/(umax – D)) Dmax = Dmax = = 0.987 hr -1 -1 Thus dilution rate at which washout occurs is 0.987hr . (d) DC C rg , D C SO m CC vO rgV Divide by CCV, CS CS rS , rg CC CCV max D KmD / ( max KM Cs Cs D) 9-44 Cs Km Cs max , Now rS DC C DYC / S C SO CC YS / C rg d DC C dD Dmax,prod = 0.88 hr CS CS DCc = D YC/S (CS0 - KmD / ( Now, for Dmax . prod , YC / S C SO max D) ) 0 -1 Using this value of D we can find the value of Cs Cs = CS KmD / ( max D) 3 = 1.83 g/dm CC YC / S C SO CS = 9.085g/dm 3 3 rs = D(Cs0 – Cs) = 15.98 g/dm /hr (e) Cell death cannot be neglected. Kd =0.02 hr-1 DCc = rg –rd And D(CS0 –Cs)= rS For steady state operation to obtain mass flow rate of cells out of the system, Fc FC =CCv0 = (rg-rd)V= (µ-kd) CCV After dividing by CcV; D=µ-kd Now since maintenance is neglected. Substituting for µ in terms of substrate concentration; Cs = ( D kd )k s ( D kd ) max The stoichiometry equation can be written as : -rs = rg YS/C CC = Yc/s CS 0 ( D kd )ks ( D kd ) max 9-45 Now the dilution rate at can be found by substituting Cc =0; Thus Dmax = max KS CS 0 CS 0 kd = 0.96 hr-1 Similarly the expression for dilution rate for maximum production is given by solving the equation ; (D+kd) Cc = (D+kd ) YC/S (CS0 - Km( D Now for Dmax . prod , d DC C dD kd ) / ( max ( D kd )) ) 0 Thus we obtain Dmax,prod = 0.86 hr-1 (f) In this case the maintenance cannot be neglected. m = 0.2 g/hr/dm3 The correlation for steady substrate concentration will remain the same. Cs = DK S max D But the cell maintenance cannot be neglected. Thus the stoichiometry equation will be changed. The equation will be -rs = Ys/Crg + mCc => -rs = rg/YS/C + mCc t => (Cs0 – Cs) = Cc/YC/S + mCc dt 0 Also we know that by mass balance - dCc / dt ( D )CC Using this relation, the stoichiometric equation for substrate consumption changes to - (CS 0 CS ) CC (1/ YC / S Cc = m/( D)) D(CS 0 DK S / ( max D)) 1/ YC / S m / ( max D)) Now for finding the dilution rate at which wash out occurs, Cc =0; 9-46 So Dwashout = 0.98 hr -1 Similarly to calculate Dmax . prod , d DC C dD 0 Thus we obtain Dmax,prod = 0.74 hr-1 (g) Individualised soultion (h) Individualised solution P9-16 Tessier Equation, rg max 1 e CS / k CC Redoing P9-15 part (a) For batch reaction, dC S dt rS , rS YS / C rC , CC C CO YC / S C SO CS rg See Polymath program P9-16-a.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 7 7 Cs 20 0.0852675 20 0.0852675 Cco 0.1 0.1 0.1 0.1 Ycs 0.5 0.5 0.5 0.5 Cso 20 20 20 20 Cc 0.1 0.1 10.057366 10.057366 k 8 8 8 8 umax 1 1 1 1 Ysc 2 2 2 2 rg 0.0917915 0.0917915 3.8563479 0.1066265 rs -0.183583 -7.7126957 -0.183583 -0.213253 Rates 0.183583 0.183583 7.7126957 0.213253 ODE Report (RKF45) Differential equations as entered by the user [1] d(Cs)/d(t) = rs 9-47 max 1 e CS / k CC Explicit equations as entered by the user [1] Cco = 0.1 [2] Ycs = 0.5 [3] Cso = 20 [4] Cc = Cco+Ycs*(Cso-Cs) [5] k = 8 [6] umax = 1 [7] Ysc = 2 [8] rg = umax*(1-exp(-Cs/k))*Cc [9] rs = -Ysc*rg [10] RateS = -rs Redoing P9-15 part (b) D C SO DC C rg m C C vO Divide by CCV, CS rg V D k ln 1 CS rS rg CC max 1 e CS / k CCV max 1 e CS / k D max Now rS CC YS / C rg YC / S C SO For dilution rate at which wash out occur, k ln 1 CSO = CS CS CC = 0 D max DMAX max 1 e CS 0 / k 3 1hr 1 1 e 20 g / dm / 8 g / dm # Redoing P9-15 part (c) DC C DYC / S C SO CS CS k ln 1 D max 9-48 0.918hr 1 DCC DYC / S C SO k ln 1 D max Now d DC C dD For Dmax . prod , 0 Dmax . prod = 0.628 hr-1 P9-16 (b) Individualized solution P9-17 (a) rg = max CC For CSTR, KM DC C CS CS CS D C SO rg YC / S C SO DC C rg CS v0CC dCC dt V dCC dt rg Substrate Balance: rg FC dCS dt v0CS 0 v0CS YS rg C CS CC K M CS max 9-49 YS / C rg D 4.5 g / dm 0.8hr 1 1g / dm 3 4.5 g / dm 3 4 1 g / dm 3 6250dm 3 rgV 3 C S CC K M CS Flow of cells out = Flow of cells in Cell Balance: FC 1g / dm 3 0.5(10 1) g / dm P9-17 (b) FC rS max vO 4.5 g / dm 3 V V rS 10 g / dm 3 1 0.9 C SO 1 X CC CS 3 vO V This would result in the Cell concentration growing exponentially. This is not realistic as at some point there will be too many cells to fit into a finite sized reactor. Either a cell death rate must be included or the cells cannot be recycled. P9-17 (c) Two CSTR’s For 1st CSTR, V = 5000dm3 , DC C rS rg D C SO YS / C rg rg = CS max KM CS CC CS See Polymath program P9-17-c-1cstr.pol. POLYMATH Results NLES Solution Variable Value f(x) Ini Guess Cc 4.3333333 9.878E-12 4 Cs 1.3333333 1.976E-11 5 umax 0.8 Km 4 Csoo 10 Cso 10 Ysc 2 rg 0.8666667 rs -1.7333333 V 5000 vo 1000 D 0.2 X 0.8666667 Cco 4.33 NLES Report (safenewt) Nonlinear equations [1] f(Cc) = D*(Cc)-rg = 0 [2] f(Cs) = D*(Cso-Cs)+rs = 0 Explicit equations [1] umax = 0.8 [2] Km = 4 [3] Csoo = 10 [4] Cso = 10 [5] Ysc = 2 [6] rg = umax*Cs*Cc/(Km+Cs) 9-50 rS D vO V [7] rs = -Ysc*rg [8] V = 5000 [9] vo = 1000 [10] D = vo/V [11] X = 1-Cs/Csoo [12] Cco = 4.33 CC1 = 4.33 g/dm3 CS1 = 1.33 g/dm3 For 2nd CSTR, D C C 2 X = 0.867 CP1 = YP/CCC1 =0.866 g/dm3 C C1 rg D C S1 See Polymath program P9-17-c-2cstr.pol. POLYMATH Results NLES Solution Variable Value f(x) Ini Guess Cc 4.9334151 3.004E-10 4 Cs 0.1261699 6.008E-10 5 umax 0.8 Km 4 Csoo 10 Cs1 1.333 Ysc 2 rg 0.120683 rs -0.241366 V 5000 vo 1000 D 0.2 X 0.987383 Cc1 4.33 NLES Report (safenewt) Nonlinear equations [1] f(Cc) = D*(Cc-Cc1)-rg = 0 [2] f(Cs) = D*(Cs1-Cs)+rs = 0 Explicit equations [1] umax = 0.8 [2] Km = 4 [3] Csoo = 10 [4] Cs1 = 1.333 [5] Ysc = 2 [6] rg = umax*Cs*Cc/(Km+Cs) [7] rs = -Ysc*rg [8] V = 5000 [9] vo = 1000 9-51 CS rS [10] D = vo/V [11] X = 1-Cs/Csoo [12] Cc1 = 4.33 CC2 = 4.933 g/dm3 CS2 = 1.26 g/dm3 X = 0.987 CP1 = YP/CCC1 =0.9866 g/dm3 P9-17 (d) For washout dilution rate, Dmax DMAX .PROD max 1 CC = 0 max KM C SO C SO 0.8hr 1 10 g / dm 3 4 g / dm 3 10 g / dm 3 KM K M C SO 0.57hr 1 4 g / dm 3 4 g / dm 3 10 g / dm 3 0.8hr 1 1 0.37 hr 1 Production rate = CCvO(24hr) = 4.85 g / dm 3 x1000dm3/hrx24hr = 116472.56g/day P9-17 (e) For batch reactor, V = 500dm3, dC C dt rg dC S dt rS CCO = 0.5 g/dm3 CSO = 10g/dm3 rS YS / C rg rg = max KM See Polymath program P9-17-e.pol. POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 6 6 Cc 0.5 0.5 5.4291422 5.4291422 Cs 10 0.1417155 10 0.1417155 Km 4 4 4 4 Ysc 2 2 2 2 umax 0.8 0.8 0.8 0.8 rg 0.2857143 0.1486135 1.403203 0.1486135 rs -0.5714286 -2.8064061 -0.2972271 -0.2972271 ODE Report (RKF45) Differential equations as entered by the user [1] d(Cc)/d(t) = rg [2] d(Cs)/d(t) = rs 9-52 CS CC CS Explicit equations as entered by the user [1] Km = 4 [2] Ysc = 2 [3] umax = 0.8 [4] rg = umax*Cs*Cc/(Km+Cs) [5] rs = -Ysc*rg For t = 6hrs, CC = 5.43g/dm3. So we will have 3 cycle of (6+2)hrs each in 2 batch reactors of V = 500dm3. Product rate = CC x no. of cycle x no. of reactors x V = 5.43 g/dm3 x 3 x 2 x 500dm3 = 16290g/day. P9-17 (f) Individualized solution P9-17 (g) Individualized solution P9-18 (a) max D CS D KS max CS CS KS KS CS max max is the intercept and 1 is the slope max 9-53 CS gm /dm2 D(day-1) CS/D 1 1 1 Slope = 0.5 day max 3 1.5 2 4 1.6 2.5 intercept = 0.5 gm/dm3 = 2 KS = 0.5*2 = 1 P9-18 (b) CC DK S YC S CSO max D Inserting values from dataset 4 4 1.8 1.0 2.0 1.8 YC S 50 YS C 1 YC / S 4 50 9.0 10.25 P9-18 (c) Individualized solution P9-18 (d) Individualized solution P9-19 (a) See Polymath program P9-19-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cc 1. 1. 1.774022 1.774022 2 f 0 0 0.99985 0 3 t 0 0 48. 48. Differential equations 1 d(Cc)/d(t) = f* Cc * 0.9 / 24 Explicit equations 9-54 10 1.8 5.6 1 f = (If (((t > 0) And (t < 12)) Or ((t > 24) And (t < 36))) Then (sin(3.14 * t / 12)) Else (0)) (b) Given the initial concentration as Co = 0.5 mg/litre we have, = ln = Cc = exp = 0.9 day -1 = 0.0375 hr -1 From 6am to 6pm , t= 12 hrs Cc = exp Cc = exp Cc = exp Cc = 1.332 } } *0.0375* } Thus the concentration progresses as = 1.332(conc. of previous day) 9-55 Therefore the time taken to reach the concentration of 200 mg/dm 3 using MS Excel is 22 days. (d) From part (b) Concentration at the end of 1st day = 1.33Co Concentration at the start of 2nd day =1.33Co/2 + 100 (mg/lit) Concentration at the end of 2rd day= 1.33(1.33Co/2 + 100) And so forth. Thus the concentration progresses as = 1.332(conc. of previous day)+100 Solving for the progression on MS Excel we find the concentration to converge to 299.4011mg/lit Thus, at the end of 365 days the conc. becomes = 299.4011mg/lit (e) Assuming that dilution and removal of algae is done at the end of the day after the growth period is over. Then, Rate of decrease of conc. = = - k Cc where, k = 1 (day-1) At t=0, Co= 200mg/lit (i.e. maximum concentration allowed for maximum productivity at the end of the day) So, removal per day:Cc= Co exp (-kt) = 200 exp (-1 day-1 x 1 day) = 200 exp (-1) Cc= 73.5 mg/dm3/day Volume of the pond = 5000 gallons or 18940.5 dm3 Total mass flow rate of algae = 1392.1 g/day 9-56 (f) Now, since CO2 will affect the rate of growth of algae too, then let the reaction be:CO2 + Algae more algae Hence, A +C 2C Where, A: CO2 C: algae Now, rate of growth of algae should be rc = k sin( CaCc Earlier, Ca = 1.69gm/kg of water = 1.69 gm/dm3 of water (density of water = 1kg/lit) We have rate law as rc = sin ( Cc ( CO2 concentration was assumed to be a constant = 1.69g /dm3 of water ) Hence, = k 1.69 gm / dm3 k = (.9 per day) (1.69 gm / dm3) k = 0.5325 dm3/g day or 0.022 dm3/g hr A At t=0 + Ca0 C Cc0 2C 0 Let conversion with respect to C is X Then, At t=t C Ca0 – XCc0 Cc0 (1-X) 2Cc0X Cc= Cc0 (1+ X) Ca= Ca0 – XCc0 = Cc0 (M – X) where, M= Ca0/Cc0 Hence, = k sin ( CaCc 9-57 thus, total number of moles of => = k sin ( => = Cc0 k sin ( => (1+X) (M-X) = => ln = (M+1)k Cc0 {1 - => => Cc0 (1+X) Cc0 (M-X) } = exp [(M+1) k Cc0 {1 X (1 + exp [k (M+1) Cc0 {1 - {1 - } } } ] ]/M) = exp [k (M+1) Cc0 ]-1 => X = Now, X= 1Hence , =1- We have, Ca0 = Ks = 2g/dm3 & Cc0 = 1mg/ dm3 (assuming initial seeding value of algae from (c)) M= Ca0/Cc0 = 2000 Substituting the values we have the concentration profile i.e. (g) Let A: the species of unwanted algae C: the species of desired algae Then, Rate of growth of A = 2 = 2 for A = 2 x for C Now overall density of the medium at any time t 9-58 Vs. t = Ca + Cc Hence, from given conditions, Ca=0.5(Ca + Cc) So, at that time Ca=Cc Now, = Cc Cc = Cc0 exp( = Ca Ca = Ca0 exp (2 Assuming, Cco= initial seed concentration of desired algae= 1 mg/litre & Cao = 0.1 mg/litre (given). Now, since the concentration is very less assuming there is no constraint of sunlight. Ca = Cc Cc0 exp( = Ca0 exp (2 ln (Cco/Cao) = exp ( where, = 0.9 per day Putting the values, we get t = 2.56 days or 61.4 hrs. Since the number of days is coming less than 4.347 days which was calculated in part (c), so the effect of daylight can be neglected. Hence, the initial assumption is verified. P9-20 The following errors are present in this solution1. For the Eadie-Hofstee model, we plot –rS as a function of [-rS/(S)] and for the HanesWoolf model, we plot [(S)/-rS] as a function of (S). Since the y-axis plot parameter here is [(S)/-rS], it is a Hanes-Woolf plot and not the Eadie-Hofstee plot.\ 2. For Competitive Inhibition, Hanes-Woolf form is: For Uncompetitive Inhibition, Hanes-Woolf form is: 9-59 Since the intercept is fixed and slope is changing in the given plot, this is uncompetitive inhibition rather than being competitive one. 3. The x-axis variable is written wrong as (S + S2). It should be (S) for Hanes-Woolf form. 4. The expression for intercept is correct but the slope is given wrong. The correct expressions are - 5. As concentration of inhibitor (I) increases, slope increases. In the given plot, slope for line 1 is more as compared to line 2 in spite of having lower concentrations. This implies that the concentration values are switched. Also the numerically calculated slope values are wrong. The correct values are as – Line 1: (I) = 0.05 M Slope 1 = 35 Line 2: (I) = 0.02 M Slope 2 = 15.5 6. Calculations on the basis of correct values – ; ; Solving these above equations, we get kinetic law parameters Vmax = 0.4 ; KM = 0.04 KI = 3.85e-3 ; 9-60 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. 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All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 10-1 Solutions for Chapter 10 – Catalysis and Catalytic Reactors P10-1 Individualized solution P10-2 (a) Example 10-1 (1) CT .S CB . s Cv KT PT Cv K B PB KT PT 0 (1 X ) K B PT 0 X KB 1.39 KT KT (1 X ) KB X 1.038 CT .S Therefore, C = f(X) can be plotted. B.s (2) Cv Ct 1 1 KT PT K B PB 1 1 KT PT 0 (1 X ) K B PT 0 X Here, PT0 = yA0PTotal = 0.3X40 atm = 12 atm & K B 1.39 KT 1.038 Cv Therefore, C = f(X) can be plotted. t (3) CB . S Ct Cv K B PB Cv (1 KT PT K B PB ) K B PT 0 X 1 KT PT 0 (1 X ) K B PT 0 X CB .S Therefore, C = f(X) can be plotted. t P10-2 (b) Example 10-2 (1) See polymath problem P10-2-b.pol Increasing the pressure will increase the conversion for the same catalyst weight. At 40 atm, we had 68.2% conversion for a catalyst weight of 10000kg. While, at 80 atm we have 85.34% conversion for the same weight of the catalyst. 10-2 At 1 atm, we get 0.95% conversion for 10000 kg of catalyst. However, it’s not practically possible to operate at inlet pressure of 1 atm, because there will be no flow of feed into the PFR, due to absence of pressure difference. (2) If the flow rate is decreased the conversion will increase for two reasons: (1) smaller pressure drop and (2) reactants spend more time in the reactor. (3) From figure E10-3.1 we see that when X = 0.6, W = 5800 kg. P10-2 (c) Example 10-3 With the new data, model (a) best fits the data (a) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe*Ph/(1+Kea*Pea+Ke*Pe) Variable Ini guess Value 95% confidence k 3 3.5798145 0.0026691 Kea 0.1 0.1176376 0.0014744 Ke 2 2.3630934 0.0024526 Precision R^2 R^2adj Rmsd Variance = 0.9969101 = 0.9960273 = 0.0259656 = 0.0096316 (b) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe*Ph/(1+Ke*Pe) Variable Ini guess Value 95% confidence k 3 2.9497646 0.0058793 Ke 2 1.9118572 0.0054165 Precision R^2 R^2adj Rmsd Variance = 0.9735965 = 0.9702961 = 0.0759032 = 0.0720163 (c) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe*Ph/((1+Ke*Pe)^2) Variable Ini guess Value 95% confidence 10-3 k Ke Precision R^2 R^2adj Rmsd Variance 3 2 1.9496445 0.3508639 0.319098 0.0756992 = 0.9620735 = 0.9573327 = 0.0909706 = 0.1034455 (d) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe^a*Ph^b Variable Ini guess Value 95% confidence k 3 0.7574196 0.2495415 a 1 0.2874239 0.0955031 b 1 1.1747643 0.2404971 Precision R^2 R^2adj Rmsd Variance = 0.965477 = 0.9556133 = 0.0867928 = 0.107614 Model (e) at first appears to work well but not as well as model (a). However, the 95% confidence interval is larger than the actual value, which leads to a possible negative value for Ka. This is not possible and the model should be discarded. Model (f) is the worst model of all. In fact it should be thrown out as a possible model due to the negative R^2 values. (e) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe*Ph/((1+Ka*Pea+Ke*Pe)^2) Variable Ini guess Value 95% confidence k 3 2.113121 0.2375775 Ka 1 0.0245 0.030918 Ke 1 0.3713644 0.0489399 Precision R^2 R^2adj Rmsd Variance = 0.9787138 = 0.9726321 = 0.0681519 = 0.0663527 (f) POLYMATH Results Nonlinear regression (L-M) Model: ReactionRate = k*Pe*Ph/(1+Ka*Pea) 10-4 Variable k Ka Precision R^2 R^2adj Rmsd Variance Ini guess 3 1 Value 95% confidence 44.117481 7.1763989 101.99791 16.763192 = -0.343853 = -0.5118346 = 0.5415086 = 3.6653942 P10-2 (d) Individualized solution P10-3 Solution is in the decoding algorithm given with the modules P10-4 P10-4 (a) 10-5 P10-4 (b) Adsorption of isobutene limited P10-4 (c) 10-6 P10-4 (d) P10-4 (e) Individualized solution P10-5 (a) H H2 E Ethylene A Ethane H2 C 2H 4 H E cat C 2H 6 A Because neither H2 or C2H6 are in the rate law they are either not adsorbed or weakly adsorbed. Assume H2 in the gas phase reacts with C2H6 adsorbed on the surface and ethane goes directly into the gas phase. Then check to see if this mechanism agrees with the rate law Eley Rideal E S E S H E S A S rE k AD PE CV rS k SC E SPH 2 CE S KE 10-7 Assume surface reaction CE S K E PE C V rS k S C E SPH CT CV rA k SK E C T CE S PE PH 1 K E PE P10-5 (b) Individualized solution P10-6 O2 2S 2O S A2 C3 H 6 O S C3 H 5OH S C3 H 6OH S C3 H 5OH rB rS rAD k A PA2 CV2 rAD kA 0 CA S CV K A PA rB rS rC S k D CC S rC S kD 0 CC S K C PC CV CT CV rB rS C S S C A2 S KA k3 PBCV K A PA CA S CC S k D CC S CV 1 K C PC CV K A PA K C PC k3CT PB K A PA 1 K A PA 2A S B A S k3 PB C A S PC CV KD 2S KC PC 10-8 C S C S P10-7 (a) P10-7 (b) 10-9 P10-7 (c) 10-10 P10-7 (d) Individualized solution P10-7 (e) Individualized solution P10-8 10-11 P10-9 P10-9 (a) 10-12 P10-9 (b) P10-10 10-13 P10-10 (a) 10-14 P10-10 (b) 10-15 Substituting the expressions for CV and CA·S into the equation for –r’A P10-10 (c) Individualized solution P10-10 (d) First we need to calculate the rate constants involved in the equation for –r’A in part (a). We can rearrange the equation to give the following 10-16 Thus from the slope and intercept data See Polymath program P10-10-d.pol. POLYMATH Results Calculated values of the DEQ variables Variable W X e initial value 0 0 1 minimal value 0 0 1 maximal value 23 0.9991499 1 10-17 final value 23 0.9991499 1 Pao Pa k1 k2 Fao ra rate 10 10 560 2.04 600 -12.228142 12.228142 10 0.0042521 560 2.04 600 -68.5622 2.3403948 10 10 560 2.04 600 -2.3403948 68.5622 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(W) = -ra/Fao Explicit equations as entered by the user [1] e = 1 [2] Pao = 10 [3] Pa = Pao*(1-X)/(1+e*X) [4] k1 = 560 [5] k2 = 2.04 [6] Fao = 600 [7] ra = -k1*Pa/((1+(k2*Pa))^2) [8] rate = -ra P10-10 (e) Individualized solution P10-10 (f) 10-18 10 0.0042521 560 2.04 600 -2.3403948 2.3403948 Use these new equations in the Polymath program from part (d). See Polymath program P10-10-f.pol. POLYMATH Results Calculated values of the DEQ variables Variable W X y e Pao Pa k1 k2 Fao ra rate alpha initial value 0 0 1 1 10 10 560 2.04 600 -12.228142 12.228142 0.03 minimal value 0 0 0.0746953 1 10 7.771E-05 560 2.04 600 -68.584462 0.0435044 0.03 maximal value 23 0.9997919 1 1 10 10 560 2.04 600 -0.0435044 68.584462 0.03 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(W) = -ra/Fao [2] d(y)/d(W) = -alpha*(1+X)/2/y Explicit equations as entered by the user [1] e = 1 [2] Pao = 10 [3] Pa = y*Pao*(1-X)/(1+e*X) [4] k1 = 560 [5] k2 = 2.04 [6] Fao = 600 [7] ra = -k1*Pa/((1+(k2*Pa))^2) [8] rate = -ra [9] alpha = .03 10-19 final value 23 0.9997919 0.0746953 1 10 7.771E-05 560 2.04 600 -0.0435044 0.0435044 0.03 P10-11(a) 10-20 P10-11 (b) P10-11 (c) The estimates of the rate law parameters were given to simplify the search techniques to make sure that it converged on a false minimum. In real life, one should make a number of guesses of the rate law parameters and they should include a large range of possibilities P10-11 (d) A ra PA B H kPA 1 K A PA K B PB PA0 (1 X ) , PB (1 X ) K H PH 2 PA0 X , PH (1 X ) PA0 X here, (1 X ) 10-21 y A0 1(2 1) 1 Where, k 0.00137 K A 4.77 KB 0.259 KH 0.424 PA0 15atm FA0 10mol / sec Now, the design equation for the PFR, rA dX dW FA0 Solving the above equations using Polymath (Refer to P10-11-d.pol) Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Fao 10. 