Thermochemistry - Energy of Chemical Reactions Contents: • heat, work, forms of energy • specific heat and energies of phase changes • enthalpy changes in chemical reactions • standard enthalpies of formation • Hess’s law • estimating enthalpies of reaction from Bond Energies 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 1 CHEMICAL ENERGY Chemical bonds are a source of energy • BOND BREAKING - requires energy • BOND MAKING - releases energy In a chemical reaction: • if more energy is released in forming bonds than is used in breaking bonds then . . . reaction is EXOTHERMIC Energy is released as HEAT, LIGHT, SOUND, WORK • if more energy is used in breaking bonds than is released in forming bonds then . . . reaction is ENDOTHERMIC Energy can be provided by 22 September, 1997 Chem 1A03E/1E03E - LIGHT - photochemistry - WORK - electrochemistry - COOLING of surroundings THERMOCHEMISTRY (Ch. 6) 2 Energy and Chemistry ENERGY is the capacity to do work or transfer heat. HEAT is the form of energy that flows between 2 samples because of a difference in temperature. WORK is the form of energy that results in a macroscopic displacement of matter such as gas expansion or motion of an object (force x distance) Other forms of energy — • Chemical • light • gravitational potential • electrical • electrostatic potential • kinetic 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 3 Specific Heat Capacity Thermochemistry is the science of heat (energy) flow. A difference in temperature leads to energy transfer. The heat “lost” or “gained” is related to a) sample mass b) change in T, and c) specific heat capacity by Specific heat capacity = heat lost or gained by substance (J) (mass, g) (T change, K) 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 4 Specific Heat Capacity Substance H2O Al glass Spec. Heat (J/g•K) 4.184 0.902 0.84 Water Aluminum 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 5 Specific Heat Capacity - an example If 25.0 g of Al cool from 310 oC to 37 oC, how many joules of heat energy are lost