10. 10. 10. 2 k 0.00137 0.00137 0.00137 0.00137 3 Ka 4.77 4.77 4.77 4.77 4 Kb 0.262 0.262 0.262 0.262 5 Kh 0.423 0.423 0.423 0.423 6 Pa 15. 3.064E-09 15. 3.064E-09 7 Pao 15. 15. 15. 15. 8 Pb 0 0 7.5 7.5 9 Ph 0 0 7.5 7.5 10 ra -3.904E-06 -1.26E-05 -1.114E-13 -1.114E-13 11 W 0 0 2.0E+06 2.0E+06 12 X 0 0 1. 1. 10-22 Differential equations 1 d(X)/d(W) = -ra/Fao Explicit equations 1 Pao = 15 2 k = 0.00137 3 Ka = 4.77 4 Kb = 0.262 5 Kh = 0.423 6 Fao = 10 7 Ph = Pao*X/(1+X) 8 Pa = Pao*(1-X)/(1+X) 9 Pb = Pao*X/(1+X) 10 ra = -k*Pa/((1+Ka*Pa+Kb*Pb+Kh*Ph)^2) From the above graph, we get the weight of catalyst required for 85% conversion is 1.2083x106 kg. The required catalyst weight is so high because of very low value of reaction constant ’k’. 10-23 P10-12(a) Proposed Single site Mechanism: S ' H 2O S ' H 2O S ' H 2O S ' H2 S ' H2 S ' H2 S' 1 O2 2 1 O2 2 S Rate of adsorption: rAD Rate of surface reaction: rs Rate of desorption: rD CS ' H 2O k AD (Cv ' PH 2O K H 2O ) ks CS ' H 2O ---------- (1) k D (CS ' H 2 K H 2 PH 2 Cv ' ) Assuming, surface reaction to be rate limiting, we get rAD rD 0 k AD k D CS ' H 2 O K H 2OCv ' PH 2O and CS ' H 2 K H 2 PH 2 Cv ' From total site balance, we get Ct Cv ' 1 K H 2O PH 2O K H 2 PH 2 Putting all the values in equation (1), we get k s K H 2O Ct PH 2O rs 1 K H 2O PH 2O K H 2 PH 2 rs kPH 2O 1 K H 2O PH 2O K H 2 PH 2 Where, k ks K H 2OCt P10-12(b) Proposed Mechanism: S ' H 2O S ' H 2O S ' H 2O S H2 S H2 S H2 Rate of adsorption: rAD k D (Cv ' PH 2O CS ' H 2O K H 2O ) 10-24 Rate of surface reaction: rs Rate of desorption: rD ks (CS ' H 2O CS H 2 ) ---------- (1) k D (CS H 2 K H 2 PH 2 Cv ) Assuming, surface reaction to be rate limiting, we get rAD rD 0 k AD k D K H 2OCv ' PH 2O and CS H 2 CS ' H 2 O K H 2 PH 2 Cv From total site balance, we get Ct ' Cv ' 1 K H 2O PH 2O Cv Ct 1 K H 2 PH 2 Putting all the values in equation (1), we get K H O PH O Ct ' K H 2 PH 2 Ct rs k s ( 2 2 ) 1 K H 2O PH 2O 1 K H 2 PH 2 P10-12(c) Proposed Mechanism: Step (1) S h S ' O2 S ' O2 S ' O2 S ' H 2O Step (2) S ' H 2O S H2 S ' H 2O S H2 S H2 For Step (1) Rate of adsorption of O2: rAD O 2 Rate of Reaction: rSO 2 kD O 2 (Cv kSO 2 (CS ' O2 CS ' O2 KS ) KO2 PO2 Cv ' ) Rate of surface reaction of water is rate controlling, we get rAD O 2 rS O 2 0 kD O 2 kS O 2 CS ' O2 Cv K S ----------- (2) 10-25 CS ' O2 KO2 PO2 Cv ' ------- (3) Equating (2) and (3), we get Cv KO2 PO2 Cv ' KS -------- (4) Now, here the site balance gets modified because oxygen is also getting adsorbed. Ct Cv Cv ' CS ' O2 CS ' H 2O CS H 2 Putting, the values and replacing Cv using equation (4), we get Cv ' (1 K O2 PO2 And, Cv rs K H 2O PH 2O KO2 PO2 Cv ' KS Ct K O2 PO2 K O2 K H 2 PO2 PH 2 KS KS = K S (1 KO2 PO2 ) KO2 PO2 Ct KO2 PO2 K H 2O PH 2O KS Putting all the values in equation (1), we get K H 2O PH 2OCt ks ( KO2 PO2 K O2 K H 2 PO2 PH 2 (1 KO2 PO2 K H 2O PH 2O ) KS KS P10-13 (a) 10-26 K O2 K H 2 PO2 PH 2 KS K S (1 KO2 PO2 ) K H 2 PH 2 K O2 PO2 Ct K O2 PO2 K H 2O PH 2O KS K O2 K H 2 PO2 PH 2 KS ) ) P10-13 (b) P10-14 Assume the rate law is of the form rDep At high temperatures K rDep rDep 2 PVTIPO Run 1 k 0.028 0.45 0.2 Run 5 2 as T and therefore KPVTIPO 2 kPVTIPO 0.05 Run 2 2 kPVTIPO 2 1 KPVTIPO 11.2 2 11.28 2 11.25 7.2 0.8 2 At low temperature and low pressure rDep 2 kPVTIPO 10-27 1 rDep k 2 PVTIPO Run 1 0.004 0.1 Run 2 2 0.015 0.2 2 0.4 0.375 These fit the low pressure data 2 At high pressure KPVTIPO 2 kPVTIPO 2 KPVTIPO rDep 1 k K This fits the high pressure data At PVTIPO = 1.5, r = 0.095 and at PVTIPO = 2, r = 0.1 Now find the activation energy At low pressure and high temperature k = 11.2 At low pressure and low temperature k = 0.4 ln k2 k1 E 1 R T1 ln 11.2 0.4 E R E R 7743 E 15330.65 1 T2 E T2 T1 R T1T2 473 393 473 393 cal mol 10-28 P10-15 P10-16 (a) Using Polymath non-linear regression few can find the parameters for all models: See Polymath program P10-16.pol. (1) POLYMATH Results Nonlinear regression (L-M) Model: rT = k*PM^a*PH2^b Variable k a b Ini guess 1 0.1 0.1 Value 1.1481487 0.1843053 -0.0308691 95% confidence 0.1078106 0.0873668 0.1311507 10-29 Precision R^2 R^2adj Rmsd Variance = 0.7852809 = 0.7375655 = 0.0372861 = 0.0222441 α = 0.184 β = -0.031 k = 1.148 (2) POLYMATH Results Nonlinear regression (L-M) Model: rT = k*PM/(1+KM*PM) Variable k KM Precision R^2 R^2adj Rmsd Variance Ini guess 1 2 Value 12.256274 9.0251862 95% confidence 2.1574162 1.8060287 = 0.9800096 = 0.9780106 = 0.0113769 = 0.0018638 k = 12.26 KM = 9.025 (3) POLYMATH Results Nonlinear regression (L-M) Model: rT = k*PM*PH2/((1+KM*PM)^2) Variable k KM Precision R^2 R^2adj Rmsd Variance Ini guess 1 2 Value 8.4090333 2.8306038 95% confidence 18.516752 4.2577098 = -4.3638352 = -4.9002187 = 0.1863588 = 0.5001061 k = 8.409 KM = 2.83 (4) 10-30 POLYMATH Results Nonlinear regression (L-M) Model: rT = k*PM*PH2/(1+KM*PM+KH2*PH2) Variable k KM KH2 Ini guess 1 2 2 Value 101.99929 83.608282 67.213622 95% confidence 4.614109 7.1561591 5.9343217 Nonlinear regression settings Max # iterations = 300 Precision R^2 R^2adj Rmsd Variance = -3.2021716 = -4.1359875 = 0.1649487 = 0.4353294 k = 102 KM = 83.6 KH2 = 67.21 P10-16 (b) We can see from the precision results from the Polymath regressions that rate law (2) best describes the data. P10-16 (c) Individualized solution. P10-16 (d) We have chosen rate law (2) Proposed Mechanism M S M S M S H 2( g ) T( g ) Rate of adsorption: rAD k AD (Cv PM Rate of surface reaction: rs CM S ) KM k s CM S ---------- (1) Assuming, surface reaction to be rate limiting: rAD 0 k AD CM S Cv PM K M 10-31 Putting, the value of CM S in Equation (1) rs ks Cv PM K M ----------------- (2) Now, applying site balance Ct Cv CM S Ct Cv Cv PM K M Cv Ct 1 PM K M Putting in Equation (2), we get ks K M Ct PM rs 1 K M PM rs kPM Where, k = ks K M Ct 1 K M PM P10-17 Mistakes in the solution: 1) In the CC.S expression, the constant should be KA2 instead of KDC 2) The overall site balance should include the product, as it too is getting adsorbed. 3) The final rate law expression derived is wrong. The correct expression has been derived below: Assuming, desorption to be rate controlling, we get: rS1 kS1 rAD k AD A S C A.S A.S rS 2 kS 2 0 A.S K A PACV A.S A2 .S S C A2 .S K S C A2.s / CV C A2 .S K S K A 2 PA 2CV 10-32 A2 .S B ( g ) rS2 C.S CC .S ] K A2 k S2 [ PB C A 2 .S CC .S K A2 PB C A2 .S C A2. S CC .S K A2 PB K S CC .S K A2 PB K S K A 2 PA 2Cv CV now, Ct CV C A.S C A2 .S CC .S Putting, all the values in equation (1), we get Ct CV K A PACV K S C A2.S CV Ct CV (1 K A PA K S K A2 PA 2 C A2 . S K A2 PB K S K A2 K S K A2 PB PA2 ) 2 CV now, rC rC rC kc CC .S kC K A2 PB K S C A2.S CV kC K A2 K S K A2 PB PA2Cv kC K A2 K S K A2 PB PA2 (1 K A PA K S K A2 PA 2 (1 K A PA kPB PA2 K S K A2 PA 2 K A2 K S K A2 PB PA2 ) Where, k K A2 K S K A2 PB PA2 ) kC K A2 K S K A2 10-33 CD10GA-1 10-34 10-35 CD10GA-2 10-36 CD10GA-3 10-37 10-38 10-39 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. No liability is assumed for the incidental or consequential damage in connection with or arising out of the use of the information or programs contained herein. Visit us on the Web : www.prenhallprofessional.com Copyright © 2011 Pearson Education,Inc . This work is protected by United States copyright laws and is provided solely for the use of the instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including the World Wide Web ) will destroy the integrity of the work and is not permitted . The work and the materials from it should never be made available to the students except by the instructors using the accompanying texts in the classes. All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 11-1 Solutions for Chapter 11: Non-isothermal Reactor Design-The Steady-state energy balance and adiabatic PFR applications P11-1 Individualized solution P11-2 (a) Example 11-1 For CSTR V X FA0 X rA X k 1 X k Ae E RT 1 Ae E RT 1 k T T0 0 One equation, two unknowns Adiabatic energy balance H Rx X CPA In two equations and two unknowns In Polymath form the solution Ae E RT X 1 Ae E RT f X f T H Rx X CPA T0 Enter X, A, E, R, C PA , T0 and HRx to find τ and from that you can find V. P11-2 (b) Example 11-2 Helium would have no effect on calculation %Error CP T TR H Rx CP T TR 1270 100 5.47% 23,210 11-2 P11-2 (c) Example 11-3 Set Vfinal = 0.8 m3 POLYMATH Results Calculated values of the DEQ variables Variable V X Ca0 Fa0 T Kc k Xe ra rate initial value 0 0 9.3 146.7 330 3.099466 4.2238337 0.7560658 -39.281653 39.281653 minimal value 0 0 9.3 146.7 330 2.852278 4.2238337 0.7404133 -56.196156 39.281653 maximal value 0.8 0.2603491 9.3 146.7 341.27312 3.099466 9.3196276 0.7560658 -39.281653 56.196156 final value 0.8 0.2603491 9.3 146.7 341.27312 2.852278 9.3196276 0.7404133 -56.196156 56.196156 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra/Fa0 Explicit equations as entered by the user [1] Ca0 = 9.3 [2] Fa0 = .9*163 [3] T = 330+43.3*X [4] Kc = 3.03*exp(-830.3*((T-333)/(T*333))) [5] k = 31.1*exp(7906*(T-360)/(T*360)) [6] Xe = Kc/(1+Kc) [7] ra = -k*Ca0*(1-(1+1/Kc)*X) [8] rate = -ra Change the entering temperature T0 in the polymath code above (highlighted in yellow), and record the exiting conversion: T X 330 0.26 340 0.54 350 0.68 370 0.66 390 0.65 X 11-3 420 0.62 450 0.59 500 0.55 600 0.48 We see that there is a maximum in the exit conversion corresponding to T0 = 350K. Therefore, the inlet temperature we would recommend is 350K. P11-2(d) Aspen Problem P 11-2(e) (1) (2) At high To, the graph becomes asymptotic to the X-axis, that is the conversion approaches 0. At low To, the conversion approaches 1. (3) On addition of equal molar inerts, the energy balance reduces to: X EB CPA T T0 CPI (T T0 ) H Rx CPA CPI 11-4 X EB 2CPA T T0 H Rx (4) It is observed that at the same inlet temperature, the equilibrium conversion on the addition of inerts is greater. This also follows from the Le Chatelier’s principle. P11-2(f) . . Q m CP T . Q 220kcal / s 220 103 m 18(400 270) 854.7 mol / s . For the2nd case: Hot Stream: 460K 350K Cold Stream: 270K 400K LMTD = 69.52 oC 220 103 A 100 69.52 31.64m2 11-5 P11-3 A B C 3 Since the feed is equimolar, CA0 = CB0 = .1 mols/dm CA = CA0(1-X) CB = CB0(1-X) Adiabatic: T X[ H R (T0 )] X CP i CPi T0 CP C pC C pB C pA H R (T ) HC Ci C pA i T 30 15 15 0 HB H A = -41000-(-15000-(-20000) = -6000 cal/mol A cal 15 15 30 B C pB mol K 6000 X 300 200 X 30 k C A2 0 (1 X ) 2 .01 k (1 X )2 300 rA P11-3 (a) dX rA VPFR FA0 VCSTR FA0 X rA For the PFR, FA0 = CA0v0 = (.1)(2) = .2 mols/dm3 See Polymath program P11-3-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 X 0 0 0.85 0.85 2 V 0 0 308.2917 308.2917 3 Ca0 0.1 0.1 0.1 0.1 4 Fa0 0.2 0.2 0.2 0.2 5 T 300. 300. 470. 470. 6 k 0.01 0.01 4.150375 4.150375 7 ra -0.0001 -0.0018941 -0.0001 -0.0009338 Differential equations 1 d(V)/d(X) = -Fa0 / ra Explicit equations 1 Ca0 = .1 2 Fa0 = .2 11-6 3 T = 300 + 200 * X 4 k = .01*exp((10000 / 2) * (1 / 300 - 1 / T)) 5 ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2) V = 308.2917dm3 For the CSTR, X = .85, T = 300+(200)(85) = 470 K. k = 4.31 (Using T = 470K in the formula). -rA = .000971 mol/dm3/s FA0 X V rA .1 2 .85 175 dm3 -4 9.71 10 The reason for this difference is that the temperature and hence the rate of reaction remains constant throughout the entire CSTR (equal to the outlet conditions), while for a PFR, the rate increases gradually with temperature from the inlet to the outlet, so the rate of increases with length. P11-3 (b) T T0 X[ HR ] i CPi For boiling temp of 550 k, 550 = T0 + 200 T0 = 350K P11-3 (c) P11-3 (d) FA0 X rA VCSTR VCSTR ( rA ) FA0 X For V = 500 dm3, FA0=.2 rA T k C A2 0 (1 X ) 2 300 200 X .01 k (1 X )2 Now use Polymath to solve the non-linear equations. 11-7 See Polymath program P11-3-d-1.pol. Calculated values of NLE variables Variable Value f(x) Initial Guess 0 480. 1 T 484.4136 2 X 0.9220681 -2.041E-09 0.9 Variable Value 1 k 6.072856 2 ra 0.0003688 Nonlinear equations 1 f(T) = 300 + 200 * X - T = 0 2 f(X) = 500 - .2 * X / ra = 0 Explicit equations 1 k = .01 * exp(10000 / 1.98 * (1 / 300 - 1 / T)) 2 ra = 0.01 * k * (1 - X) ^ 2 Hence, X = .922 and T = 484.41 K For the conversion in two CSTR’s of 250 dm3 each, For the first CSTR, using the earlier program and V = 250 dm3, Calculated values of NLE variables Variable Value f(x) Initial Guess 1 T 476.482 1.137E-13 480. 2 X 0.88241 -5.803E-09 0.9 Variable Value 1 k 5.105278 2 ra 0.0007059 Nonlinear equations 1 f(T) = 300 + 200 * X - T = 0 2 f(X) = 250 - .2 * X / ra = 0 Explicit equations 1 k = .01 * exp(10000 / 1.98 * (1 / 300 - 1 / T)) 2 ra = 0.01 * k * (1 - X) ^ 2 T = 476.48 ad X = .8824 Hence, in the second reactor, 11-8 VCSTR X T FA0 ( X X 1 ) rA VCSTR ( rA ) X 1 FA0 Tout ,CSTR1 200( X X1 ) See Polymath program P11-3-d-2.pol. Calculated values of NLE variables Variable Value f(x) Initial Guess 0 480. 1 T 493.8738 2 X 0.9693688 -1.359E-09 0.8824 Variable Value 1 k 7.415252 2 ra 6.958E-05 3 X1 0.8824 Nonlinear equations 1 f(T) = 476.48 + 200 * (X - X1) - T = 0 2 f(X) = 250 - .2 * (X - X1) / ra = 0 Explicit equations 1 k = .01 * exp(10000 / 1.98 * (1 / 300 - 1 / T)) 2 ra = 0.01 * k * (1 - X) ^ 2 3 X1 = .8824 Hence, final X = .9694 P11-3 (e) Individualized solution P11-3 (f) Individualized solution 11-9 P11-4 (a) 11-10 P11-4 (b) P11-4 (c) Individualized solution P11-4 (d) 11-11 11-12 11-13 P11-5 (a) A B C CA CT I FA FT FI FA CT C A CI FT FA FI C A01 C A 0 CI 0 C A01 C A 0 CI 0 1 I FA0 FA0 FI 0 P11-5 (b) Mole balance: dX dV rA FA0 Rate law: rA kC A Stoichiometry: C A C A01 1 X T0 1 X T y A0 1 1 1 1 11-14 FA0 FT 0 1 y A0 1 T FA0 FA0 1 Fi 0 1 CPA i i i X H RX CPA i CPi T0 CPi Enter these equations into Polymath See Polymath program P11-5-b.pol. POLYMATH Results Calculated values of the DEQ variables Variable V X Cao Cio theta Fao Cao1 e To dHrx Cpa Cpi T k ra initial value 0 0 0.0221729 0.0221729 100 10 4.391E-04 0.009901 1100 8.0E+04 170 200 1100 25.256686 -0.0110894 minimal value 0 0 0.0221729 0.0221729 100 10 4.391E-04 0.009901 1100 8.0E+04 170 200 1098.3458 24.100568 -0.0110894 maximal value 500 0.417064 0.0221729 0.0221729 100 10 4.391E-04 0.009901 1100 8.0E+04 170 200 1100 25.256686 -0.0061524 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra/Fao Explicit equations as entered by the user [1] Cao = 2/(.082*1100) [2] Cio = Cao [3] theta = 100 [4] Fao = 10 [5] Cao1 = (Cao+Cio)/(theta+1) [6] e = 1/(1+theta) [7] To = 1100 [8] dHrx = 80000 [9] Cpa = 170 [10] Cpi = 200 [11] T = (X*(-dHrx)+(Cpa+theta*Cpi)*To)/(Cpa+theta*Cpi) [12] k = exp(34.34-34222/T) [13] ra = -k*Cao1*(1-X)*To/(1+e*X)/T 11-15 final value 500 0.417064 0.0221729 0.0221729 100 10 4.391E-04 0.009901 1100 8.0E+04 170 200 1098.3458 24.100568 -0.0061524 P11-5 (c) There is a maximum at θ = 8. This is because when θ is small, adding inerts keeps the temperature low to favor the endothermic reaction. As θ increases beyond 8, there is so much more inert than reactants that the rate law becomes the limiting factor. P11-5 (d) The only change to the Polymath code from part (b) is that the heat of reaction changes sign. The new code is not shown, but the plots are below. See Polymath program P11-5-d.pol. 11-16 The maximum conversion occurs at low values of theta (θ < 8) because the reaction is now exothermic. This means heat is generated during the reaction and there is no advantage to adding inerts as there was in the endothermic case. P11-5 (e) We need to alter the equations from part (c) such that rA kC A2 and CA0 = 1 A plot of conversion versus theta shows a maximum at about θ = 5. See Polymath program P11-5-e.pol. P11-5 (f) We need to alter the equations from part (c) such that We already know that C A C A0 rA k CA CB CC KC 1 X T0 . Now weed need expressions for CB and CC. From 1 X T stoichiometry we can see that CB = CC. In terms of CA0 we find that: CB CC C A0 X 1 T0 X T We also need an equation for KC: K C KC1 exp H RX 1 R T1 1 T 2 exp 80000 1 1 8.314 1100 T When we enter these into Polymath we find that the maximum conversion is achieved at approximately θ = 8. See Polymath program P11-5-f.pol. 11-17 P11-5 (g) See Polymath program P11-5-g.pol. P11-6 (a) Adiabatic Mole Balance (1) Rate Law Stoichiometry dX dW W rA FA0 bV dX dV rA B FA0 rA FA0 (2) rA k CA (3) k k 1 exp (4) KC KC2 exp (5) CA CA0 1 X y T0 T (6) CB CA0Xy T0 T CB KC E 1 R T1 11-18 1 T H Rx 1 R T2 1 T dy FT T dW y FT 0 T0 W V dy b T dV 2y T0 Parameters (7) – (15) T 2y T0 FA0, k1, E, R, T1, KC2, H Rx , T2, CA0 , T0 , , b Energy Balance CP Adiabatic and (16A) 0 H Rx X iC Pi T T0 Additional Parameters (17A) & (17B) T0 , dT dV rA FiCPi FA0 Heat Exchange (16B) dT dV rA i C Pi C PA I C PI H Rx Ua T Ta FiCPi iCPi H Rx FA0 11-19 CP X , if CP Ua T Ta iC Pi 0 then (a) Adiabatic 11-20 Adiabatic 11-21 P11-7 (a) Mole Balance (1) dX dW rA rA FA 0 k C AC B Rate Law (2) Rate Law (3) k Rate Law (4) k 1 0.0002 Rate Law (5) T1 Rate Law (6) E 25,000 k 1 exp E 1 R T1 CC2 KC 1 T 310 11-22 KC K C 2 exp H Rx 1 R T2 1 T Rate Law (7) Rate Law (8) H Rx Rate Law (9) T2 Rate Law (10) K C2 1,000 KC 1000exp 20,000 305 20,000 1 1.987 305 1 T 2 1 1 0 y A0 Stoichiometry (11) CA 0.5 2 1 1 CA0 1 X y B Stoichiometry (12) Stoichiometry (13) Stoichiometry (14) Stoichiometry (15) 2 C B C A0 2 X CC T 2y T0 = 0.00015 11-23 T0 y T T 2CA 0X 0 y T dy dW (b) T0 T 0 rA k C A0 1 X y T0 T C A0 2 X y rA kC 2A0 KC 4C 2A0 X 2e C 2A0 1 X e 2 X e T 4X 2 1 X 2 X 2C A0 Xy T0 KC T0 T KC y T0 2 T (c) Equilibrium Conversion X 2e 1 Xe 2 Xe KC 4 2 KC 4 3K C Xe 4 KC 1 X 2e 4 Equilibrium Conversion (19) Xe 3KC 4 3KC 4 2 Xe X 2e 3K C K Xe 2 C 4 4 2 KC 4 Xe K C X 2e 4 2KC KC 4 0 1 1 T X W W Section 1.01 Case 1 Adiabatic 11-24 2 (d) Energy Balance (16) Energy Balance (17) T H Rx X T0 iC Pi T0 = 325 H Rx CP 2C PC HR C PA C P T TR C PB CP i C Pi C PA 20 2 20 Energy Balance (e) iC Pi (18) T T0 H Rx X i C Pi 11-25 2 20 20 20 0 0 B C PB C C PC 0 20 I C PI Everything that enters 1 40 100 cal mol K 400 20,000X 100 400 200X (f) Adiabatic 11-26 0 Adiabatic Gas Phase Adiabatic 11-27 Gas Phase Adiabatic 11-28 P11-8 1 Xe 2 KC Xe T X e2 CC CD C AC B KC 1 T0 KC HR X CPA CPB 30000 X 25 25 300 300 600 X See Polymath program P11-8.pol. Calculated values of NLE variables Variable Value 1 Xe f(x) Initial Guess 0.9997644 3.518E-11 0.5 ( 0 < Xe < 1. ) Variable Value 1 T 300. 2 Kc 1.8E+07 Nonlinear equations 1 f(Xe) = Xe - (1 - Xe) * Kc ^ 0.5 = 0 Explicit equations 1 T = 300 2 Kc = 500000 * exp(-30000 / 1.987 * (1 / 323 - 1 / T)) T X 300 1 320 0.999 340 0.995 360 0.984 380 0.935 400 0.887 420 0.76 440 0.585 460 0.4 480 0.26 500 0.1529 520 0.091 540 0.035 560 0.035 11-29 Xe 1 Xe (Eqm Conversion) 0.9 0.8 0.7 0.6 Xe 0.5 0.4 0.3 0.2 0.1 0 300 350 400 450 500 550 Temp (K) P11-9 For first reactor, KC X e1 or X e1 1 X e1 KC 1 KC For second reactor KC X e2 orX e 2 1 X e2 B2 KC B2 1 KC For 3rd reactor KC X e3 orX e3 1 X e3 B3 KC B3 1 KC 1st reactor: in first reaction Xe = 0.3 So, FB = FA01(.3) 2nd reactor: Moles of A entering the 2nd reactor: FA02 = 2FA01 - FA01(.3) = 1.7FA01 B2 .2 FA01 1.7 FA0 .12 FA02 CPi i T T0 X C pA B FA02 X HR 0 C pB T T 0 HR Slope is now negative 3rd reactor: 11-30 X e2 = 0.3 Say B (.2 FA01 ) .3FA02 FA01 (.2 .3 1.8) FA03 FA01 FA02 (1 X e 2 ) FA03 2.26 FA01 FA01 1.8 FA01 (1 X e 2 ) 1 1.8(1 .3) FA01 Feed to the reactor 3: (2 FA01 ) .3FA02 B3 FA01 (.2 .3 1.8) 0.7FA01 .74 2.26 Feed Temperature to the reactor 2 is (520+450)/2 = 485 K Feed Temperature to reactor 3 is 480 K Xfinal = .4 Moles of B = .2FA01 + .3FAo2 + .4FA03 = FA01(.2 + .54 + (.4)(2.26)) = 1.64 FA01 X = FB/3FA01 = .54 P11-9 (b) The same setup and equations can be used as in part (a). The entering temperature for reactor 1 is now 450 K and the outlet is 520 K. When the two streams are joined prior to entering reactor 2 the temperature is (520+450)/2 = 485 K Say that the outlet temperature for reactor 2 is 510 K. Then the entering temperature for reactor 3 would be (510+510+450)/3 = 490 K For any reactor j, FA0 j CPi i T T0 X C pA B FA0 j X HR 0 C pB T T 0 HR and θB for reactor 1 = 0. For reactor 2, θB > 0. This means that the slope of the conversion line from the energy balance is larger for reactor 2 than reactor 1. And similarly θB for reactor 3 > θB for reactor 2. So the line for conversion in reactor 3 will be steeper than that of reactor 2. The mass balance equations are the same as in part (b) and so the plot of equilibrium conversion will decrease from reactor 1 to reactor 2, and, likewise, from reactor 2 to reactor 3. 11-31 P11-10 1) The standard heat of reaction should have been -10000 cal/mol instead of -5000 cal/mol 2) While calculating CP 1 CP 2 B CP for the reaction, the following expression should have been employed: 1 CP CPA 2 C The Cp of inerts should not have appeared in the CP . 3) In the equation for the variation of T with conversion terms , the following should have been used, T 0 X ( H Rx (TR )) X CPTR i T T CPi i CPi T X CP X (10000) X ( 9)(298) 33*300 33 X ( 9) 7318 X 9900 33 9 X 11-32 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. 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All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 12-1 Solutions for Chapter 12: Steady State Non-isothermal Reactor Design- Flow Reactors with Heat Exchange P12-1 Individualized solution P12-2(a) (1) Part (a) Co-current See polymath program P12-2-a(1).pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca0 9.3 9.3 9.3 9.3 2 Cp0 159. 159. 159. 159. 3 Cpc 28. 28. 28. 28. 4 deltaH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 5 Fa0 14.67 14.67 14.67 14.67 6 k 0.5927441 0.5927441 654.8375 3.449562 7 Kc 1817.59 215.5325 1817.59 1063.552 8 m 500. 500. 500. 500. 9 Qg 1.103E+05 0.1990791 1.448E+06 0.1990791 10 Qr -2.5E+04 -2.5E+04 5.301E+05 5.445171 11 ra -5.51252 -72.4152 -9.954E-06 -9.954E-06 12 rate 5.51252 9.954E-06 72.4152 9.954E-06 13 T 305. 305. 417.9988 327.2341 14 Ta 310. 309.9439 327.233 327.233 15 Ua 5000. 5000. 5000. 5000. 16 V 0 0 5. 5. 17 X 0 0 0.9990603 0.9990603 18 Xe 0.9994501 0.9953818 0.9994501 0.9990606 Differential equations 1 d(Ta)/d(V) = Ua*(T-Ta)/m/Cpc 2 d(T)/d(V) = ((ra*deltaH)-Ua*(T-Ta))/Cp0/Fa0 3 d(X)/d(V) = -ra/Fa0 12-2 Explicit equations 1 Cpc = 28 2 Ua = 5000 3 k = 31.1*exp(7906*(T-360)/(T*360)) 4 Cp0 = 159 5 deltaH = -20000 6 Ca0 = 9.3 7 Kc = 1000*exp(-(20000/8.314)*((T-330)/(T*330))) 8 ra = -k*Ca0*(1-(1+1/Kc)*X) 9 Xe = Kc/(1+Kc) 10 Fa0 = .9*163*.1 11 rate = -ra 12 m = 500 13 Qg = ra*deltaH 14 Qr = Ua*(T-Ta) Plot of X versus V Plot of Ta versus V 12-3 Plot of T versus V Part (b) Counter current First multiply the right hand side of equation (E12-1.2) with by minus one to obtain; d(Ta)/d(V) = - Ua*(T-Ta)/m/Cpc 12-4 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca0 9.3 9.3 9.3 9.3 2 Cp0 159. 159. 159. 159. 3 Cpc 28. 28. 28. 28. 4 deltaH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 5 Fa0 14.67 14.67 14.67 14.67 6 k 0.5927441 0.1050316 640.6661 0.1050316 7 Kc 1817.59 216.9721 3077.31 3077.31 8 m 500. 500. 500. 500. 9 ra -5.51252 -73.92857 -0.000591 -0.000591 10 rate 5.51252 0.000591 73.92857 0.000591 11 T 305. 285.9125 417.5158 285.9125 12 Ta 310. 285.8822 310.0614 285.8822 13 Ua 5000. 5000. 5000. 5000. 14 V 0 0 5. 5. 15 X 0 0 0.9990703 0.9990703 16 Xe 0.9994501 0.9954123 0.9996751 0.9996751 Differential equations 1 d(Ta)/d(V) = -Ua*(T-Ta)/m/Cpc 2 d(T)/d(V) = ((ra*deltaH)-Ua*(T-Ta))/Cp0/Fa0 3 d(X)/d(V) = -ra/Fa0 Explicit equations 1 Cpc = 28 2 Ua = 5000 3 k = 31.1*exp(7906*(T-360)/(T*360)) 4 Cp0 = 159 5 deltaH = -20000 6 Ca0 = 9.3 7 Kc = 1000*exp(-(20000/8.314)*((T-330)/(T*330))) 8 ra = -k*Ca0*(1-(1+1/Kc)*X) 9 Xe = Kc/(1+Kc) 10 Fa0 = .9*163*.1 12-5 11 rate = -ra 12 m = 500 Plot of X versus V Plot of T versus V Plot of Ta versus V 12-6 Part (c) Constant Ta For constant Ta, we have to use Polymath program (a) but multiply the right hand side of E12-1.1 by 0 in the program; i.e d(Ta)/d(V) = Ua*(T-Ta)/m/Cpc *0 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca0 9.3 9.3 9.3 9.3 2 Cp0 159. 159. 159. 159. 3 Cpc 28. 28. 28. 28. 4 deltaH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 5 Fa0 14.67 14.67 14.67 14.67 6 k 0.5927441 0.5927441 648.9771 0.9009882 7 Kc 1817.59 216.1228 1817.59 1600.16 8 m 500. 500. 500. 500. 9 ra -5.51252 -72.24709 -0.000498 -0.000498 10 rate 5.51252 0.000498 72.24709 0.000498 11 T 305. 305. 417.8002 310.0078 12 Ta 310. 310. 310. 310. 13 Ua 5000. 5000. 5000. 5000. 12-7 14 V 0 0 5. 5. 15 X 0 0 0.9993161 0.9993161 16 Xe 0.9994501 0.9953943 0.9994501 0.9993755 Differential equations 1 d(Ta)/d(V) = -Ua*(T-Ta)/m/Cpc *0 2 d(T)/d(V) = ((ra*deltaH)-Ua*(T-Ta))/Cp0/Fa0 3 d(X)/d(V) = -ra/Fa0 Explicit equations 1 Cpc = 28 2 Ua = 5000 3 k = 31.1*exp(7906*(T-360)/(T*360)) 4 Cp0 = 159 5 deltaH = -20000 6 Ca0 = 9.3 7 Kc = 1000*exp(-(20000/8.314)*((T-330)/(T*330))) 8 ra = -k*Ca0*(1-(1+1/Kc)*X) 9 Xe = Kc/(1+Kc) 10 Fa0 = .9*163*.1 11 rate = -ra 12 m = 500 Plot of X versus V 12-8 Plot of T versus V Plot of Ta versus V Ta will remain constant with V Part (d) Adiabatic Using the polymath program of part (a) and making the parameter Ua =0; we have; 12-9 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca0 9.3 9.3 9.3 9.3 2 Cp0 159. 159. 159. 159. 3 Cpc 28. 28. 28. 28. 4 deltaH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 5 Fa0 14.67 14.67 14.67 14.67 6 k 0.5927441 0.5927441 1115.107 1115.105 7 Kc 1817.59 183.3032 1817.59 183.3033 8 m 500. 500. 500. 500. 9 ra -5.51252 -265.5745 0.0023739 -4.937E-05 10 rate 5.51252 -0.0023739 265.5745 4.937E-05 11 T 305. 305. 430.1037 430.1037 12 Ta 310. 310. 310. 310. 13 Ua 0 0 0 0 14 V 0 0 5. 5. 15 X 0 0 0.9945744 0.9945742 16 Xe 0.9994501 0.9945742 0.9994501 0.9945742 Differential equations 1 d(Ta)/d(V) = -Ua*(T-Ta)/m/Cpc *0 2 d(T)/d(V) = ((ra*deltaH)-Ua*(T-Ta))/Cp0/Fa0 3 d(X)/d(V) = -ra/Fa0 Explicit equations 1 Cpc = 28 2 Ua = 5000*0 3 k = 31.1*exp(7906*(T-360)/(T*360)) 4 Cp0 = 159 5 deltaH = -20000 6 Ca0 = 9.3 7 Kc = 1000*exp(-(20000/8.314)*((T-330)/(T*330))) 8 ra = -k*Ca0*(1-(1+1/Kc)*X) 9 Xe = Kc/(1+Kc) 10 Fa0 = .9*163*.1 12-10 11 rate = -ra 12 m = 500 Plot of X versus V; Plot of T versus V Plot of Ta versus V; 12-11 Ta remains a constant (2) Since the temperature reaches a maximum which is above 400K in all of the above systems at some point during the operation thus they cannot prevent reaching the 400 K temperatures which will start of another exothermic reaction. Hence the heat exchanger needs to be changed in order that the heat removed by the exchanger is such that the maximum temperature in the reactor does not go above 400K at any point during the operation. (3) Making the necessary changes in the polymath code and adding variables Qg and Qr as asked for in the problem we plot them for a co-current exchanger as follows: 12-12 For counter current heat exchanger we have For constant Ta; For adiabatic operation; 12-13 (4) Varying the values of m (i) when m =0; a plot of Qg and Qr versus volume is as follows, this seems to be an unsafe operating condition because generated heat is not taken out at the same time. (ii) when m =2000; 12-14 In this case the conditions are safer than for m=500 and the heat generated is simultaneously removed. Variation of entering feed temperature: (i) Keeping other conditions constant we change value of T0 only now. Let T0 = 273K then, 12-15 Plot of Qg and Qr versus V is as follows; (ii) T0 = 315K; Plot of Qg and Qr versus V is as follows; Since again the heat generation term, Qg is much larger than Qr thus an unsafe operating condition can result in this condition. 12-16 (5) An unsafe condition will result if the entering coolant temperature is made Ta(0) = 300K in a concurrent heat exchanger ;resulting in great amount of heat generation compared to the rate of heat removal. The plot of Qg and Qr with V is as shown; Similarly other unsafe operating conditions can be found out keeping in view that the heat generated during the course of the reaction, is not removed efficiently by the exchanger such that there is a wide difference between the two terms at any position in the reactor. P12-2(b) (1) The terms Qg = ra*△HRx and Qr = Ua*(T-Ta) are added in the polymath code given in example 12.2. See polymath program P12.2-b(1) Case1: adiabatic operation Qr=0 in this case 12-17 Case 2 : For constant heat exchange conditions Case 3: Co-current heat exchange 12-18 Case 4 : counter current heat exchange : We need to guess a value of Ta such that at exit Ta = 1250K If we take Ta(0) = 995.15K then this can be done. (2) Now, V = 0.5 m3 T0 = 1050 K Ta0 = 1250K Case 1: adiabatic operation; Substitute; Ua = 0 in the polymath code 12-19 (3) Substitute, the volume V= 5 m3 in the polymath code and get the results. (4) Plot of Qg for all 4 cases against volume Plot of Qr versus volume for all cases Plot of -ra (rate) versus V 12-20 It can be seen that the rate for constant heat exchange fluid temperature Ta , is higher than the rest of cases because the difference beween heat generated and heat removed in this case is highest. The rate of reaction for all cases is decreasing because the temperature of the system is decreasing with volume. The rate of reaction for counter-current heat exchanger system is a U shaped curve plotted against volume. At the front of the reactor, the reaction takes place very rapidly, drawing energy from the sensible heat of the gas causing the gas temperature to drop because the heat exchanger cannot supply energy at an equal or greater rate. This drop in temperature, coupled with the consumption of reactants, slows the reaction rate as we move down the reactor. (5) Introduction of inert will introduce a change in energy balance equation and the value of Ѳ1 as well. (6) (i) ѲI = 0 All the plots will remain as for part(1) ( ii ) ѲI = 1.5 Instead of the energy equation which was used previously 12-21 d (T ) = (Ua*(Ta-T)+ra* H)/(Fa0*(CpA+X*delCp)) the equation will change. d (V ) Now we have to change the value of i Cpi Now the value will be ∑Cp = ѲI*CpI + CpA = 1.5×50 + 1×163 = 238 Value of Ѳ will change as well FX 0 FX 1 (1.5C A0 2C A0 ) (1.5C A0 Ѳ= = FX 0 (1.5C A0 C A0 ) C A0 ) 1 2.5 0.4 (iii) Ѳ I = 3 ∑Cp = ѲI*CpI + CpA = 3×50 + 1×163 = 313J/molA/K FX 0 FX 1 Ѳ= FX 0 (3CA0 2C A0 ) (3C A0 C A0 ) 1 0.25 = (3CA0 C A0 ) 4 Incorporating these changes in the code and plotting X versus V for different cases. See polymath code P12-2-b(6). The analysis is as follows: Case I: adiabatic operation: 12-22 Case2: Constant heat exchange fluid temperature Ta Case 3: Co-current heat exchange The polymath program for reference is for the case of co-current heat exchange with ѲI =3. By changing values of ∑Cp and ε variables as shown we can change the program for various cases and sub cases. 12-23 Case 4: Countercurrent heat exchange Remarks: Thus we can see that for all cases when inert gas concentration is more then the reaction proceeds faster but then the overall yield is less as well. In the case of adiabatic operation this phenomenon is very significant . In case of constant heat exchange fluid temperature the effect of inert gas is negligible. (7) Here we will change the polymath program as entered in P12-2(b) part1. The Ta value will be changed and the program will be tested for following values of Ta. 1000K, 1175K, 1350K Case 1: adiabatic conditions 12-24 Case 2: Constant heat exchange fluid temperature Ta Case 3: Co-current conditions 12-25 Case 4: Countercurrent conditions We need to enter Ta (V =0) values such that at V=Vf, Taf = 1000K, 1175K and 1350K respectively Ta ( V=0) (K) 983.75 992 999 Ta( V=V f) (K) 1000 1175 1350 (d) Example 12-3 (1) CA0 will decrease but this will have no effect 12-26 (2) Will decrease 401.1 ft 3 466.1 ft 3 s (3) In the energy balance the slope of the energy balance of X vs. T will be greater i CPC 35 18.65 18 4 501 1.67 19.5 35 335.7 130.2 BTU kmol R XM B XM, T Base case Change QM 12-27 Less Conversions P12-2 (e) Example 12-4 Change CP = 29 and –ΔH = 38700 POLYMATH Results NLES Solution Variable Value f(x) Ini Guess X 0.7109354 2.444E-11 0.367 T 593.6885 1.2E-09 564 tau 0.1229 A 1.696E+13 E 3.24E+04 R 1.987 k 20.01167 NLES Report (safenewt) Nonlinear equations [1] f(X) = X-(397.3*(T-535)+92.9*(T-545))/(38700+7*(T-528)) = 0 [2] f(T) = X-tau*k/(1+tau*k) = 0 Explicit equations [1] tau = 0.1229 [2] A = 16.96*10^12 [3] E = 32400 [4] R = 1.987 [5] k = A*exp(-E/(R*T)) Vary the heat exchanger area to find the effect on conversion. 12-28 P12-2 (f) (1) Example 12-5 See Polymath program P12-2-f.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 1.05 1.05 1.05 1.05 2 Ca 0.1 1.306E-07 0.1 1.306E-07 3 Cb 0 0 0.0208092 8.93E-07 4 Cc 0 0 0.0038445 1.739E-07 5 Cto 0.1 0.1 0.1 0.1 6 Fa 100. 9.521981 100. 9.521981 7 Fb 0 0 65.11707 65.11707 8 Fc 0 0 12.68047 12.68047 9 Ft 100. 87.31953 100. 87.31953 10 Fto 100. 100. 100. 100. 11 k1a 482.8247 482.8247 1.753E+04 1.706E+04 12 k2a 553.0557 553.0557 1.79E+06 1.683E+06 13 r1a -48.28247 -136.5345 -0.0022276 -0.0022276 14 r2a -5.530557 -90.93151 -2.87E-08 -2.87E-08 15 T 423. 423. 682.1122 678.9481 16 To 423. 423. 423. 423. 17 V 0 0 0.8 0.8 18 y 1. 1.922E-05 1. 1.922E-05 Differential equations 1 d(Fa)/d(V) = r1a+r2a 2 d(Fb)/d(V) = -r1a 3 d(Fc)/d(V) = -r2a/2 4 d(T)/d(V) = (4000*(373-T)+(-r1a)*20000+(-r2a)*60000)/(90*Fa+90*Fb+180*Fc) 5 d(y)/d(V) = -alpha/(2*y)*(Ft/Fto)*(T/To) Explicit equations 1 k1a = 10*exp(4000*(1/300-1/T)) 2 k2a = 0.09*exp(9000*(1/300-1/T)) 3 Cto = 0.1 4 Ft = Fa+Fb+Fc 5 To = 423 6 Ca = Cto*(Fa/Ft)*(To/T)*y 7 Cb = Cto*(Fb/Ft)*(To/T)*y 8 Cc = Cto*(Fc/Ft)*(To/T)*y 12-29 9 r1a = -k1a*Ca 10 r2a = -k2a*Ca^2 11 Fto = 100 12 alpha = 1.05 (f) (2) In the polymath program of part (f) (1), rate equation will be changed like – r1a = -k1a*(Ca-Cb/Kc) with Kc= 10*exp(20000*(1/450-1/T)) 12-30 P12-2(g) See Polymath program P12-2-g.pol. Entering Temperature (T0 in K) Reactor temperatures (Ts in K) 1. 200 250 2. 220 265, 625 3. 244 275, 563, 644 4. 261 292, 409, 571, 661 12-31 5. 283 310, 363, 449, 558, 677 6. 292 373, 463, 562, 674 7. 304 475, 551, 686 8. 338 518, 713 9. 350 720 Plot of steady state reactor temperature; Ts(Y axis) versus T0 (X axis) The extinction temperature is 220 K and the ignition temperature is 338K. Vary UA UA 4000 J m3 s K No steady state occurs in this case and G (T) is always more than R (T). UA 40, 000 J m3 s K five steady states will exist here T = 310, 363K, 449K ,558K and 677 depending how you read the intersection on the graph. UA 4, 00, 000 J m3 s K Only one steady states occurs at around T = 350K (about). Vary 0.001 Only the lower steady state exists at about T = 316 K 0.01 ; A number of steady states occur; 5 steady states occur 12-32 0.1, Only an upper steady state occurs at 678K. Thus we see that if we go on increasing the value of residence time, firstly the number of steady states will increase and then it will start decreasing. P12-2(h) Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 V 0 0 10. 10. 2 Fa 5. 0.3455356 5. 0.3455356 3 Fb 10. 0.7169561 10. 0.7169561 4 Fc 0 0 4.62858 4.62858 5 Fd 0 0 0.0258848 0.0258848 6 T 300. 300. 914.7896 518.2818 7 Ta 325. 322.7616 506.8902 506.8902 8 E2 1.2E+04 1.2E+04 1.2E+04 1.2E+04 9 y 1. 1. 1. 1. 10 R 1.987 1.987 1.987 1.987 11 Ft 15. 5.716956 15. 5.716956 12 To 310. 310. 310. 310. 13 k2c 2. 2. 1.511E+06 9619.448 14 E1 8000. 8000. 8000. 8000. 15 Cto 0.2 0.2 0.2 0.2 16 Ca 0.0688889 0.0072303 0.0688889 0.0072303 17 Cc 0 0 0.096852 0.096852 18 r2c 0 -0.0081056 0 -0.0004569 19 Cpco 10. 10. 10. 10. 20 m 50. 50. 50. 50. 21 Cb 0.1377778 0.0150021 0.1377778 0.0150021 22 k1a 40. 3.318E+05 1.14E+04 23 r1a -0.0523079 -3.727241 -0.0185467 -0.0185467 24 r1b -0.1046159 -7.454481 -0.0370935 -0.0370935 25 rb -0.1046159 -7.454481 -0.0370935 -0.0370935 26 r2a 0 -0.0081056 0 -0.0004569 27 DH1b -1.5E+04 -1.5E+04 -1.5E+04 -1.5E+04 28 DH2a -10000. -10000. -10000. -10000. 40. 12-33 29 r1c 0.0523079 0.0185467 3.727241 0.0185467 30 Ta55 325. 325. 325. 325. 31 Cpd 16. 16. 16. 16. 32 Cpa 10. 10. 10. 10. 33 Cpb 12. 12. 12. 12. 34 Cpc 14. 14. 14. 14. 77.2731 170. 77.2731 35 sumFiCpi 170. 36 rc 0.0523079 0.0180899 3.725968 0.0180899 37 Ua 80. 80. 80. 80. 38 r2d 0 0 0.0162112 0.0009137 39 ra -0.0523079 -3.728513 -0.0190036 -0.0190036 40 rd 0 0 0.0162112 0.0009137 41 Qg 1569.238 560.9706 1.118E+05 560.9706 42 Qr -2000. -2000. 4.139E+04 911.3246 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(T)/d(V) = (Qg - Qr) / sumFiCpi 6 d(Ta)/d(V) = Ua * (T - Ta) / m / Cpco Explicit equations 1 E2 = 12000 2 y=1 3 R = 1.987 4 Ft = Fa + Fb + Fc + Fd 5 To = 310 6 k2c = 2 * exp((E2 / R) * (1 / 300 - 1 / T)) 7 E1 = 8000 8 Cto = 0.2 9 Ca = Cto * (Fa / Ft) * (To / T) * y 10 Cc = Cto * (Fc / Ft) * (To / T) * y 11 r2c = -k2c * Ca ^ 2 * Cc ^ 3 12-34 12 Cpco = 10 13 m = 50 14 Cb = Cto * (Fb / Ft) * (To / T) * y 15 k1a = 40 * exp((E1 / R) * (1 / 300 - 1 / T)) 16 r1a = -k1a * Ca * Cb ^ 2 17 r1b = 2 * r1a 18 rb = r1b 19 r2a = r2c 20 DH1b = -15000 21 DH2a = -10000 22 r1c = -r1a 23 Ta55 = 325 24 Cpd = 16 25 Cpa = 10 26 Cpb = 12 27 Cpc = 14 28 sumFiCpi = Cpa * Fa + Cpb * Fb + Cpc * Fc + Cpd * Fd 29 rc = r1c + r2c 30 Ua = 80 31 r2d = -2 * r2c 32 ra = r1a + r2a 33 rd = r2d 34 Qg = r1b * DH1b + r2a * DH2a 35 Qr = Ua * (T - Ta) 12-35 Addition of Inerts: The adding of inerts will decrease the peak in the reactor temperature. By trial and error, an inert flow rate of 6.2 mol/min is seen to be sufficient to keep the reactor temperature below 700K. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 V 0 0 10. 10. 2 Fa 5. 0.4822244 5. 0.4822244 3 Fb 10. 0.9811024 10. 0.9811024 4 Fc 0 0 4.501122 4.501122 5 Fd 0 0 0.0166535 0.0166535 6 T 300. 300. 697.1199 570.593 7 Ta 325. 322.0417 477.6044 477.6044 8 E2 1.2E+04 1.2E+04 1.2E+04 1.2E+04 9 y 1. 1. 1. 1. 10 R 1.987 1.987 1.987 1.987 11 Ft 15. 5.981102 15. 5.981102 12 To 310. 310. 310. 310. 12-36 13 k2c 2. 2. 1.914E+05 2.8E+04 14 E1 8000. 8000. 8000. 8000. 15 Cto 0.2 0.2 0.2 0.2 16 Ca 0.0688889 0.0087606 0.0688889 0.0087606 17 Cc 0 0 0.081772 0.081772 18 r2c 0 -0.0040086 0 -0.0011748 19 Cpco 10. 10. 10. 10. 20 m 50. 50. 50. 50. 21 Cb 0.1377778 0.0178237 0.1377778 0.0178237 22 k1a 40. 8.369E+04 2.323E+04 23 r1a -0.0523079 -1.876998 -0.0523079 -0.0646601 24 r1b -0.1046159 -3.753997 -0.1046159 -0.1293201 25 rb -0.1046159 -3.753997 -0.1046159 -0.1293201 26 r2a 0 -0.0040086 0 -0.0011748 27 DH1b -1.5E+04 -1.5E+04 -1.5E+04 -1.5E+04 28 DH2a -10000. -10000. -10000. -10000. 29 r1c 0.0523079 0.0523079 1.876998 0.0646601 30 Ta55 325. 325. 325. 325. 31 Fi 6.2 6.2 6.2 6.2 32 Cpa 10. 10. 10. 10. 33 Cpb 12. 12. 12. 12. 34 Cpc 14. 14. 14. 14. 35 Cpd 16. 16. 16. 16. 36 rc 0.0523079 0.0523079 1.876239 0.0634852 37 Ua 80. 80. 80. 80. 38 r2d 0 0 0.0080172 0.0023497 39 ra -0.0523079 -1.877758 -0.0523079 -0.0658349 40 rd 0 0 0.0080172 0.0023497 41 Qg 1569.238 1569.238 5.632E+04 1951.55 42 Qr -2000. -2000. 2.358E+04 7439.087 43 Cpi 10. 10. 10. 10. 141.8776 232. 141.8776 44 sumFiCpi 232. 40. 12-37 Differential equations 1 d(Fa)/d(V) = ra 2 d(Fb)/d(V) = rb 3 d(Fc)/d(V) = rc 4 d(Fd)/d(V) = rd 5 d(T)/d(V) = (Qg - Qr) / sumFiCpi 6 d(Ta)/d(V) = Ua * (T - Ta) / m / Cpco Explicit equations 1 E2 = 12000 2 y=1 3 R = 1.987 4 Ft = Fa + Fb + Fc + Fd 5 To = 310 6 k2c = 2 * exp((E2 / R) * (1 / 300 - 1 / T)) 7 E1 = 8000 8 Cto = 0.2 9 Ca = Cto * (Fa / Ft) * (To / T) * y 10 Cc = Cto * (Fc / Ft) * (To / T) * y 11 r2c = -k2c * Ca ^ 2 * Cc ^ 3 12 Cpco = 10 13 m = 50 14 Cb = Cto * (Fb / Ft) * (To / T) * y 15 k1a = 40 * exp((E1 / R) * (1 / 300 - 1 / T)) 16 r1a = -k1a * Ca * Cb ^ 2 17 r1b = 2 * r1a 18 rb = r1b 19 r2a = r2c 20 DH1b = -15000 21 DH2a = -10000 22 r1c = -r1a 23 Ta55 = 325 24 Fi = 6.2 12-38 25 Cpa = 10 26 Cpb = 12 27 Cpc = 14 28 Cpd = 16 29 rc = r1c + r2c 30 Ua = 80 31 r2d = -2 * r2c 32 ra = r1a + r2a 33 rd = r2d 34 Qg = r1b * DH1b + r2a * DH2a 35 Qr = Ua * (T - Ta) 36 Cpi = 10 37 sumFiCpi = Cpa * Fa + Cpb * Fb + Cpc * Fc + Cpd * Fd + Cpi * Fi P12-2 (i) CD Example CDR12.4-1 ~ 2 1 dP1 P01 dP2 P0 2 1 dP P0 1 1 12 2 1 12-39 No effect for turbulent flow if both dP and P changed at the same time. P12-3 T (K) (a) 390 380 370 360 350 340 330 320 310 Fao = 8 mol/s Fao = 5 mol/s Fao = 1 mol/s 0 1000 2000 3000 4000 5000 X W (g) 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 Fao = 8 mol/s Fao = 5 mol/s Fao = 1 mol/s 0 1000 2000 3000 4000 5000 W (g) 1 Xe 0.8 Fao = 8 mol/s 0.6 Fao = 5 mol/s 0.4 Fao = 1 mol/s 0.2 0 0 1000 2000 3000 4000 5000 W (g) When the flowrate of A is large (high Fao), the reactants spend less time in the reactor. That is, the residence time is short, so the exit conversion is small. At small Fao, the residence time is long, so the exit conversion is large. Notice that at low Fao, the conversion reaches equilibrium conversion, while at high Fao, the conversion does not reach equilibrium conversion. 12-40 (b) 420 T (K) 400 380 thetaI = 4 360 thetaI = 1 340 thetaI = 0.5 320 300 0 1000 2000 3000 4000 5000 W (g) 0.6 X 0.5 0.4 thetaI = 4 0.3 thetaI = 1 0.2 thetaI = 0.5 0.1 0 0 1000 2000 3000 4000 5000 W (g) 1 Xe 0.8 thetaI = 4 0.6 thetaI = 1 0.4 thetaI = 0.5 0.2 0 0 1000 2000 3000 4000 5000 W (g) As the fraction of inerts in the entering stream increases, the concentration of A in the entering stream decreases. Low concentration of A slower reaction rate lower conversion and less heat evolved by the reaction (that is, lower temperature in the reactor). (c) 12-41 T (K) 400 380 Ua/rho = 0.1 cal/kg/s/K 360 340 Ua/rho = 0.5 cal/kg/s/K 320 Ua/rho = 0.8 cal/kg/s/K 300 0 1000 2000 3000 4000 5000 W (g) 0.6 0.5 Ua/rho = 0.1 cal/kg/s/K X 0.4 Ua/rho = 0.5 cal/kg/s/K 0.3 0.2 Ua/rho = 0.8 cal/kg/s/K 0.1 0 0 1000 2000 3000 4000 5000 W (g) Xe 1 0.8 Ua/rho = 0.1 cal/kg/s/K 0.6 0.4 Ua/rho = 0.5 cal/kg/s/K 0.2 Ua/rho = 0.8 cal/kg/s/K 0 0 1000 2000 3000 4000 5000 W (g) A higher heat transfer coefficient means there is a faster rate of heat transfer from the reactor to the coolant. Thus, at high Ua the reactor temperature is low. The lower reactor temperature causes reaction rate to be slow, and thus lower conversion is observed. 12-42 (d) 420 T (K) 400 380 To = 310K 360 To = 330K 340 To = 350K 320 300 0 1000 2000 3000 4000 5000 W (g) 0.6 X 0.5 0.4 To = 310K 0.3 To = 330K 0.2 To = 350K 0.1 0 0 1000 2000 3000 4000 5000 W (g) 1 0.8 To = 310K 0.6 To = 330K 0.4 To = 350K 0.2 0 0 1000 2000 3000 4000 5000 A higher entrance temperature causes reaction rate to be fast, thus high conversion is observed. Conversely, a low entrance temperature causes reaction rate to be slow, thus a lower conversion is observed. 12-43 (e) 400 T (K) 380 Tao = 300K 360 Tao = 320K 340 Tao = 340K 320 300 0 1000 2000 3000 4000 5000 W (g) 0.6 X 0.5 0.4 Tao = 300K 0.3 Tao = 320K 0.2 Tao = 340K 0.1 0 0 1000 2000 3000 4000 5000 W (g) 1 Xe 0.8 Tao = 300K 0.6 Tao = 320K 0.4 Tao = 340K 0.2 0 0 1000 2000 3000 4000 5000 W (g) A lower coolant temperature results in lower reactor temperatures. Lower reactor temperatures result in lower reaction rate, thus lower conversion. (f) T0 = 350K 12-44 420 400 T (K) 380 mc = 50 g/s 360 mc = 1000 g/s 340 320 300 0 1000 2000 3000 4000 5000 W (g) 0.6 0.5 X 0.4 mc = 50 g/s 0.3 mc = 1000 g/s 0.2 0.1 0 0 1000 2000 3000 4000 5000 W (g) 1 Xe 0.8 0.6 mc = 50 g/s 0.4 mc = 1000 g/s 0.2 0 0 1000 2000 3000 4000 5000 W (g) With a higher coolant flowrate, the coolant can remove heat from the reactor at a faster rate. Thus, the temperature of the reactor will be lower with a higher coolant flowrate. Again, a lower reactor temperature causes slower reaction rate, which results in smaller conversion. (g) T0 = 350K 12-45 420 400 mc = 50 g/s (countercurrent) T (K) 380 360 mc = 1000 g/s (countercurrent) 340 320 300 0 2000 4000 6000 W (g) 0.6 0.5 mc = 50 g/s (countercurrent) X 0.4 0.3 mc = 1000 g/s (countercurrent) 0.2 0.1 0 0 2000 4000 6000 W (g) 1 Xe 0.8 0.6 mc = 50 g/s (countercurrent) 0.4 mc = 1000 g/s (countercurrent) 0.2 0 0 2000 4000 6000 W (g) The counter-current case is similar to the co-current case, except when mc=50 g/s, the temperature of the reactor is lower in the counter-current case. This is because, in general, counter-current heat exchange is more efficient than cocurrent heat exchange. (h) Fluidized bed CSTR Parameters: Weight of the bed : 5000 kg UA : 500 cal/s.k Ta : 320 K Density of bed : 2 Kg/m3 Rest all parameters are as specified in the base case. 12-46 Mole Balance: X MB W FAo rA' rA' CC2 ) KC k (C A C B CA CB C A0 1 X MB CC 2C A0 X MB T0 T T0 T W k C A0 1 X MB 2 T0 T 2C Ao X MB KC 2 X MB FA0 Solving this implicit equation will give X MB T Energy Balance: C P 0 and B I mc C Pc (Ta 1, C T ) 1 exp X EB T 0 UA mc C Pc 0 H Rx So we have X EB (T ) Equilibrium Conversion: At equilibrium, rA' C AC B CC2 KC C A0 1 X e Xe 0 2 2C A0 X e KC 2 K C0.5 K C0.5 2 12-47 FA 0 i C Pi (T Ti 0 ) 1.2 1 X 0.8 XMB 0.6 XEB 0.4 0.2 39 3 38 9 38 5 38 1 37 7 37 3 36 9 36 5 36 1 35 7 35 3 34 9 0 T Xe 0.7 0.6 X 0.5 0.4 Xe 0.3 0.2 0.1 39 3 38 9 38 5 38 1 37 7 37 3 36 9 36 5 36 1 35 7 35 3 34 9 0 T The intersection of mole balance and energy balance curve gives the conversion achieved in the reactor. Conversion achieved X = 0.438 Temperature = 369.7 K (Xe = 0.441) T (K) (i) Endothermic, varying Fao 332 330 328 326 324 322 320 318 316 Fao = 8 mol/s Fao = 5 mol/s Fao = 1 mol/s 0 1000 2000 3000 4000 5000 W (g) 12-48 0.12 X 0.1 0.08 Fao = 8 mol/s 0.06 Fao = 5 mol/s 0.04 Fao = 1 mol/s 0.02 0 0 1000 2000 3000 4000 5000 W (g) 0.2 0.15 Xe Fao = 8 mol/s 0.1 Fao = 5 mol/s Fao = 1 mol/s 0.05 0 0 1000 2000 3000 4000 5000 W (g) When the flowrate of A is large (high Fao), the reactants spend less time in the reactor. That is, the residence time is short, so the exit conversion is small. At small Fao, the residence time is long, so the exit conversion is large. Notice that at low Fao, the conversion reaches equilibrium conversion, while at high Fao, the conversion does not reach equilibrium conversion. Endothermic, varying thetaI 332 330 328 326 thetaI = 4 324 322 thetaI = 1 thetaI = 0.5 320 318 316 0 1000 2000 3000 4000 5000 12-49 0.08 0.07 0.06 0.05 thetaI = 4 0.04 0.03 thetaI = 1 thetaI = 0.5 0.02 0.01 0 0 1000 2000 3000 4000 5000 0.18 0.16 0.14 0.12 0.1 0.08 0.06 0.04 0.02 0 thetaI = 4 thetaI = 1 thetaI = 0.5 0 1000 2000 3000 4000 5000 As the fraction of inerts in the entering stream increases, the concentration of A in the entering stream decreases. Low concentration of A slower reaction rate lower conversion and less heat consumed by the reaction (that is, higher temperature in the reactor). Endothermic, varying To 355 350 345 340 335 330 325 320 315 310 305 To = 310K To = 330K To = 350K 0 1000 2000 3000 4000 5000 12-50 0.12 X 0.1 0.08 To = 310K 0.06 To = 330K 0.04 To = 350K 0.02 0 0 1000 2000 3000 4000 5000 Xe W (g) 0.35 0.3 0.25 0.2 0.15 0.1 0.05 0 To = 310K To = 330K To = 350K 0 1000 2000 3000 4000 5000 W (g) A higher entrance temperature causes reaction rate to be fast, thus high conversion is observed. Conversely, a low entrance temperature causes reaction rate to be slow, thus a lower conversion is observed. OVERALL: Exothermic reactions: -equilibrium conversion varies inversely with reactor temperature Exothermic reactions: -equilibrium conversion varies with reactor temperature Conversion approaches equilibrium conversion with: -a faster reaction rate (higher T or higher amount of reactants) -Notice in all the plots, a higher T causes X to approach Xe -a longer residence time P12-4 Solution is in the decoding algorithm available in the beginning of this manual 12-51 P12-5 (a) Individualized solution P12-5 (b) NH 4 NO3 2H 2O g A 2W g N 2O g Bg From Rate Data k ln 2 k1 E T2 T1 R T2T1 ln E R 50 E R 970 1020 2.912 0.307 44518 E 1 1 R 970 T k 0.307 exp Mole Balance FA0 X rA V k rAV FA 0 X MB M V V FA 0 kM FA0 Energy Balance FA0 H A0 FA0 H A0 FA0 W FW0 H W0 FA H A g H W0 FA0 1 X H A g H A g, T H Rx FW H W g FA0 HA 2H W g W FB H B g 2FA0 X H W g ,T H Vap HB g HA 0 FA0 XH B g 0 H Rx H A0 H A g W CPA T 660 HA ,T H W0 H W g 2H W g HB g HA H Vap X 0 0 H A0 XE 1 X H Vap CP T 660 W W HS 500 F H W 200 F C PS T 500 HS 500 F H W 200 F C PS T 500 H Rx 12-52 H Rx X W 0.17 0.83 FW FA 18 80 0.9103 BTU 80lb BTU 30.4 lb R mol lbmol R BTU 18lb BTU C PS 0.47 8.46 lb R mol lbmol R BTU 80lb BTU H Rx 336 26,880 lb mol lbmol BTU BTU H g 200 F 168 2,916 lb lbmol BTU BTU H W 500 F 1, 202 21,636 lb lbmol C PA 0.38 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cpa 30.4 30.4 30.4 30.4 2 Cps 8.46 8.46 8.46 8.46 3 delH -2.688E+04 -2.688E+04 -2.688E+04 -2.688E+04 4 Fao 257.3 257.3 257.3 257.3 5 Hg 2916. 2916. 2916. 2916. 6 Hw 2.164E+04 2.164E+04 2.164E+04 2.164E+04 7 k 0.307 0.307 0.7758943 0.7758943 8 M 500. 500. 500. 500. 9 Qg 1.604E+04 1.604E+04 4.053E+04 4.053E+04 10 Qr 2.654E+04 2.654E+04 2.73E+04 2.73E+04 11 t 0 0 20. 20. 12 T 970. 970. 990. 990. 13 thetaw 0.9103 0.9103 0.9103 0.9103 14 Xe 0.9874192 0.9874192 1.015768 1.015768 15 Xm 0.5965799 0.5965799 1.507762 1.507762 Differential equations 1 d(T)/d(t) = 1 Explicit equations 1 thetaw = 0.9103 2 Cpa = 30.4 3 Cps = 8.46 4 delH = -26880 5 k = 0.307*exp(44518*(1/970-1/T)) 6 M = 500 12-53 7 Fao = 310*0.83 8 Hw = 21636 9 Hg = 2916 10 Xm = k*M/Fao 11 Xe = Cpa*(T-660)/(-delH)+thetaw*(Hw-Hg+Cps*(T-960))/(-delH) 12 Qg = -delH*Xm 13 Qr = -delH*Xe The temperature prior to shutdown is 981.10 0R 12-54 P12-5 (c) Individualized solution P12-5 (d) Individualized solution P12-5 (e) Individualized solution P12-6 A B lb mole hr Tio(F) Fio 2C A B C 10 10 0.0 80 80 - ~ CPio Btu lb mole F 51 44 47.5 MW , lb lb mol 128 94 222 63 67.2 65 20, 000 Btu , lb mol A i, lb ft 3 HR Energy balance with work term included is: Q WS X A HR FA0 A 1, B FB 0 FA0 i CPi T To 10 1, X AF 10 1 Q UA(Ts T ) Substituting into energy balance, UA(TS T ) WS FA0 H R X AF UA(TS T ) WS T T0 FA0 H R FA0 C pA C pB T T0 FA0 C pA C pB UA(TS T ) WS FA0 H R FA0 C pA C pB UA Ws 63525 T 199 F Btu hr 12-55 UA T T0 P12-7 (a) A B C Since the feed is equimolar, CA0 = CB0 = 0 .1 mol/dm3 CA = CA0(1-X) CB = CB0(1-X) Adiabatic: T X[ H R (T0 )] X CP i CPi T0 CP C pC C pB C pA H R (T ) HC Ci C pA i 30 15 15 0 HB H A = - 41000 - (-15000 ) - (-20000) = -6000 cal/mol A C pB 15 15 30 B rA 6000 X 300 200 X 30 k C A2 0 (1 X ) 2 .01 k (1 X )2 VPFR FA0 T cal mol K 300 dX rA FA0 X rA FA0 = CA0v0 = (.1)(2) = 0.2 mols/dm3 VCSTR k = .01*exp((10000 / 2) * (1 / 300 - 1 / T)) See Polymath program P12-7-a.pol. Calculated values of NLE variables Variable Value f(x) Initial Guess 1T 483.8314 -1.421E-13 700. 2X 0.919157 -1.516E-10 0.99 Variable Value 1 Ca0 0.1 2 Fa0 0.2 12-56 3k 5.625546 4 ra -0.0003677 5V 500. Nonlinear equations 1 f(T) = T- 300 - 200 * X = 0 2 f(X) = X + V*ra/Fa0 = 0 Explicit equations 1 V = 500 2 k = 0.01*exp((10000 / 2) * (1 / 300 - 1 / T)) 3 Fa0 = 0.2 4 Ca0 = 0.1 5 ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2) For 500 dm3 CSTR, X = 0.92 For two 250 dm3 CSTR in series, X = 0.967 P12-7 (b) Constant heat exchanger temperature Ta When heat exchanger is added, the energy balance can be written as H Rxn (T ) dT Ua(Ta T ) ( rA ) dV F ( C Cˆ ) A0 So with Cˆ P = 0, i C pi i pi P 30 , H Rxn = -6000 cal/mol dT dV Ua(Ta T ) ( rA ) 6000 FA0 (30) Where Ua = 20 cal/m3/s/K, Ta = 450 K See Polymath program P12-7-b.pol. 12-57 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3634806 0.3634806 T 300 300 455.47973 450.35437 k 0.01 0.01 3.068312 2.7061663 Kc 286.49665 9.2252861 286.49665 9.9473377 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0221893 -1.0E-04 -0.0010758 Xe 0.8298116 0.3682217 0.8298116 0.3810642 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Ta 450 450 450 450 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = ((ra*DH)-Ua*(T-Ta))/(Fao*sumcp) Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Ta = 450 [10] Fao = 0.2 [11] sumcp = 30 12-58 500 450 T [K] 400 350 300 250 0 1 2 3 4 5 6 7 8 9 10 6 7 8 9 10 3 V [m ] 0.4 0.35 0.3 X 0.25 0.2 0.15 0.1 0.05 0 0 1 2 3 4 5 V [m3] 0.9 0.8 0.7 0.6 Xe 0.5 0.4 0.3 0.2 0.1 0 0 1 2 3 4 5 6 7 3 V [m ] 12-59 8 9 10 P12-7 (c) For a co-current heat exchanger, CpC = 1cal/g/K, Ta1=450 K, m 50 g sec See Polymath program P12-7-c.pol. Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3611538 0.3611538 T 300 300 442.15965 442.15965 Ta 450 434.90618 450 441.60853 k 0.01 0.01 2.1999223 2.1999223 Kc 286.49665 11.263546 286.49665 11.263546 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0160802 -1.0E-04 -0.0019246 Xe 0.8298116 0.4023362 0.8298116 0.4023362 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 mc 50 50 50 50 Cpc 1 1 1 1 12-60 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(T-Ta)/mc/Cpc Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Fao = 0.2 [10] sumcp = 30 [11] mc = 50 [12] Cpc = 1 500 Ta 450 400 350 T 300 250 0 1 2 3 4 5 6 7 8 V [m3] 12-61 9 10 0.9 0.8 0.7 0.6 Xe 0.5 0.4 0.3 X 0.2 0.1 0 0 1 2 3 4 5 6 7 8 9 10 3 V [m ] Next increase the coolant flow rate and run the same program to compare results. P12-7 (d) For counter-current flow, swap (T – Ta) with (Ta-T) in dTa/dV equation in the previous polymath program. See Polymath program P12-7-d.pol. Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 12-62 X 0 0 0.3647241 0.3647241 T 300 300 463.44558 450.37724 Ta 440.71 440.71 457.98124 450.00189 k 0.01 0.01 3.7132516 2.7077022 Kc 286.49665 8.2274817 286.49665 9.9439517 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0256436 -1.0E-04 -9.963E-04 Xe 0.8298116 0.3488462 0.8298116 0.381006 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 mc 50 50 50 50 Cpc 1 1 1 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(Ta-T)/mc/Cpc Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Fao = 0.2 [10] sumcp = 30 [11] mc = 50 [12] Cpc = 1 12-63 500 Ta 450 T 400 350 300 250 0 1 2 3 4 5 6 7 8 9 10 6 7 8 9 10 V [m3] 0.9 0.8 0.7 Xe 0.6 0.5 0.4 0.3 0.2 0.1 X 0 0 1 2 3 4 5 V [m3] P12-7 (e) Adiabatic See Polymath program P12-7-e.pol. 12-64 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca0 0.1 0.1 0.1 0.1 2 Cpc 1. 1. 1. 1. 3 DH -6000. -6000. -6000. -6000. 4 Fa0 0.2 0.2 0.2 0.2 5 k 0.01 0.01 0.010587 0.010587 6 Kc 286.4967 276.8576 286.4967 276.8576 7 mc 50. 50. 50. 50. 8 Qg 0.6 0.6 0.6286162 0.6286162 9 Qr 0 0 0 0 10 ra -0.0001 -0.0001048 -0.0001 -0.0001048 11 sumCp 30. 30. 30. 30. 12 T 300. 300. 301.0235 301.0235 13 Ta 450. 450. 450. 450. 14 Ua 0 0 0 0 15 V 0 0 10. 10. 16 X 0 0 0.0051176 0.0051176 17 Xe 0.8298116 0.827152 0.8298116 0.827152 Differential equations 1 d(X)/d(V) = -ra/Fa0 2 d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fa0*sumCp) 3 d(Ta)/d(V) = Ua*(T-Ta)/mc/Cpc Explicit equations 1 Kc = 10*exp(-6000/1.987*(1/450-1/T)) 2 k = 0.01*exp((10000/1.987)*(1/300-1/T)) 3 Fa0 = 0.2 4 Ca0 = 0.1 5 ra = -k*(Ca0^2)*((1-X)^2-X/Ca0/Kc) 6 Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 7 DH = -6000 8 Ua = 20*0 9 sumCp = 30 12-65 10 mc = 50 11 Cpc = 1 12 Qg = ra*DH 13 Qr = Ua*(T-Ta) 12-66 P12-7 (f) We see that it is better to use a counter-current coolant flow as in this case we achieve the maximum equilibrium conversion using a lesser volume of the PFR. 12-67 P12-8 Refer to solution P11-6 rA dT dV Heat Exchange FiCPi (16B) FA0 rA dT dV H Rx Ua T Ta FiCPi iCPi H Rx FA0 CP X , if CP Ua T Ta iC Pi A. Constant Ta (17B) Ta = 300 Additional Parameters (18B – (20B): Ta, i C Pi , Ua, B. Variable Ta Co-Current (17C) dTa dV Ua T Ta , V 0 ÝCPcool m Ta Tao Ta ? C. Variable Ta Counter Current (18C) dTa dV Ua Ta T ÝCPcool m V 0 Guess Ta at V = 0 to match Ta = Tao at exit, i.e., V = Vf (a) Variable Ta Co-Current 12-68 0 then (b) Gas Phase Counter Current Heat Exchange Vf = 20 dm3 Matches 12-69 (c) Constant Ta 12-70 ----------------------------------------------------------------------------------------------------------------------------(d) refer to problem P11-6 (e) Endothermic PFR A B dX dV k1 1 1 X KC 0 , Xe KC 1 KC Xe X XEB X EB i C Pi T T0 H Rx T0 12-71 C PA I C PI H Rx T T0 H Rx X CPA I C PI T T0 PFR Adiabatic FA0 FT 1. Irreversible A A. B Liquid Phase, Keep FA0 Constant First order dX dV rA FA0 F 1 X k A0 FA0 kCA FA0 k 1 X kCA0 1 X FA0 Constant density liquid volumetric flow rate without inert 0 0 FA0 FI FA0 0 1 I k1 X 0 1 I dX dV First Order Irreversible I ISO I 1 ISO k T 1 V V 12-72 I I k 1 yI X k 1 I I OP T I Endothermic Adiabatic 12-73 I OP T I 12-74 12-75 ----------------------------------------------------------------------------------------------------------------------------- P12-9 Refer to solution P11-7 For Heat Exchanger A Energy Balance terms (20), CP 15 Same as adiabatic 0 Ua Energy Balance 1 dT b dW FA0 Ta T rA H Rx rA H Rx Ua T Ta b i C Pi FA0 CP X Ua 320 b 1400 12-76 0.23 i C Pi (21) dT 0.23 Ta T dW 500 Ta A Constant Ta (22A) 300 K Ua B Co-Current Exchange (22B) C Counter Current (22C) T Ta dTa b dW Ýc C PCool m Ua dTa dW rA H Rx Ta T b mcCPCool (a) Co-Current Heat Exchange Gas Phase Co-current Variable Ta 12-77 , mc = 018, C PCool 18 (b) Counter Current Ta Matches 12-78 Gas Phase Counter Current Variable Ta 12-79 Gas Phase Counter Current Variable Ta Gas Phase Counter Current Variable Ta 12-80 (c) Constant Ta Constant Ta 12-81 Gas Phase Constant Ta 12-82 Gas Phase Constant Ta (d) Refer to solution P11-7 for comparison P12-10 (a) For reversible reaction, the rate law becomes rA T 300 200 X k k (300) exp KC k C AC B E 1 1 R 300 T K C (450) exp H Rxn 1 1 R 450 T Stoichiometry: CC C A0 X CA C A0 (1 X ) CB C A0 (1 X ) 12-83 CC KC See Polymath program P12-10-a.pol. POLYMATH Results No Title 03-21-2006, Rev5.1.233 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.0051176 0.0051176 T 300 300 301.02352 301.02352 k 0.01 0.01 0.010587 0.010587 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 Kc 286.49665 276.85758 286.49665 276.85758 ra -1.0E-04 -1.048E-04 -1.0E-04 -1.048E-04 Xe 0.8298116 0.827152 0.8298116 0.827152 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 Explicit equations as entered by the user [1] T = 300+200*X [2] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] Kc = 10 * exp(-6000 /1.987 * (1 / 450 - 1 / T)) [6] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [7] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 12-84 301.2 0.006 301 0.005 300.8 X T [K] 0.004 300.6 0.003 300.4 0.002 300.2 0.001 300 299.8 0 0 1 2 3 4 5 6 7 8 9 10 0 1 2 3 3 4 5 V [m ] 0.83 0.8295 Xe 0.829 0.8285 0.828 0.8275 0.827 0 1 2 3 4 5 6 7 8 9 10 V [m3] P12-10 (b) When heat exchanger is added, the energy balance can be written as H Rxn (T ) dT Ua (Ta T ) ( rA ) dV FA0 ( CöP ) i C pi C 30 , H = -6000 cal/mol So with Cö = 0, P i pi 6 3 V [m ] Rxn dT dV Ua(Ta T ) ( rA ) 6000 FA0 (30) Where Ua = 20 cal/m3/s/K, Ta = 450 K See Polymath program P12-10-b.pol. 12-85 7 8 9 10 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3634806 0.3634806 T 300 300 455.47973 450.35437 k 0.01 0.01 3.068312 2.7061663 Kc 286.49665 9.2252861 286.49665 9.9473377 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0221893 -1.0E-04 -0.0010758 Xe 0.8298116 0.3682217 0.8298116 0.3810642 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Ta 450 450 450 450 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = ((ra*DH)-Ua*(T-Ta))/(Fao*sumcp) Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Ta = 450 [10] Fao = 0.2 [11] sumcp = 30 12-86 500 0.4 0.35 450 0.3 0.25 X T [K] 400 350 0.2 0.15 0.1 300 0.05 250 0 0 1 2 3 4 5 6 7 8 9 10 0 3 0.9 0.8 0.7 0.6 Xe 0.5 0.4 0.3 0.2 0.1 0 0 1 2 3 4 5 1 2 3 4 5 V [m3] V [m ] 6 7 8 9 10 V [m3] P12-10 (c) For a co-current heat exchanger, g sec See Polymath program P12-10-c.pol. CpC = 1cal/g/K, Ta1=450 K, m 50 12-87 6 7 8 9 10 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3611538 0.3611538 T 300 300 442.15965 442.15965 Ta 450 434.90618 450 441.60853 k 0.01 0.01 2.1999223 2.1999223 Kc 286.49665 11.263546 286.49665 11.263546 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0160802 -1.0E-04 -0.0019246 Xe 0.8298116 0.4023362 0.8298116 0.4023362 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 mc 50 50 50 50 Cpc 1 1 1 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(T-Ta)/mc/Cpc Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Fao = 0.2 [10] sumcp = 30 [11] mc = 50 [12] Cpc = 1 12-88 500 0.9 0.8 Ta 450 0.7 0.6 Xe 400 0.5 0.4 350 0.3 T X 0.2 300 0.1 250 0 0 1 2 3 4 5 6 7 8 9 10 0 1 2 3 4 3 5 6 7 8 3 V [m ] V [m ] Next increase the coolant flow rate and run the same program to compare results. P12-10(d) For counter-current flow, See Polymath program P12-10-d.pol. Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3647241 0.3647241 T 300 300 463.44558 450.37724 Ta 440.71 440.71 457.98124 450.00189 k 0.01 0.01 3.7132516 2.7077022 Kc 286.49665 8.2274817 286.49665 9.9439517 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0256436 -1.0E-04 -9.963E-04 Xe 0.8298116 0.3488462 0.8298116 0.381006 DH -6000 -6000 -6000 -6000 Ua 20 20 20 20 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 mc 50 50 50 50 Cpc 1 1 1 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(Ta-T)/mc/Cpc 12-89 9 10 Explicit equations as entered by the user [1] k = .01 * exp((10000 / 1.987) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(-6000 / 1.987 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = -6000 [8] Ua = 20 [9] Fao = 0.2 [10] sumcp = 30 [11] mc = 50 [12] Cpc = 1 500 0.9 0.8 Ta 450 0.7 Xe T 0.6 400 0.5 0.4 350 0.3 0.2 300 0.1 250 X 0 0 1 2 3 4 5 6 7 8 9 10 0 V [m3] 1 2 3 4 5 6 7 8 9 10 V [m3] P12-10 (e) We see that it is better to use a counter-current coolant flow as in this case we achieve the maximum equilibrium conversion using a lesser volume of the PFR. P12-10 (f) If the reaction is irreversible but endothermic, we have rA k C A2 0 (1 X )2 .01 k (1 X )2 as obtained in the earlier problem. H Rxn 6000cal / mol See Polymath program P12-10-f-co.pol. we use 8- 7f cocurrent.pol 12-90 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.4016888 0.4016888 T 300 300 428.84625 424.16715 Ta 450 425.45941 450 425.45941 k 0.01 0.01 1.4951869 1.314808 Ca0 0.1 0.1 0.1 0.1 Fa0 0.2 0.2 0.2 0.2 ra -1.0E-04 -0.0132694 -1.0E-04 -0.0047067 DH 6000 6000 6000 6000 Ua 20 20 20 20 Fao 0.2 0.2 0.2 0.2 sumcp 30 30 30 30 mc 50 50 50 50 Cpc 1 1 1 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(T-Ta)/mc/Cpc Explicit equations as entered by the user [1] k = .01 * exp((10000 / 2) * (1 / 300 - 1 / T)) [2] Ca0 = 0.1 [3] Fa0 = 0.2 [4] ra = -k * (Ca0 ^ 2) *(1 - X) ^ 2 [5] DH = 6000 [6] Ua = 20 [7] Fao = 0.2 [8] sumcp = 30 [9] mc = 50 [10] Cpc = 1 12-91 For counter-current flow, See Polymath program P12-10-f-counter.pol. Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 10 10 X 0 0 0.3458817 0.3458817 T 300 300 449.27319 449.27319 Ta 423.8 423.8 450.01394 450.01394 k 0.01 0.01 2.5406259 2.5406259 Kc 0.3567399 0.3567399 9.8927301 9.8927301 Fa0 0.2 0.2 0.2 0.2 Ca0 0.1 0.1 0.1 0.1 ra -1.0E-04 -0.0141209 -1.0E-04 -0.0019877 Xe 0.0333352 0.0333352 0.3801242 0.3801242 DH 6000 6000 6000 6000 12-92 Ua Fao sumcp mc Cpc 20 0.2 30 50 1 20 0.2 30 50 1 20 0.2 30 50 1 20 0.2 30 50 1 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra / Fa0 [2] d(T)/d(V) = (Ua*(Ta-T)+(ra)*DH)/(Fao*sumcp) [3] d(Ta)/d(V) = Ua*(Ta-T)/mc/Cpc Explicit equations as entered by the user [1] k = .01 * exp((10000 / 2) * (1 / 300 - 1 / T)) [2] Kc = 10 * exp(6000 / 2 * (1 / 450 - 1 / T)) [3] Fa0 = 0.2 [4] Ca0 = 0.1 [5] ra = -k * (Ca0 ^ 2) * ((1 - X) ^ 2 - X /Ca0/ Kc) [6] Xe = (2+1/Kc/Ca0-((2+1/Kc/Ca0)^2-4)^0.5)/2 [7] DH = 6000 [8] Ua = 20 [9] Fao = 0.2 [10] sumcp = 30 [11] mc = 50 [12] Cpc = 1 12-93 P12-11 (a) Constant Ta, PBR Part (1) Calculated values of the DEQ variables Variable initial value minimal value maximal value final value W 0 0 50 50 X 0 0 0.8987768 0.8987768 T 450 450 893.55511 893.55511 To 450 450 450 450 vo 20 20 20 20 Cao 0.2706726 0.2706726 0.2706726 0.2706726 Ca 0.2706726 0.0072668 0.2706726 0.0072668 k 0.133 0.133 8.5739542 8.5739542 ra -0.0359995 -0.1539472 -0.0359995 -0.062305 Ta 323 323 323 323 Cpa 40 40 40 40 delH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 Uarho 0.08 0.08 0.08 0.08 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(W) = -ra/(Cao*vo) [2] d(T)/d(W) = (Uarho*(Ta-T)+ra*delH)/(Cao*vo*Cpa) Explicit equations as entered by the user 12-94 [1] To = 450 [2] vo = 20 [3] Cao = 10/0.0821/450 [4] Ca = Cao*(1-X)/(1+X)*To/T [5] k = 0.133*exp(31400/8.314*(1/450-1/T)) [6] ra = -k*Ca [7] Ta = 323 [8] Cpa = 40 [9] delH = -20000 [10] Uarho = 0.08 Ua rho 0.08 J s kgcat K Part (2) Ua rho 240 J s kgcat K 12-95 In part (1), Ua/rho is so small that the reactor behaves as if there is no heat exchange occurring. In part (2), Ua/rho is 3000 times larger, causing the heat exchange term Ua/rho*(T-Ta) to be much larger. Therefore, in part (2), we can see the effect of heat exchange in the temperature drop, which causes the reaction to be slower, hence the lower conversion X. Part (3) Keep Ua rho 240 J s kgcat K Add differential equation dy dW 2y * (1 X )* T , with To And include pressure drop in expression for Ca: C a C ao 0.019 kg -1 (1 X ) To y (1 X ) T If there is pressure drop in the PBR, we observe a slight decrease in the conversion X. The pressure drop causes Ca to decrease (y 1 always), which decreases reaction rate slightly, which decreases conversion slightly. P12-11 (b) Co-current and Counter-current heat exchange, PBR For co-current heat exchange, add equation: dTa dW For counter-current heat exchange, add equation: with mc 0.2 kg and C p ,coolant s 5000 J kg K Part (1) 12-96 Ua rho (T Ta ) mcoolantC p , coolant dTa dW Ua rho (Ta T ) , mc C p , coolant Ua rho 0.08 J s kgcat K Co-current Counter-current Again, Ua/rho is so small that the reactor behaves as if there is no heat exchange. Therefore, it doesn’t matter whether we use a counter-current or co-current heat exchanger; the temperature and conversion profiles will be similar. Part (2) Ua rho 240 J s kgcat K Co-current 12-97 Counter-current The heat exchange is significant in this part, so we will see a difference in the temperature and conversion profiles depending on whether a co-current or counter-current heat exchange is used. The counter-current heat exchanger is generally better at heat transfer than the cocurrent heat exchanger. Therefore, in the counter-current case, the temperature of the reactor is almost constant at 323K. Notice that the temperature and conversion profiles are similar to the constant Ta case (P8-9a, part 2). The co-current heat exchanger, on the other hand, is not able to keep the reactor temperature as low as the counter-current. Therefore, the higher reactor temperature results in a higher conversion in the co-current case. Part (3) Keep Ua rho 240 J s kgcat K Add differential equation dy dW 2y * (1 X )* T , with To 12-98 0.019 kg -1 And include pressure drop in expression for Ca: C a C ao (1 X ) To y (1 X ) T Co-current Counter-current The pressure drop causes Ca to decrease (y 1), which decreases reaction rate slightly, which decreases conversion slightly. P12-11 (c) Step 1: Find XMB = f(T): FA0 X W rA ' rA ' kC A CA C A0 (1 X ) T0 (1 X ) T Combining: FA0 X W (1 X ) T0 kC A0 (1 X ) T 12-99 Note V W 0 b 0 k b (1 T T0 X2 X (1 X ) TT0 k b )X k b X) ( TT0 T X MB Where k T2 T0 k b k1 exp E 1 R T1 0 6TT0 k b 2T T0 2 2 k2 b 2 1 T Step 2: Find XEB = f(T): When C P 0 and pure A enters the reactor, X EB UA(T Ta ) C PA (T T0 ) FA0 H RXN 0.16 0.14 0.12 X 0.1 Xmb 0.08 Xeb 0.06 0.04 0.02 0 365 370 375 380 385 T(K) The intersection of the mass balance and energy balance lines correspond to the conditions in the reactor. Therefore, the reactor operates at T=376.7K and X=0.101. Parameters: 12-100 T0 450K 4000s 0.001 b kg dm 3 k 0.0133* exp Ta 323K UA 500 1 dm 3 R 450 T kg s J s K FA0 CA 0 0 CPA 40 H RXN 1 E 10 mol 0.0821* 450 dm 3 * 20 dm 3 s 05.41 mol s J mol K 20000 J mol P12-11 (d) For a reversible reaction, we have all the previous equations, but the rate law is modified as: rA k f C A kr CB CC X T0 1 X T Plugging the equation for kr, and solving using POLYMATH program, we get the plots. Only the co-current program and plots are shown. CB CC C A0 See Polymath program P12-11-d.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 W 0 0 80. 80. 2 X 0 0 0.057593 0.057593 3 T 450. 420.7523 450. 420.7523 4 Ta 323. 323. 426.1627 420.7565 5 T0 450. 450. 450. 450. 6 v0 20. 20. 20. 20. 12-101 7 k 0.133 0.0742131 0.133 0.0742131 8 Uarho 240. 240. 240. 240. 9 P0 1.013E+06 1.013E+06 1.013E+06 1.013E+06 10 CA0 270.8283 270.8283 270.8283 270.8283 11 CA 270.8283 258.1071 270.8283 258.1071 12 kr 0.2 0.076962 0.2 0.076962 13 CC 0 0 15.77362 15.77362 14 CB 0 0 15.77362 15.77362 15 rA -36.02017 -36.02017 -0.0062421 -0.0062421 Differential equations 1 d(X)/d(W) = -rA / v0 / CA0 2 d(T)/d(W) = (Uarho * (Ta - T) + rA * 20000) / v0 / CA0 / 40 3 d(Ta)/d(W) = Uarho * (T - Ta) / .2 / 5000 + sign = cocurrent, -ve sign = countercurrent in RHS of eqn. Explicit equations 1 T0 = 450 2 v0 = 20 3 k = 0.133 * exp(31400 / 8.314 * (1 / T0 - 1 / T)) 4 Uarho = .08 * 3000 5 P0 = 1013250 6 CA0 = P0 / 8.314 / T0 7 CA = CA0 * (1 - X) / (1 + X) * T0 / T 8 kr = 0.2 * exp(51400 / 8.314 * (1 / T0 - 1 / T)) 9 CC = CA0 * X / (1 + X) * T0 / T 10 CB = CA0 * X / (1 + X) * T0 / T 11 rA = -(k * CA - kr * CB * CC) 12-102 P12-11 (e) Individualized solution P12-12 (a) Start with the complete energy balance: dEˆ dt Q WS Fi H i in Fi H i out Fi RV i out The following simplifications can be made: It is steady state. In part (a), there is no heat taken away or added There is no shaft work That leaves us with Fi H i in Fi H i out Evaluating energy terms: Fi RV i out H A0 FA0 H B 0 FB 0 H C 0 FC 0 Out: H A FA H B FB H C ( FC RCV ) In: Now we evaluate Fi FA FA0 FA0 X FB FB 0 FA0 X FC FC 0 FA0 X FB0 = FC0 = 0 12-103 Inserting these into our equation gives: H A FA0 H A FA0 X H B FA0 X H C FA0 X H C RCV H A0 FA0 0 Combining and substituting terms gives: FA0 H A H A0 FA0 X H RX H C RC 0 FA0CPA T T0 FA0 X H RX H C (T0 ) CPC T T0 RC 0 RC 0 Differentiating with respect to V with ΔCP = 0 FA0C p dT dV dX dV FA0 (rA ) dT dV H Rx T H Rx T H C (T0 ) CPC T T0 H C (T0 ) CPC T T0 FA0 i C pi Combine that with the mole balance and rate law: rA dFA dV CA rB rC k CA CB CC KC dF dFB rB ; C rC RC dV dV F T F T CT 0 A 0 CB CT 0 B 0 CC FT T FT T rA ; CT 0 FC T0 FT T See Polymath program P12-11-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 0.2710027 0.1839444 0.2710027 0.1839444 2 Cb 0 0 0.0098751 0.0098751 3 Cc 0 0 0.0065147 0.0029402 4 Cpa 40. 40. 40. 40. 5 Cpb 25. 25. 25. 25. 6 Cpc 15. 15. 15. 15. 7 Ct0 0.2710027 0.2710027 0.2710027 0.2710027 8 dHrx -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 12-104 RC 9 Fa 5.42 5.143851 5.42 5.143851 10 Fa0 5.420054 5.420054 5.420054 5.420054 11 Fb 0 0 0.2761489 0.2761489 12 Fc 0 0 0.1641532 0.0822207 13 Ft 5.42 5.42 5.584153 5.502221 14 Hc -3.735E+04 -3.735E+04 -3.48E+04 -3.48E+04 15 k 0.133 0.133 1.325591 1.325591 16 kc 1.5 1.5 1.5 1.5 17 Kc 0.0006905 0.0001596 0.0006905 0.0001596 18 ra -0.0360434 -0.0589786 -0.0027523 -0.0027523 19 Rc 0 0 0.009772 0.0044103 20 T 450. 450. 619.7977 619.7977 21 To 450. 450. 450. 450. 22 V 0 0 30. 30. 23 Xe 0.0504144 0.0284733 0.0504144 0.0284733 Differential equations 1 d(Fc)/d(V) = -ra-Rc 2 d(Fb)/d(V) = -ra 3 d(Fa)/d(V) = ra 4 d(T)/d(V) = (Fa0*ra*dHrx - Rc*Hc)/(Fa0*Cpa) Explicit equations 1 k = .133*exp((31400/8.314)*(1/450-1/T)) 2 To = 450 3 Ct0 = 10/0.082/450 4 Ft = Fa + Fb + Fc 5 Cc = Ct0*Fc/Ft*To/T 6 Fa0 = Ct0*20 7 Ca = Ct0*Fa/Ft*To/T 8 dHrx = -20000 9 Cb = Ct0*Fb/Ft*To/T 10 Kc = 0.01*exp((dHrx/8.314)*(1/300-1/T)) 11 Cpc = 15 12 ra = -k*(Ca-Cb*Cc/Kc) 12-105 13 kc = 1.5 14 Rc = kc*Cc 15 Xe = ((Kc*T/(Ct0*To))/(1+(Kc*T/(Ct0*To))))^0.5 16 Cpa = 40 17 Cpb = 25 18 Hc = -40000+Cpc*(T-273) P12-12 (b) Now, the heat balance equation needs to be modified. dT dV Ua(Ta T ) (rA ) H Rx T FA0 H C (T0 ) CPC T T0 i C pi Temperature reaches a peak value of 628 K before again dropping down. 12-106 RC P12-13 (a) Substrate More cells + Product SC+P G(T) = X*-∆HRX To solve for G(T) we need X as a function of temperature, which we get by solving the mass balance equation. rg FA0 X FS 0 X V and since rS then, rA rS Yc / s V Yc / s FS 0 X rg rg CC and (T ) CS KS CS 6700 T 48000 1 exp 153 T 0.0038* T exp 21.6 where (T ) 1max if we combine these equations we get: Yc / s FS 0 X V (T )CC CS K S CS 12-107 V CS V Yc / s FS 0 X K S CS (T )CC CS CS 0 1 X and CC Yc / s FS 0 X K S CS 0Yc / s X CS 0 1 X (T )CS 0Yc / s XCS 0 1 X Canceling and combining gives: V FS 0 K S (T )C CS 0 1 X 2 S0 1 X Now solve this expression for X: FS 0 K S X 1 (T )VCS20 FS 0CS 0 It can be observed from graph that if the reactor operates at a steady state temperature of 294.4<T(K)>316.79, Conversion achieved is 0. Now that we have X as a function of T, we can plot G(T). To get R(T) we must calculate the heat removed which is the sum of the heat absorbed by reactants to get to the reaction temperature and the heat removed from any heat exchangers. The heat gained by the reactants = CP 0 T T0 The heat removed by the heat exchanger = UA(T-Ta)/FS0 UA R(T ) CPS T T0 T Ta FS 0 12-108 Now enter the equations into polymath and specify all other constants. The adiabatic case is shown below. The non-adiabatic case would be with explicit equation [12] as A = 1.1. See Polymath program P12-13-a.pol. Differential equations as entered by the user [1] d(T)/d(t) = 1 Explicit equations as entered by the user [1] mumax = .5 [2] Ycs = .8 [3] vo = 1 [4] Ta = 290 [5] mu = mumax*(.0038*T*exp(21.6-6700/T))/(1+exp(153-48000/T))) [6] Ks = 5 [7] V = 6 [8] Cso = 100 [9] Fso = vo*Cso [10] Cps = 5 [11] dH = -20000 [12] UA = 0*300 [13] kappa = UA/(Cps*Fso) [14] To = 280 [15] X = 1-((Fso*Ks)/((mu*V*(Cso^2))-Fso*Cso)) [16] Gt = if T<294.4 or T>316.7 then 0 else X*(-dH)*Ycs [17] Rt = Cps*(T-To)+UA*(T-Ta)/Fso Independent variable variable name : t initial value : 0 T(0): 280 final value : 45 Adiabatic case 12-109 Non adiabatic case 12-110 P12-13 (b) To maximize the exiting cell concentration, we want to maximize the conversion of substrate. If we look at G(T) from part A, we see that it is at a maximum at about 310 K. This corresponds to the highest conversion that can be achieved. By changing the values of UA and m c we can change the slope of the R(T). What we are looking to do is get R(T) to intersect with G(T) at 310 K. Since we now have a limited coolant flow rate we will use a different value for Q. Q mC C PC T Ta 1 exp UA mC C PC and so, R(T ) mC C PC T Ta 1 exp UA mC C PC C PS T T0 Now we set R(T) equal to the maximum value of G(T) which is 15600 J/h G (T ) 15600 FS 0 mC C PC T Ta 1 exp UA mC C PC FS 0 C PS T T0 And now plug in the known values. Assume the maximum coolant flow rate and that will give the minimum heat exchange area. 12-111 15600 g J 100 g hr 60000 g hr 1560000 UA 4.2 J hr J 310 K gK 290 K 1 exp 5040000 J hr 1 exp UA g 60000 hr J 4.2 gK UA 252000 J hr K J hr K A=1.85 m2 Plot of G(T) ,R(T) Vs T 12-112 100 11000 g h J hr 5 J 310 K gK 288 K P12-13 (c) From the plot of G(T) vs R(T) for (1) Aiabatic case : There are two steady states possible- 281K (stable and X=0), 294.2K (unstable) and 316.76K (stable and X=0.175) (2) Non adiabatic case with large coolant flow rate : There are three steady states –289K (stable and X=0), 294.2K (unstable) and 315.7K (stable and X=0.89) (3) Non adiabatic case with limited coolant flow rate : There are three steady states –289K (Stable and X=0), 294.3K (unstable) and 309K (stable and X=0.975) P12-13 (d) (1) Adiabatic case : Varying To From the graph, it can be observed that increasing To will increase the steady state temperature. 12-113 (2) Non adiabatic case with large coolant flow rate : Varying Ta Increasing Ta will increase steady state temperature. (3) Non adiabatic case with limited coolant flow rate Varying coolant flow rate Increasing coolant flow rate will decrease steady state temperature achieved. 12-114 P12-14 Assume Adiabatic (a) -12,000 cal/mol (b) Ignition = 260°C Extinction = 190°C (c) Ignition, T = 300°C, 475°C Extinction, T = 215°C, 375°C (d) X (Ignition) = 0.281 X (Extinction) = 0.86 P12-15 (a) G(T) X HR X k 1 k ,k 6.6 10 3 exp R(T) C p 0 1 T Tc C p0 50 Tc i C pi UA C p0 FA 0 8000 50 80 Ta T0 1 350K E 1 R 350 1 T 2 To find the steady state T, we must set G(T) = R(T). This can be done either graphically or solving the equations. We find that for T0 = 450 K, steady state temperature 399.94 K. 12-115 POLYMATH Results 02-22-2006, Rev5.1.233 Calculated values of the DEQ variables Variable initial value minimal value maximal value final value t 0 0 1000 1000 T 350 350 450 450 RT 0 0 1.5E+04 1.5E+04 EoR 2.013E+04 2.013E+04 2.013E+04 2.013E+04 k 0.0066 0.0066 2346.7972 2346.7972 tau 100 100 100 100 X 0.3975904 0.3975904 0.9999957 0.9999957 GT 2981.9277 2981.9277 7499.968 7499.968 at 2981.9277 -7500.032 4336.6841 -7500.032 12-116 ODE Report (RKF45) Differential equations as entered by the user [1] d(T)/d(t) = 0.1 Explicit equations as entered by the user [1] RT = 150*(T-350) [2] EoR = 40000/1.987 [3] k = 6.6*0.001*exp(EoR*(1/350-1/T)) [4] tau = 100 [5] X = tau*k/(1+tau*k) [6] GT = 7500*X [7] at = GT-RT P12-15 (b) First, we must plot G(T) and R(T) for many different T0’s on the same plot. From this we must generate data that we use to plot Ts vs To. Calculated values of NLE variables Variable Value f(x) Initial Guess 1T 399.9425 1.337E-10 450. ( 300. < T < 600. ) Variable Value 1 EoR 2.013E+04 2 GT 7491.375 3k 8.685615 4 RT 7491.375 5 tau 100. 6X 0.99885 Nonlinear equations 1 f(T) = RT - GT = 0 Explicit equations 1 RT = 150*(T-350) 2 EoR = 40000/1.987 3 k = 6.6*0.001*exp(EoR*(1/350-1/T)) 4 tau = 100 12-117 5 X = tau*k/(1+tau*k) 6 GT = 7500*X 400 390 380 370 T 360 350 340 330 320 310 300 310 330 350 370 390 410 430 To P12-15 (c) For high conversion, the feed stream must be pre-heated to at least 404 K. At this temperature, X = .991 and T = 384.2 K in the CSTR. Any feed temperature above this point will provide for higher conversions. P12-15 (d) For a temperature of 369.2 K, the conversion is 0.935 P12-15 (e) The extinction temperature is 363.3 K (90oC). P12-16 (a) Mol Balance : FA0 X v0C A0 X V rA k C A CB / K e V v0 X k 1 X X / Ke 12-118 X 1 X k (1 1/ K e ) k k 1 k (1 1/ K e ) G (T ) H Rx X 80000 X k 1min 1 10 min K e 100 10 X .901 1 10(1.01) G (400) 72080 cal / mol P12-16 (b) UA FA0C pA R(T ) C pA (1 3600 10* 40 9 )(T TC ) 400(T TC ) T0 Ta 310 1 R(T ) 400(T 310) The following plot gives us the steady state temperatures of 310, 377.5 and 418.5 K TC See Polymath program P12-16-b.pol. P12-16 (c) 12-119 P12-16 (d) P12-16 (e) The plot below shows Ta varied. The next plot shows how to find the ignition and extinction temperatures. The ignition temperature is 358 K and the extinction temperature is 208 K. 12-120 P12-16 (f) P12-16 (g) At the maximum conversion G(t) will also be at its maximal value. This occurs at approximately T = 404 K. G(404 K) = 73520 cal. For there top be a steady state at this temperature, R(T) = G(T). See Polymath program P12-16-g.pol. UA FA0C pA R(T ) C pA (1 )(T TC ) 73520 T0 Ta 1 If we plug in the values and solve for UA, we get: UA = 7421 cal/min/K where TC P12-16 (h) Individualized solution P12-16 (i) The adiabatic blowout flow rate occurs at V 0.0041s v0 v0 V 0.0041*10 v0 0.041 0.0041s dm3 min 12-121 See Polymath program P12-16-i.pol. P12-16 (j) Lowing T0 or Ta or increasing UA will help keep the reaction running at the lower steady state. P12-17 Given the first order, irreversible, liquid phase reaction: A B Ta 100 C UA 1.0 cal / min/ C Pure A Feed 0.5g mol / min C pA Cp C pB HR C pA Design Eqn : V Rate Law : 0 FA0 X rA rA kC A Stoichiometry : C A C pB 2cal / g mol / C 100cal / g v0 k (1 X ) C A0 (1 X ) Energy Balance : UA(T TA ) FA0 X H R FA0 i C pi (T T0 ) Simplifying, k 1 X 1 k 1 1 k HR 1 1 k The equation for heat removal curve is: UA R(T ) C pA 1 T Tc , , Tc C pA FA0 G (T ) HR X Ta To 1 Plot this along with the heat generation curve for various T0. 12-122 mol / C P12-17 (a) (a) Tc=156oC R T CP 0 1 C PS C PA T TC ICP I UA FA0C PA R T Tc C PA 2 1cal min K mol 2cal 0.5 min mol K 2 1 1 T TC 1 Ta T0 1 1 Ta 1 4 T Tc T0 2 100 T0 2 Draw R(T) with slope 4such that it is tangent to G(T) curve. The point of the tangency is at G(T) = R(T) = 27.5 and T 163°C. We could solve for Tc or read it off the graph by extrapolating to R(T) = 0 to find Tc = 156. R T Ta 4 T T0 4T 200 2T0 2 27.5cal mol A From the above Figure at the point of tangency R(T) = 27.5 and T = 163oC solving for T0, T 0 212 C or Tc Ta 1 T0 156 100 T0 , T0 2 212 R(T) slope is 4. Move 27.5 4 163 Tc Tc 156 100 T0 156 2 T0 312 100 212oC 12-123 P12-17 (b) (b) Ts=180oC Ts=163oC We see there are two intersections at which the reactor can operate. At upper intersection T = 180. T = 163oC and 180oC from Figure P12-17. P12-17 (c) Slope of R(T) curve is 4 if we move to left we see that there are 3 intersections. Because we heated the RcTr above the extraction temperature it will operate at the upper steady state at the upper steady state G(T) = R(T) = 90 cal/mol and T = 180°C. Extrapolating G(T) to large T, X = 1 so G = (– HRx) we find – HRx = 100 cal/mol). GT X H Rx X 100 X 0.9 90 4 180 Tc 100 T0 2 Solving for T Tc 157 or get Tc at R T T0 214 12-124 0, Tc 157 (c) P12-17 (d) (d) Tc=148oC At the point of tangency R(T) = G(T) = 80 and T = 167 R T 80 Tc 147 Tc T0 Ta 1 194 4 167 Tc 100 T0 2 T0 *Note all the temperatures in parts (a) – (d) are 2°C due to accuracy of reading the graph 12-125 P12-17 (e) Individualized solution P12-18 TC = Ta = T0 = 330 K τ = V/υ0 = 1.2 h V = FA0X/-rA = CA0υ0X/ -rA -rA = k(CA – CB/KC) = kCA0(1-X – X/KC) k = 0.001exp(30000/1.987(1/300-1/T) X = τk/(1+τK+τK/KC) G(T) = (-∆HRx)X G(T) is plotted as a function of T. See Polymath program P12-18.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cpo 250. 250. 250. 250. 2 DHrx -4.2E+04 -4.2E+04 -4.2E+04 -4.2E+04 3 E 3.0E+04 3.0E+04 3.0E+04 3.0E+04 4 GT 50.33959 0.0001053 3.61E+04 0.0001053 5 k 0.001 0.001 8.48E+07 8.48E+07 6 Kc 5.0E+06 2.507E-09 5.0E+06 2.507E-09 7 t 0 0 300. 300. 8 T 300. 300. 600. 600. 9 tau 1.2 1.2 1.2 1.2 0.8596127 2.507E-09 10 X 0.0011986 2.507E-09 Differential equations 1 d(T)/d(t) = 1 Explicit equations 1 E = 30000 12-126 2 k = 0.001*exp((E/1.987)*(1/300-1/T)) 3 DHrx = -42000 4 Kc = 5000000*exp((DHrx/1.987)*(1/300-1/T)) 5 Cpo = 250 6 tau = 1.2 7 X = tau*k/(1+tau*k + tau*k/Kc) 8 GT = X*(-DHrx) From the plot, the maximum conversion achieved, Xmax = 0.86 At Xmax, T = 367.6 K and G(T) = 36100 cal/mol R(T) = G(T) 12-127 κ = 2.84 Since Therefore, UA = (2.84)(10 mol/h)(250 cal/mol/K) = 7,100 cal/h/K P12-19 Adiabatic POLYMATH Report Ordinary Differential Equations No Title 08-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 0.019 0.019 0.019 0.019 2 Ca 1.9 0.7510709 1.902453 0.7510709 3 Ca0 1.9 1.9 1.9 1.9 4 Cc 0 0 0.1974831 0.1113793 5 Cp0 40. 40. 40. 40. 6 Cpc 4200. 4200. 4200. 4200. 7 deltaCp -30. -30. -30. -30. 8 DH -2.0E+04 -2.0E+04 -2.0E+04 9 epsilon -1. -1. -1. -1. 10 Fa0 5. 5. 5. 5. 11 k 0.01 0.01 0.0261675 0.0261675 12 Kc 10000. 902.809 10000. 902.809 13 m 0.05 0.05 0.05 0.05 14 ra -0.0361 -0.0627617 -0.014758 -0.014758 15 T 450. 450. 817.9727 817.9727 16 T0 450. 450. 450. 450. 17 Ta 500. 500. 500. 500. 18 Ua 0 0 0 0 -2.0E+04 12-128 19 W 0 0 50. 50. 20 X 0 0 0.4949381 0.4949381 21 y 1. 0.2174708 1. 0.2174708 Differential equations 1 d(X)/d(W) = -ra/Fa0 2 d(y)/d(W) = -alpha/2/y*(1+epsilon*X)*T/T0 3 d(T)/d(W) = (ra*(DH+deltaCp*(T-298)) - Ua*(T-Ta))/Fa0/Cp0 4 d(Ta)/d(W) = Ua*(T-Ta)/m/Cpc Explicit equations 1 Cp0 = 40 2 DH = -20000 3 epsilon = -1 4 T0 = 450 5 Ca0 = 1.9 6 Fa0 = 5 7 alpha = 0.019 8 Ca = Ca0*(1-X)/(1+epsilon*X)*T/T0*y 9 Ua = 0.8*0 10 deltaCp = 1/2*20-40 11 Kc = 10000*exp(DH/8.314*(1/450-1/T)) 12 Cc = Ca0*X/2/(1+epsilon*X)*T0/T*y 13 m = 0.05 14 Cpc = 4200 15 k = 0.01*exp(8000/8.314*(1/450-1/T)) 16 ra = -k*(Ca^2-Cc/Kc) General Total number of equations 20 Number of differential equations 4 Number of explicit equations 16 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 12-129 Now, constant temperature Ta = 300K POLYMATH Report Ordinary Differential Equations No Title 08-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 0.019 0.019 0.019 0.019 2 Ca 1.9 0.7615715 1.906858 0.7615715 3 Ca0 1.9 1.9 1.9 1.9 4 Cc 0 0 0.1991675 0.1180575 5 Cp0 40. 40. 40. 40. 6 Cpc 4200. 4200. 4200. 4200. 7 deltaCp -30. -30. -30. -30. 8 DH -2.0E+04 -2.0E+04 -2.0E+04 9 epsilon -1. -1. -1. -1. 10 Fa0 5. 5. 5. 5. 11 k 0.01 0.01 0.0248669 0.0248669 12 Kc 10000. 1025.524 10000. 1025.524 13 m 0.05 0.05 0.05 0.05 -2.0E+04 12-130 14 ra -0.0361 -0.0610755 -0.0144197 -0.0144197 15 T 450. 450. 783.9972 783.9972 16 T0 450. 450. 450. 450. 17 Ta 500. 500. 500. 500. 18 Ua 0.8 0.8 0.8 0.8 19 W 0 0 50. 50. 20 X 0 0 0.4848172 0.4848172 21 y 1. 0.2300674 1. 0.2300674 Differential equations 1 d(X)/d(W) = -ra/Fa0 2 d(y)/d(W) = -alpha/2/y*(1+epsilon*X)*T/T0 3 d(T)/d(W) = (ra*(DH+deltaCp*(T-298)) - Ua*(T-Ta))/Fa0/Cp0 4 d(Ta)/d(W) = Ua*(T-Ta)/m/Cpc *0 Explicit equations 1 Cp0 = 40 2 DH = -20000 3 epsilon = -1 4 T0 = 450 5 Ca0 = 1.9 6 Fa0 = 5 7 alpha = 0.019 8 Ca = Ca0*(1-X)/(1+epsilon*X)*T/T0*y 9 Ua = 0.8 10 deltaCp = 1/2*20-40 11 Kc = 10000*exp(DH/8.314*(1/450-1/T)) 12 Cc = Ca0*X/2/(1+epsilon*X)*T0/T*y 13 m = 0.05 14 Cpc = 4200 15 k = 0.01*exp(8000/8.314*(1/450-1/T)) 16 ra = -k*(Ca^2-Cc/Kc) General Total number of equations 20 12-131 Number of differential equations 4 Number of explicit equations 16 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 Now, Co-current heat exchanger POLYMATH Report Ordinary Differential Equations No Title 08-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 0.019 0.019 0.019 0.019 2 Ca 1.9 0.7614153 1.906781 0.7614153 3 Ca0 1.9 1.9 1.9 1.9 4 Cc 0 0 0.1990505 0.1177523 5 Cp0 40. 40. 40. 40. 6 Cpc 4200. 4200. 4200. 4200. -30. -30. -30. 7 deltaCp -30. 12-132 8 DH -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 9 epsilon -1. -1. -1. -1. 10 Fa0 5. 5. 5. 5. 11 k 0.01 0.01 0.0249108 0.0249108 12 Kc 10000. 1021.01 10000. 1021.01 13 m 0.05 0.05 0.05 0.05 14 ra -0.0361 -0.0610733 -0.0144393 -0.0144393 15 T 450. 450. 785.126 785.126 16 T0 450. 450. 450. 450. 17 Ta 500. 499.0741 521.1534 521.1534 18 Ua 0.8 0.8 0.8 0.8 19 W 0 0 50. 50. 20 X 0 0 0.4849408 0.4849408 21 y 1. 0.2296895 1. 0.2296895 Differential equations 1 d(X)/d(W) = -ra/Fa0 2 d(y)/d(W) = -alpha/2/y*(1+epsilon*X)*T/T0 3 d(T)/d(W) = (ra*(DH+deltaCp*(T-298)) - Ua*(T-Ta))/Fa0/Cp0 4 d(Ta)/d(W) = Ua*(T-Ta)/m/Cpc Explicit equations 1 Cp0 = 40 2 DH = -20000 3 epsilon = -1 4 T0 = 450 5 Ca0 = 1.9 6 Fa0 = 5 7 alpha = 0.019 8 Ca = Ca0*(1-X)/(1+epsilon*X)*T/T0*y 9 Ua = 0.8 10 deltaCp = 1/2*20-40 11 Kc = 10000*exp(DH/8.314*(1/450-1/T)) 12 Cc = Ca0*X/2/(1+epsilon*X)*T0/T*y 13 m = 0.05 12-133 14 Cpc = 4200 15 k = 0.01*exp(8000/8.314*(1/450-1/T)) 16 ra = -k*(Ca^2-Cc/Kc) General Total number of equations 20 Number of differential equations 4 Number of explicit equations 16 Elapsed time 1.157 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 12-134 Now, counter – current heat exchanger POLYMATH Report Ordinary Differential Equations No Title 08-May-2009 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 alpha 0.019 0.019 0.019 0.019 2 Ca 1.9 0.7671508 1.910238 0.7671508 3 Ca0 1.9 1.9 1.9 1.9 4 Cc 0 0 0.2023329 0.1203647 5 Cp0 40. 40. 40. 40. 6 Cpc 4200. 4200. 4200. 4200. 7 deltaCp -30. -30. -30. -30. 8 DH -2.0E+04 -2.0E+04 -2.0E+04 9 epsilon -1. -1. -1. -1. 10 Fa0 5. 5. 5. 5. 11 k 0.01 0.01 0.025358 0.025358 12 Kc 10000. 976.5939 10000. 976.5939 13 m 0.05 0.05 0.05 0.05 -2.0E+04 12-135 14 ra -0.0361 -0.062846 -0.0149206 -0.0149206 15 T 450. 450. 796.6909 796.6909 16 T0 450. 450. 450. 450. 17 Ta 520. 500.0379 521.8302 500.0379 18 Ua 0.8 0.8 0.8 0.8 19 W 0 0 50. 50. 20 X 0 0 0.4958573 0.4958573 21 y 1. 0.2280604 1. 0.2280604 Differential equations 1 d(X)/d(W) = -ra/Fa0 2 d(y)/d(W) = -alpha/2/y*(1+epsilon*X)*T/T0 3 d(T)/d(W) = (ra*(DH+deltaCp*(T-298)) - Ua*(T-Ta))/Fa0/Cp0 4 d(Ta)/d(W) = - Ua*(T-Ta)/m/Cpc Explicit equations 1 Cp0 = 40 2 DH = -20000 3 epsilon = -1 4 T0 = 450 5 Ca0 = 1.9 6 Fa0 = 5 7 alpha = 0.019 8 Ca = Ca0*(1-X)/(1+epsilon*X)*T/T0*y 9 Ua = 0.8 10 deltaCp = 1/2*20-40 11 Kc = 10000*exp(DH/8.314*(1/450-1/T)) 12 Cc = Ca0*X/2/(1+epsilon*X)*T0/T*y 13 m = 0.05 14 Cpc = 4200 15 k = 0.01*exp(8000/8.314*(1/450-1/T)) 16 ra = -k*(Ca^2-Cc/Kc) General Total number of equations 20 12-136 Number of differential equations 4 Number of explicit equations 16 Elapsed time 0.000 sec Solution method RKF_45 Step size guess. h 0.000001 Truncation error tolerance. eps 0.000001 12-137 P12-20 (a) Liquid Phase : A B dX dV rA FA0 rA kC ACB k E 1 R T .01*exp C 1 300 C A C A0 (1 X ) CB The energy Balance: dT Ua(Ta T ) ( rA )( dV FA0 C pA C pB 4 D Assume D HR ) a U 4 5J 1cal 1m 2 m 2 Ks 4.184 J 10dm 2 .0120 cal dm 2 Ks See Polymath program P12-20-a.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 V 0 0 1000. 1000. 2 T 300. 300. 434.7779 348.2031 3 X 0 0 0.9620102 0.9620102 4 Ta 300. 300. 300. 300. 5 R 1.988 1.988 1.988 1.988 6 E 10000. 10000. 10000. 10000. 7 cao 0.1 0.1 0.1 0.1 8 ca 0.1 0.003799 0.1 0.003799 9 cb 0.1 0.003799 0.1 0.003799 10 k 0.01 0.01 1.808628 0.1018746 11 ra -0.0001 -0.0010427 -1.47E-06 -1.47E-06 12 cpb 15. 15. 15. 15. 13 cpa 15. 15. 15. 15. 14 fao 0.2 0.2 0.2 0.2 12-138 15 Dhr1 -6000. -6000. -6000. -6000. 16 a 1. 1. 1. 1. 17 U 0.012 0.012 0.012 0.012 Differential equations 1 d(T)/d(V) = (U * a * (Ta - T) + (-ra) * (-Dhr1)) / (fao * (cpa + cpb)) 2 d(X)/d(V) = -ra / fao Explicit equations 1 Ta = 300 2 R = 1.988 3 E = 10000 4 cao = .1 5 ca = cao * (1 - X) 6 cb = cao * (1 - X) 7 k = .01 * exp(-E / R * (1 / T - 1 / 300)) 8 ra = -k * ca * cb 9 cpb = 15 10 cpa = 15 11 fao = .2 12 Dhr1 = -6000 13 a = 1 14 U = .0120 12-139 P12-20 (b) Gas Phase: A dX rA dW FA0 B C rA k f CA k r CB CC CB CC CA0 X T0 1 X T k 0.133 exp E 1 R T kr 0.2exp Er 1 R 450 1 450 1 , Er T The energy Balance: dT Ua(Ta T ) ( rA )( dW FA0C pA HR U 51.4 kJ mol HR ) 40 50 70=-20 kJ/mol 5 See Polymath program P12-20-b.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 W 0 0 50. 50. 2 X 0 0 0.0560855 0.0560855 3 T 400. 371.902 400. 371.902 4 T0 400. 400. 400. 400. 5 k 0.133 0.0651696 0.133 0.0651696 6 v0 20. 20. 20. 20. 7 kr 0.2 0.0622149 0.2 0.0622149 8 Uarho 5. 5. 5. 5. 9 Ta 323. 323. 323. 323. 10 P0 1.013E+06 1.013E+06 1.013E+06 1.013E+06 11 CA0 304.6819 304.6819 304.6819 304.6819 12-140 12 CA 304.6819 292.8948 304.6819 292.8948 13 CC 0 0 17.40323 17.40323 14 CB 0 0 17.40323 17.40323 15 rA -40.52269 -40.52269 -0.2446624 -0.2446624 Differential equations 1 d(X)/d(W) = -rA / v0 / CA0 2 d(T)/d(W) = (Uarho * (Ta - T) + rA * 20000) / v0 / CA0 / 40 Explicit equations 1 T0 = 400 2 k = 0.133 * exp(31400 / 8.314 * (1 / T0 - 1 / T)) 3 v0 = 20 4 kr = 0.2 * exp(51400 / 8.314 * (1 / T0 - 1 / T)) 5 Uarho = 5 6 Ta = 323 7 P0 = 1013250 8 CA0 = P0 / 8.314 / T0 9 CA = CA0 * (1 - X) / (1 + X) * T0 / T 10 CC = CA0 * X / (1 + X) * T0 / T 11 CB = CA0 * X / (1 + X) * T0 / T 12 rA = -(k * CA - kr * CB * CC) 12-141 P12-21 First note that ΔCP = 0 for both reactions. This means that ΔHRx(T) = ΔHRx° for both reactions. Now start with the differential energy balance for a PFR: rij ( H Rxij ) Ua (Ta T ) r1 A ( H 1 A ) r2 B ( H Rx 2 B ) dT Ua (Ta T ) dV F j C Pj F j C Pj If we evaluate this differential equation at its maximum we get dT 0 and therefore, Ua (Ta T ) r1 A ( H Rx1C ) r2 B ( H Rx 2 B ) dV We can then solve for r1A from this information. Ua(Ta T ) r2 B ( H Rx 2 B ) r1 A ( H Rx1 A ) Ua(Ta T ) 2k 2 D C B CC ( H Rx 2 B ) r1 A ( H Rx1 A ) 10(325 500) 2(0.4)(0.2)(0.5)(5000) r1A 0.043 50000 1 1 r1 A 0.043 2 k1C C A C B 2 k1C (0.1)( 0.2) k1C 4 .3 k1C (500 ) 4.3 E 1 R 400 1 500 E 1 1.987 400 1 500 k1C ( 400 ) exp 0.043 exp cal mol Alternate Solution: E 18300 12-142 0 E = 76575 J /mol P12-22 T(K) CC 800 0.92 700 1.06 600 1.0755 500 0.78 650 1.1025 625 1.099 675 1.088 Ans: In the range between 300K to 600K, answer is 600K 600K 12-143 P12-23 Mole balance: dFA rA dW Rate Laws: rA r2 B dFB dW rB dFC dW rC r1 A r3 A rB r1 A r2 B rC r3 A r1 A k1C A r2 B k B CB r3 A k3CC Stoichiometry: FT C A CT A 0 FT T FBT0 FT T Energy balance: dT Ua(Ta T ) ( r1 A )( H R1 A ) ( rR 2 B ) ( r3 A )( dW FAC pA FBC pB FC C pC CB dT dW CT H R3 A ) 16(500 T ) ( r1 A )1800 ( rR 2 B )1800 ( r3 A )1100 100( FA FB FC ) k1 0.5exp 2(1 320 / T ) k2 k1 KC 12-144 k3 0.005exp 4.6(1 460 / T ) KC 10 exp 4.8(430 / T 1.5) See Polymath program P12-23.pol. Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 w 0 0 100. 100. 2 fb 1. 0.9261241 1.368476 0.9261241 3 fa 1. 0.6296429 1. 0.8694625 4 fc 0 0 0.2044134 0.2044134 5 T 330. 330. 416.3069 416.3069 6 Ua 16. 16. 16. 16. 7 Ta 500. 500. 500. 500. 8 Dhr1a -1800. -1800. -1800. -1800. 9 Dhr3a -1100. -1100. -1100. -1100. 10 cpa 100. 100. 100. 100. 11 cpb 100. 100. 100. 100. 12 cpc 100. 100. 100. 100. 13 k1 0.5312401 0.5312401 0.7941566 0.7941566 14 k3 0.0008165 0.0008165 0.0030853 0.0030853 15 ct 2. 2. 2. 2. 16 ft 2. 2. 2. 2. 17 To 330. 330. 330. 330. 18 Kc 3.885029 1.062332 3.885029 1.062332 19 k2 0.1367403 0.1367403 0.74756 0.74756 20 ca 1. 0.5682599 1. 0.6892094 21 cb 1. 0.7341242 1.253213 0.7341242 22 r1a -0.5312401 -0.5748799 -0.362406 -0.5473402 23 r3a -0.0008165 -0.002138 -0.0007594 -0.0021264 24 rc 0.0008165 0.0007594 0.002138 0.0021264 25 r2b -0.1367403 -0.5770243 -0.1367403 -0.5488019 12-145 26 rb 0.3944998 -0.0522707 0.3944998 -0.0014617 27 ra -0.3953164 -0.3953164 0.0510521 -0.0006647 Differential equations 1 d(fb)/d(w) = rb 2 d(fa)/d(w) = ra 3 d(fc)/d(w) = rc 4 d(T)/d(w) = (Ua * (Ta - T) + (-r1a) * (-Dhr1a) + (-r2b) * (Dhr1a) * (-r3a) * (-Dhr3a)) / (fa * cpa + fb * cpb + fc * cpc) Explicit equations 1 Ua = 16 2 Ta = 500 3 Dhr1a = -1800 4 Dhr3a = -1100 5 cpa = 100 6 cpb = 100 7 cpc = 100 8 k1 = .5 * exp(2 * (1 - 320 / T)) 9 k3 = .005 * exp(4.6 * (1 - (460 / T))) 10 ct = 2 11 ft = 2 12 To = 330 13 Kc = 10 * exp(4.8 * (430 / T - 1.5)) 14 k2 = k1 / Kc 15 ca = ct * fa / ft * To / T 16 cb = ct * fb / ft * To / T 17 r1a = -k1 * ca 18 r3a = -k3 * ca 19 rc = -r3a 20 r2b = -k2 * cb 12-146 21 rb = -r1a + r2b 22 ra = -r2b + r1a + r3a P12-23 (a) As seen in the above table, the lowest concentration of o-xylene (A) = .568 mol/dm3 P12-23 (b) The maximum concentration of m-xylene (B) = 1.253 mol/dm3 P12-23 (c) The maximum concentration of o-xylene = 1 mol/dm3 P12-23 (d) The same equations are used except that FB0 = 0. The lowest concentration of o-xylene = 0.638 mol/dm3. The highest concentration of m-xylene = 1.09 mol/dm3. The maximum concentration of o-xylene = 2 mol/dm3. P12-23 (e) Decreasing the heat of reaction of reaction 1 slightly decreases the amount of E formed. Decreasing the heat of reaction of reaction 3 causes more of C to be formed. Increasing the feed temperature causes less of A to react and increases formation of C. Increasing the ambient temperature causes a lot of C to be formed. P12-23 (f) Individualized solution P12-24 (a) A B C A D E A C F G We want the exiting flow rates B, D and F Start with the mole balance in PFR: dFC dFA dFB rA rB dV dV dV dFE dFF rE rF dV dV Rate Laws: rA r1s rB r1s rC r1s r3T rD r2 B rE r2 B rF r3T r2 B r3T 12-147 rC dFD dV dFG dV rG rD r1s (1 r2 B (1 r3T (1 10925 PA T 25000 ) exp 13.2392 PA T 11000 ) exp 0.2961 PA PC T ) exp 0.08359 FB FD PB PC K Stoichiometry: PA FA PT 0 FT PB FB PT 0 FT PC FC PT 0 FT FT FA FI steamratio .0034 FC FE FF FG FI Energy Balance: dT dV r1s H R1 A r2 B H R 2 A r3T H R 3 A FA *299 FB *283 FC *30 FD *201 FE *90 FF *249 FG *68 FI *40 K p1 exp b1 b2 T b3 ln(T ) (b4T b5 )T b6 T See Polymath program P12-24.pol. For T0 = 800K Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 v 0 0 10. 10. 2 fa 0.00344 0.002496 0.00344 0.002496 3 fb 0 0 0.0008974 0.0008974 4 fc 0 0 0.0008615 0.0008615 5 fd 0 0 1.078E-05 1.078E-05 6 fe 0 0 1.078E-05 1.078E-05 7 ff 0 0 3.588E-05 3.588E-05 12-148 8 fg 0 0 3.588E-05 3.588E-05 9 T 800. 765.237 800. 765.237 10 Hla 1.18E+05 1.18E+05 1.18E+05 1.18E+05 11 H2a 1.052E+05 1.052E+05 1.052E+05 1.052E+05 12 H3a -5.39E+04 -5.39E+04 -5.39E+04 -5.39E+04 13 p 2137. 2137. 2137. 2137. 14 phi 0.4 0.4 0.4 0.4 15 Kl 0.0459123 0.0196554 0.0459123 0.0196554 16 sr 14.5 14.5 14.5 14.5 17 fi 0.04988 0.04988 0.04988 0.04988 18 ft 0.05332 0.05332 0.0542282 0.0542282 19 Pa 0.1548387 0.1104652 0.1548387 0.1104652 20 Pb 0 0 0.0397155 0.0397155 21 Pc 0 0 0.0381277 0.0381277 22 r2b 2.991E-06 5.16E-07 2.991E-06 5.16E-07 23 rd 2.991E-06 5.16E-07 2.991E-06 5.16E-07 24 re 2.991E-06 5.16E-07 2.991E-06 5.16E-07 25 r3t 0 0 4.196E-06 4.151E-06 26 rf 0 0 4.196E-06 4.151E-06 27 rg 0 0 4.196E-06 4.151E-06 28 rls 0.0002138 2.481E-05 0.0002138 2.481E-05 29 rb 0.0002138 2.481E-05 0.0002138 2.481E-05 30 rc 0.0002138 2.066E-05 0.0002138 2.066E-05 31 ra -0.0002167 -0.0002167 -2.948E-05 -2.948E-05 Differential equations 1 d(fa)/d(v) = ra 2 d(fb)/d(v) = rb 3 d(fc)/d(v) = rc 4 d(fd)/d(v) = rd 5 d(fe)/d(v) = re 12-149 6 d(ff)/d(v) = rf 7 d(fg)/d(v) = rg 8 d(T)/d(v) = -(rls * Hla + r2b * H2a + r3t * H3a) / (fa * 299 + fb * 273 + fc * 30 + fd * 201 + fe * 90 + ff * 68 + fi * 40) Explicit equations 1 Hla = 118000 2 H2a = 105200 3 H3a = -53900 4 p = 2137 5 phi = .4 6 Kl = exp(-17.34 - 1.302e4 / T + 5.051 * ln(T) + ((-2.314e-10 * T + 1.302e-6) * T + -0.004931) * T) 7 sr = 14.5 8 fi = sr * .00344 9 ft = fa + fb + fc + fd + fe + ff + fg + fi 10 Pa = fa / ft * 2.4 11 Pb = fb / ft * 2.4 12 Pc = fc / ft * 2.4 13 r2b = p * (1 - phi) * exp(13.2392 - 25000 / T) * Pa 14 rd = r2b 15 re = r2b 16 r3t = p * (1 - phi) * exp(.2961 - 11000 / T) * Pa * Pc 17 rf = r3t 18 rg = r3t 19 rls = p * (1 - phi) * exp(-0.08539 - 10925 / T) * (Pa - Pb * Pc / Kl) 20 rb = rls 21 rc = rls - r3t 22 ra = -rls - r2b - r3t Fstyrene = 0.0008974 Fbenzene = 1.078E-05 12-150 Ftoluene = 3.588E-05 SS/BT = 19.2 P12-24 (b) T0 = 930K Fstyrene = 0.0019349 Fbenzene = 0.0002164 Ftoluene = 0.0002034 SS/BT = 4.6 P12-24 (c) T0 = 1100 K Fstyrene = 0.0016543 Fbenzene = 0.0016067 Ftoluene = 0.0001275 SS/BT = 0.95 P12-24 (d) Plotting the production of styrene as a function of To gives the following graph. The temperature that is ideal is 995K P12-24 (e) Plotting the production of styrene as a function of the steam gives the following graph and the ratio that is the ideal is 25:1 12-151 P12-24 (f) When we add a heat exchanger to the reactor, the energy balance becomes: Ua Ta T r1s H R1 A r2 B H R 2 A r3T H R 3 A dT dV FA *299 FB *283 FC *30 FD *201 FE *90 FF *249 FG *68 FI *40 With Ta = 1000 K Ua = 100 kJ/min/K = 1.67 kJ/s/K The recommended entering temperature would be T0 = 440 K. This gives the highest outlet flow rate of styrene. P12-24 (g) Individualized solution P12-24 (h) Individualized solution P12-25 Let a=A b = A2 c = A4 PART 1 POLYMATH Report Ordinary Differential Equations 21-Jun-2010 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 12-152 1 Ca 2. 0.155599 2. 0.155599 2 Cb 0 0 0.4963834 0.1995088 3 Cpa 25. 25. 25. 25. 4 Cpb 50. 50. 50. 50. 5 Cpc 100. 100. 100. 100. 6 DH1a -3.25E+04 -3.25E+04 -3.25E+04 -3.25E+04 7 DH2b -2.75E+04 -2.75E+04 -2.75E+04 -2.75E+04 8 E1 4000. 4000. 4000. 4000. 9 E2 5000. 5000. 5000. 5000. 10 Fa 100. 7.779951 100. 7.779951 11 Fb 0 0 24.81917 9.975439 12 Fc 0 0 18.06729 18.06729 13 k1 0.6 0.6 0.6 0.6 14 k1a 0.6 0.6 76.97387 6.133163 15 k2 0.35 0.35 0.35 0.35 16 k2b 0.2072016 0.2072016 89.46089 3.787125 17 Qg 7.8E+04 8971.335 1.569E+06 8971.335 18 Qr -1.5E+04 -1.5E+04 7.696E+05 1.44E+05 19 r1a -2.4 -42.01417 -0.1484903 -0.1484903 20 r1b 1.2 0.0742452 21.00708 0.0742452 21 r2b 0 -18.03538 0 -0.1507418 22 ra -2.4 -42.01417 -0.1484903 -0.1484903 23 rb 1.2 -8.261933 17.21274 -0.0764966 24 rc 0 0 9.017691 0.0753709 25 sumCp 2500. 2500. 2500. 2500. 26 T 300. 300. 1084.641 459.0062 27 T1 300. 300. 300. 300. 28 T2 320. 320. 320. 320. 29 Ta 315. 315. 315. 315. 30 Ua 1000. 1000. 1000. 1000. 31 V 0 0 10. 10. 32 vo 50. 50. 50. 50. Differential equations 12-153 1 d(T)/d(V) = (Qg-Qr)/sumCp 2 d(Fc)/d(V) = rc 3 d(Fb)/d(V) = rb 4 d(Fa)/d(V) = ra Explicit equations 1 Cpc = 100 2 Cpb = 50 3 Cpa = 25 4 k2 = .35 5 Ta = 315 6 Ua = 1000 7 DH2b = -27500 8 DH1a = - 32500 9 T1 = 300 10 E1 = 4000 11 k1 = 0.6 12 T2 = 320 13 E2 = 5000 14 k2b = k2*exp((E2/1.987)*(1/T2-1/T)) 15 vo = 50 16 Cb = Fb/vo 17 Ca = Fa/vo 18 sumCp = (Fa*Cpa+Fb*Cpb+Fc*Cpc) 19 k1a = k1*exp((E1/1.987)*(1/T1-1/T)) 20 r2b = -k2b*Cb^2 21 rc = -r2b/2 22 r1a = -k1a*Ca^2 23 r1b = -r1a/2 24 rb = r1b + r2b 25 ra = r1a 26 Qg = r1a*DH1a+r2b*DH2b 27 Qr = Ua*(T-Ta) 12-154 (b) The required reactor volume = 3.5 dm3 (c) 12-155 Part 2 12-156 12-157 P12-26 Let A = a A3 = b, A6 = c k1 = k1A and k2 = k2A3 Thus the values of quantities exiting the reactor are as follows: FA = 23.15 mol/sec FA3 = 11.906 mol/sec FA6 = 6.85 mol/sec T = 589.73 K POLYMATH Report Nonlinear Equations 21-Jun-2010 Calculated values of NLE variables Variable Value f(x) Initial Guess 12-158 1 Fa 23.15856 -4.263E-14 30. 2 Fb 11.90629 1.243E-14 30. 3 Fc 6.85376 8.882E-16 2. 4T 589.7334 -2.328E-10 1000. Variable Value 1 Ca 0.5620827 2 Cb 0.2889783 3 Cpa 25. 4 Cpb 75. 5 Cpc 150. 6 Cto 2. 7 DH1a -8.0E+04 8 DH2b -1.0E+05 9 E1 4000. 10 E2 5000. 11 Fao 100. 12 Ft 41.91861 13 k1 0.9 14 k1a 24.32177 15 k2 0.45 12-159 16 k2b 16.41453 17 Qg 7.518E+05 18 Qr 7.518E+05 19 r1a -7.684144 20 r1b 2.561381 21 r2b -1.370752 22 ra -7.684144 23 rb 1.190629 24 rc 0.685376 25 T1 300. 26 T2 320. 27 Ta 315. 28 To 300. 29 UA 100. 30 V 10. Nonlinear equations 1 f(T) = (Qr - Qg) = 0 2 f(Fc) = 0 -Fc+rc*V = 0 3 f(Fb) = 0 - Fb + rb*V = 0 4 f(Fa) = Fao-Fa+ra*V = 0 12-160 Explicit equations 1 Cpc = 150 2 Cpb = 75 3 Cpa = 25 4 k2 = 0.45 5 Ta = 315 6 UA = 100 7 DH1a = -80000 8 DH2b = -100000 9 T1 = 300 10 E1 = 4000 11 k1 = 0.9 12 T2 = 320 13 E2 = 5000 14 k2b = k2*exp((E2/1.987)*(1/T2-1/T)) 15 Cto = 2 16 Ft = Fa + Fb + Fc 17 To = 300 18 Cb = Fb/Ft*Cto*To/T 19 Ca = Fa/Ft*Cto*To/T 12-161 20 k1a = k1*exp((E1/1.987)*(1/T1-1/T)) 21 r2b = - k2b*Cb^2 22 rc = -r2b/2 23 r1a = -k1a*Ca^2 24 r1b = -r1a/3 25 rb = r1b + r2b 26 ra = r1a 27 Qg = r1a*DH1a+r2b*DH2b 28 Fao = 100 29 Qr = UA*(T-Ta)+Fao*Cpa*(T-To) 30 V = 10 12-162 CD12GA1 12-163 12-164 12-165 12-166 See Polymath program CD12GA-1.pol. 12-167 POLYMATH Results Calculated values of the DEQ variables Variable initial value minimal value maximal value final value V 0 0 1.0E+08 1.0E+08 X 0 0 0.6495463 0.6495463 Fao 1200 1200 1200 1200 T 550 225.22683 550 225.22683 Cao 0.064 0.064 0.064 0.064 To 550 550 550 550 k 1.949E+05 5.047E-05 1.949E+05 5.047E-05 Kc 1.01E+06 1841.4832 1.01E+06 1841.4832 f 1 1 2.4419826 2.4419826 Ca 0.064 0.0547713 0.064 0.0547713 Cb 0.064 0.0547713 0.064 0.0547713 Cc 0 0 0.2030311 0.2030311 ra -798.17344 -798.17344 -1.503E-07 -1.503E-07 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(V) = -ra/Fao Explicit equations as entered by the user [1] Fao = 1200 [2] T = -500*X+550 [3] Cao = .064 [4] To = 550 [5] k = .035*exp(8419.5*(1/273-1/T)) [6] Kc = 25000*exp(2405.6*(1/298-1/T)) [7] f = To/T [8] Ca = Cao*(1-X)*f [9] Cb = Cao*(1-X)*f [10] Cc = 2*Cao*X*f [11] ra = -k*(Ca*Cb-Cc^2/Kc) 12-168 CD12GA2 12-169 See Polymath program CD12GA-2.pol. POLYMATH Results NLES Solution Variable Value f(x) Ini Guess Ca 0.0016782 -1.472E-16 0.0017 Cb 0.0016782 -1.472E-16 0.0017 Cd 0.0071436 -1.154E-16 0.0072 Cu 0.0011782 -2.017E-17 0.0012 V 3794.94 1.018E-09 3794 Cao 0.01 Cbo 0.01 vo 6000 k1 6.73 k2 1.11 tau 0.63249 rd 0.0112944 ru 0.0018628 ra -0.0131572 rb -0.0131572 NLES Report (safenewt) Nonlinear equations [1] f(Ca) = tau*ra+Cao-Ca = 0 [2] f(Cb) = tau*rb+Cbo-Cb = 0 [3] f(Cd) = Cd-tau*rd = 0 [4] f(Cu) = Cu-tau*ru = 0 [5] f(V) = 171000/(20190*Ca+6660*Cb)-V = 0 Explicit equations [1] Cao = .01 [2] Cbo = .01 [3] vo = 6000 [4] k1 = 6.73 12-170 [5] k2 = 1.11 [6] tau = V/vo [7] rd = k1*Ca [8] ru = k2*Cb [9] ra = -k1*Ca-k2*Cb [10] rb = ra CD12GA 2 (a) CD12GA 2 (b) CD12GA 2 (c) Individualized solution ______________________________________________________________________________ 12-171 The authors and the publisher have taken care in the preparation of this book but make no expressed or implied warranty of any kind and assume no responsibility for errors or omissions. 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All the recipient of this work are expected to abide by these restrictions and to honor the intended pedagogical purposes and the needs of the other instructors who rely on these materials . 13-1 Solutions for Chapter 13 – Unsteady State Non-isothermal Reactor Design P13-1 Individualized solution P13-2 (a) Example 13-1 (1) If the heat of mixing had been neglected, the shape of the graphs would have been as follows: (2) The new T0 of 20 ˚F (497 ˚R) gives a new HRn and T. With T=497+89.8X the polymath program of example 9-1 gives t= 8920 s for 90 % conversion. 13-2 (3) Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 t 0 0 9000. 9000. 2 X 0 0 1. 1. 3 T 480. 480. 894.193 894.193 4 k 8.307E-06 8.307E-06 56.65781 56.65781 5 Ta 896.4 896.4 896.4 896.4 6 Ua 0.22 0.22 0.22 0.22 7 Qr 91.608 0.4855311 91.608 0.4855311 8 V 1.2 1.2 1.2 1.2 9 Nao 1. 1. 1. 1. 10 NiCpi 403. 403. 403. 403. 11 Ca 0.8333333 -5.468E-07 0.8333333 -1.392E-09 12 ra -6.923E-06 -0.0038571 8.639E-06 7.887E-08 13 Qg -0.3016323 -168.055 0.3763917 0.0034364 Differential equations 1 d(X)/d(t) = k * (1 - X) 2 d(T)/d(t) = (Qr - (-36309) * (-ra) * V) / NiCpi Explicit equations 1 k = 0.000273 * exp(16306 * ((1 / 535) - (1 / T))) 2 Ta = 896.4 3 Ua = .22 4 Qr = Ua * (Ta - T) 5 V = 1.2 6 Nao = 1 7 NiCpi = 403 8 Ca = (Nao/V) * (1 - X) 9 ra = -k * Ca 10 Qg = (-36309) * (-ra) * V 13-3 P13-2 (b) Example 13-2 To show that no explosion occurred without cooling failure. 13-4 P13-2 (c) Example 13-3 Decreasing the coolant rate to 10 kg/s gives a weak cooling effect and the maximum temperature in the reactor becomes 315 K. An increase of the coolant rate to 1000 kg/s gives a Tmax of 312 K. A big change to the coolant rate has, in this case, only a small effect on the temperature, and because the temperature does not change significantly the conversion will be kept about the same. P13-2 (d) Example 13-4 13-5 13-6 P13-2 (e) Example 13-5 Using the code from Example 9-5, we could produce the following graphs either by changing TO and finding the steady state conversion or changing the coolant flow rate and finding the steady state conversion and temperature. These are the graphs of those: 13-7 P13-2 (f) Example 13-6 (1) Individualised solution (2) The transition to runaway occurs over a very small range of Ua . If U a value is changed such that Ua is taken from 2.1 ×104 to 1.9 ×104 J/hr/K the runaway occurs. Thus it occurred over a very narrow range of Ua values . (3) The modelling is done and the changes are incorporated in the polymath code for Example 13.6 A new switch type variable is introduced . 13-8 Sw2 such that Sw2 = 1 if 300<T<422 else 0 and a new term is added in the energy equation such that the equation becomes : d(T)/d(t) = SW1*((V0*(r1A*DHRx1A+r2S*DHRx2S)-SW1*UA*(T – 373.15))/SumNCp) + SW1*Sw2*4/60 Case 1: When Ua = 2.77 × 106 J/hr/K But the cooling starts only for T>455K Thus Ua = 2.77 × 106 J/hr/K , T> 455K = 0 for T< 455K See polymath Program for part 3 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 A1A 4.0E+14 4.0E+14 4.0E+14 4.0E+14 2 A2S 1.0E+84 1.0E+84 1.0E+84 1.0E+84 3 CA 4.3 0.0457129 4.3 0.0457129 4 CB 5.1 0.8457129 5.1 0.8457129 5 CS 3. 2.999997 3. 2.999997 6 Cv1 3360. 3360. 3360. 3360. 7 Cv2 5.36E+04 5.36E+04 5.36E+04 5.36E+04 8 DHRx1A -4.54E+04 -4.54E+04 -4.54E+04 -4.54E+04 9 DHRx2S -3.2E+05 -3.2E+05 -3.2E+05 -3.2E+05 10 E1A 1.28E+05 1.28E+05 1.28E+05 1.28E+05 11 E2S 8.0E+05 8.0E+05 8.0E+05 8.0E+05 12 FD 2467.445 61.27745 8874.034 61.27745 13 Fvent 2467.445 61.27745 8874.034 61.27745 14 k1A 0.0562573 0.0562573 1.82787 0.7925113 15 k2S 8.428E-16 8.428E-16 2.367E-06 1.276E-08 16 P 4.4 4.4 4.4 4.4 17 r1A -1.233723 -4.437017 -0.0306385 -0.0306385 18 r2S -2.529E-15 -7.102E-06 -2.529E-15 -3.829E-08 19 SumNCp 1.26E+07 1.26E+07 1.26E+07 1.26E+07 20 SW1 1. 1. 1. 1. 21 Sw2 0 0 0 0 13-9 22 T 422. 422. 466.4882 454.9731 23 t 0 0 4. 4. 24 UA 0 0 2.77E+06 0 25 V0 4000. 4000. 4000. 4000. 26 VH 5000. 5000. 5000. 5000. Differential equations 1 d(CA)/d(t) = SW1*r1A mol/dm3/hr 2 d(CB)/d(t) = SW1*r1A change in concentration of cyclomethylpentadiene 3 d(CS)/d(t) = SW1*r2S change in concentration of diglyme 4 d(P)/d(t) = SW1*((FD-Fvent)*0.082*T/VH) 5 d(T)/d(t) = SW1*((V0*(r1A*DHRx1A+r2S*DHRx2S)-SW1*UA*(T-373.15))/SumNCp) + SW1*Sw2*4/60 Explicit equations 1 V0 = 4000 dm3 2 VH = 5000 dm3 3 DHRx1A = -45400 J/mol Na 4 DHRx2S = -3.2E5 J/mol of Diglyme 5 SumNCp = 1.26E7 J/K 6 A1A = 4E14 per hour 7 E1A = 128000 J/kmol/K 8 k1A = A1A*exp(-E1A/(8.31*T)) rate constant reaction 1 9 A2S = 1E84 per hour 10 E2S = 800000 13-10 J/kmol/K 11 k2S = A2S*exp(-E2S/(8.31*T)) rate constant reaction 2 12 SW1 = if (T>600 or P>45) then (0) else (1) 13 r1A = -k1A*CA*CB mol/dm3/hour (first order in sodium and cyclomethylpentadiene) 14 r2S = -k2S*CS mol/dm3/hour (first order in diglyme) 15 FD = (-0.5*r1A-3*r2S)*V0 16 Cv2 = 53600 17 Cv1 = 3360 18 Fvent = if (FD<11400) then (FD) else(if (P<28.2) then ((P-1)*Cv1) else ( (P-1)*(Cv1 +Cv2))) 19 UA = if T> 455 then (2.77e6) else (0) no cooling 20 Sw2 = if ((T>300) and (T<422)) then (1) else (0) 13-11 (4) Solving the equations with Ua = 0 for the entirety of the process, we get that the temperature reaches at 0.94 hours while the system reaches runaway at 3.649 hours. This implies the maximum time in minutes that the cooling can be lost is 163 minutes. 13-12 P13-2 (g) Example RE13-1 P13-2 (h) Example RE13-2 13-13 P13-2 (i) No solution will be given P13-3 After the feed was shut off, See Polymath program P13-3.pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cpa 0.38 0.38 0.38 0.38 2 dH -336. -336. -336. -336. 3 k 0.0081711 0.0081711 4.285E+17 4.285E+17 4 T 980. 980. 3.302E+20 3.302E+20 5 t 0 0 4. 4. Differential equations 1 d(T)/d(t) = -dH * k / Cpa Explicit equations 1 dH = -336 2 Cpa = .38 3 k = (0.307/60)* exp(44498 * (1 / 970 - 1 / T)) 13-14 As can be seen from the above plots, temperature shoots at time t = 3.16 mins Since NA doesn’t come in the temperature equation, there will not be any effect of feed present in the reactor. 0 If T0 = 100 F, Temperature will remain constant for next 4 minutes, which means no explosion. 0 If T0 = 500 F, there will not be any explosion and the temperature profile will look like 13-15 P13-4 (a) See Polymath program P13-4-a.pol 13-16 Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cbo 10. 10. 10. 10. 2 Fbo 10. 0 10. 0 3 k 0.0089352 0.0089352 10.08511 10.08511 4 Na 500. 0.1396707 500. 0.1396707 5 Nao 500. 500. 500. 500. 6 Nb 0 0 42.43357 0.1397745 7 Nc 0 0 499.8603 499.8603 8 Qg 0 0 1.24E+05 11.81314 9 Qr 0 0 0 0 10 ra 0 -0.3460808 0 -1.969E-05 11 T 298. 298. 510.4441 510.4441 12 t 0 0 120. 120. 13 V 50. 50. 100. 100. 14 vo 1. 0 1. 0 15 X 0 0 0.9997207 0.9997207 Differential equations 1 d(Na)/d(t) = ra*V 2 d(Nb)/d(t) = ra*V+Fbo 3 d(Nc)/d(t) = -ra*V 4 d(T)/d(t) = ((6000*(-ra*V))-(Fbo*15*(T-323)))/(15*Na+15*Nb+30*Nc) 5 d(X)/d(t) = -ra*V/Nao Explicit equations 1 Fbo = if(t<50)then(10)else(0) 2 Nao = 500 3 Cbo = 10 4 k = .01*exp((10000/1.987)*(1/300-1/T)) 5 vo = Fbo/Cbo 6 V = if(t<50)then(50+(vo*t))else(100) 7 ra = -k*Na*Nb/(V^2) 8 Qg = -6000*ra*V 9 Qr = 0 13-17 P13-4 (b) This is the same as part (a) except the energy balance. Energy balance: 13-18 See Polymath program P13-4-b.pol P13-4 (c) This is the same as part (b) except the reaction is now reversible. 13-19 See Polymath program P13-4-c.pol 13-20 P13-5 (a) P13-5 (b) 13-21 P13-6 13-22 See Polymath program P13-6.pol POLYMATH Results Calculated values of the DEQ variables Variable t X T k1 Ca Cb k2 Cc ra initial value 0 0 373 0.002 0.1 0.125 3.0E-05 0 -2.236E-04 minimal value 0 0 373 0.002 0.0749517 0.0999517 3.0E-05 0 -0.1344598 maximal value 10 0.2504829 562.91803 106.13627 0.1 0.125 366.75159 0.0250483 8.644E-06 ODE Report (RKF45) Differential equations as entered by the user [1] d(X)/d(t) = -ra/.1 [2] d(T)/d(t) = ((40000+(10*(T-298)))*(-ra)*(1/.1))/(56.25-(10*X)) Explicit equations as entered by the user [1] k1 = .002*exp((100000/8.314)*(1/373-1/T)) [2] Ca = .1*(1-X) [3] Cb = .1*(1.25-X) [4] k2 = .00003*exp((150000/8.314)*(1/373-1/T)) [5] Cc = .1*X [6] ra = -((k1*(Ca^.5)*(Cb^.5))-(k2*Cc)) 13-23 final value 10 0.2504829 562.91802 106.13612 0.0749517 0.0999517 366.75083 0.0250483 1.3E-07 P13-7 (a) Use Polymath to solve the differential equations developed from the unsteady state heat and mass balances. Refer to P13-7-a.pol POLYMATH Results Calculated values of the DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Cc 0.1 0.1 14.25628 14.25628 2 Cpc 4.2 4.2 4.2 4.2 3 Cps 5. 5. 5. 5. 4 Cs 300. 282.3047 300. 282.3047 5 Hrxn -2.0E+04 -2.0E+04 -2.0E+04 -2.0E+04 6 Iprime 0.0866522 0.0004366 0.3898631 0.0004366 7 Km 5. 5. 5. 5. 8 mu 0.0426159 0.0002145 0.1916769 0.0002145 9 mu1max 0.5 0.5 0.5 0.5 10 neg_rs 0.005327 0.0038221 1.083901 0.0038221 11 Q 0 0 0 0 13-24 12 rg 0.0042616 0.0030577 0.8671209 0.0030577 13 rho 1000. 1000. 1000. 1000. 14 rs -0.005327 -1.083901 -0.0038221 -0.0038221 15 t 0 0 300. 300. 16 T 278. 278. 334.6251 334.6251 17 V 25. 25. 25. 25. 18 Ycs 0.8 0.8 0.8 0.8 ODE Report (STIFF) Differential equations as entered by the user [1] d(Cc)/d(t) = rg [2] d(Cs)/d(t) = -rg/Ycs [3] d(T)/d(t) = (Q+(-Hrxn)*(rg))/(rho*Cps) Explicit equations as entered by the user [1] Iprime = (0.0038*T*exp(21.6-6700/T))/(1+exp(153-48000/T)) [2] Km = 5.0 [3] mu1max = 0.5 [4] Ycs = 0.8 [5] mu = mu1max*Iprime*(Cs/(Km+Cs)) [6] Q = 0 [7] Cps = 5 [8] Hrxn = -20000 [9] V = 25 [10] rho = 1000 [11] rg = mu*Cc [12] Cpc = 4.2 [13] rs = -rg/Ycs 13-25 P13-7 (b) When we change the initial temperature we find that the outlet concentration of species C has a maximum at T0 = 300 K. Refer to P13-7-b.pol P13-7 (c) 13-26 Cc can be maximized with respect to T0 (inlet temp), Ta (coolant/heating temperature), and heat exchanger area. Therefore, if we are to find the optimal heat exchanger area the inlet temperature and coolant/heating temperature needs to be specified. If we take T0 = 310 and Ta = 290 we find that the optimal heat exchanger area is 0.46 m2.The concentration of cells at the end of 24 hrs under these conditions is 21.55 g/dm3 . Refer to P13-7-c.pol. The plot of Cc Vs A: P13-8 (a) 13-27 See Polymath program P13-8-a.pol POLYMATH Results Calculated values of the DEQ variables Variable t Na Nb Nc X T vb k V Fbo Ca Cb Cc ra initial value 0 50 0 0 0 300 1.5 5.0E-04 10 6 5 0 0 0 minimal value 0 0.3324469 0 0 0 283.60209 1.5 2.3E-04 10 6 2.202E-04 0 0 -0.0028611 maximal value 1000 50 5900.6649 49.667553 0.9933511 300 1.5 5.0E-04 1510 6 5 3.9077251 0.0718765 0 final value 1000 0.3324469 5900.6649 49.667553 0.9933511 298.76383 1.5 4.73E-04 1510 6 2.202E-04 3.9077251 0.0328924 -1.59E-06 ODE Report (RKF45) Differential equations as entered by the user [1] d(Na)/d(t) = ra*V [2] d(Nb)/d(t) = 2*ra*V+Fbo [3] d(Nc)/d(t) = -ra*V [4] d(X)/d(t) = -ra*V/50 [5] d(T)/d(t) = ((250*(290-T))-(80*vb*(T-325))+(-55000*(-ra*V)))/(35*Na+20*Nb+75*Nc) 13-28 Explicit equations as entered by the user [1] vb = 1.5 [2] k = .0005*exp((8000/1.987)*(1/300-1/T)) [3] V = 10+(vb*t) [4] Fbo = 4*vb [5] Ca = Na/V [6] Cb = Nb/V [7] Cc = Nc/V [8] ra = -k*Ca*Cb^2 13-29 P13-8 (b) P13-9 13-30 P13-9 (a) See Polymath program P13-9-a.pol POLYMATH Results Calculated values of the DEQ variables Variable t Ca Cc Cb T UA V k1 k2 ra1 rb2 rb1 initial value 0 0.3 0 0 283 0 10 1.1172964 4.081E-09 -0.3351889 0 0.3351889 minimal value 0 1.34E-65 0 -2.02E-44 283 0 10 1.1172964 4.081E-09 -35.016552 -27.963241 -6.345E-60 maximal value 0.2 0.3 0.3 0.2895784 915.5 0 10 2.141E+05 1.041E+06 6.345E-60 2.103E-38 35.016552 ODE Report (STIFF) Differential equations as entered by the user [1] d(Ca)/d(t) = ra1 [2] d(Cc)/d(t) = -rb2 13-31 final value 0.2 1.34E-65 0.3 -1.864E-65 915.5 0 10 2.141E+05 1.041E+06 6.345E-60 -3.974E-59 -6.345E-60 [3] d(Cb)/d(t) = rb1+rb2 [4] d(T)/d(t) = ((UA*(330-T))+(55000*(-ra1*V))+(71500*(-rb2*V)))/(200*V*(Ca+Cb+Cc)) Explicit equations as entered by the user [1] UA = 0 [2] V = 10 [3] k1 = 3.03*exp((9900/1.987)*(1/300-1/T)) [4] k2 = 4.58*exp((27000/1.987)*(1/500-1/T)) [5] ra1 = -k1*Ca [6] rb2 = -k2*Cb [7] rb1 = -ra1 P13-9 (b) 13-32 P13-9 (c) 13-33 P13-10 Semi batch with parallel reactions dNa dt dNb dt dNd dt dNu dt r1 r2 V Fbo r1 r2 V r1 V r2 V Rate laws: r1 k1 Ca r2 k2.Cb k1 10 exp( 2000 / T) k2 20 exp( 3000 / T) Stoichiometry: Na V Nd Cd V V V0 v b t Ca Cb Cu Fbo Cbo Cao 5mol / dm 3 Nb V Nu V vb Cbo 1mol / dm 3 13-34 dT dt 3000( r1 V) [5000 10(T 300)]( r2 V) 30 Fbo (T Tbo) 20Na 30Nb 50Nd 40Nu See polymath program P13-10.pol Calculated values of DEQ variables Variable Initial value Minimal value Maximal value Final value 1 Ca 5. 0.0402932 5. 0.0402932 2 Cao 5. 5. 5. 5. 3 Cb 1. 0.1879238 1. 0.3260075 4 Cbo 1. 1. 1. 1. 5 Cd 0 0 0.7888994 0.6235848 6 Cu 0 0 0.0504077 0.0504077 7 Fbo 10. 10. 10. 10. 8 k1 0.0204583 0.0204583 0.0464803 0.0460806 9 k2 0.0018507 0.0018507 0.0063377 0.0062561 10 Na 500. 28.20523 500. 28.20523 11 Nb 100. 68.89056 228.2052 228.2052 12 Nd 0 0 436.5094 436.5094 13 Nu 0 0 35.28541 35.28541 14 r1 -0.1022916 -0.1022916 -0.0018567 -0.0018567 15 r2 -0.0018507 -0.0020395 -0.001066 -0.0020395 16 T 323. 323. 372.3484 371.7507 17 t 0 0 60. 60. 18 Tao 373. 373. 373. 373. 19 Tbo 323. 323. 323. 323. 20 V 100. 100. 700. 700. 21 vb 10. 10. 10. 10. Differential equations 1 d(Na)/d(t) = (r1+r2)*V 2 d(Nb)/d(t) = Fbo + (r1+r2)*V 3 d(Nd)/d(t) = -r1*V 13-35 4 d(Nu)/d(t) = -r2*V 5 d(T)/d(t) = (-30*Fbo*(T-Tbo) + 3000*(-r1*V) + (5000 + 10*(T-300))*(r2*V))/(20*Na+30*Nb+50*Nd+40*Nu) Explicit equations 1 Cbo = 1 2 Fbo = 10 3 k1 = 10*exp(-2000/T) 4 k2 = 20*exp(-3000/T) 5 vb = Fbo/Cbo 6 V = 100 + vb*t 7 Ca = Na/V 8 Cb = Nb/V 9 r1 = -k1*Ca 10 r2 = -k2*Cb 11 Cao = 5 12 Cd = Nd/V 13 Tao = 373 14 Tbo = 323 15 Cu = Nu/V 13-36 13-37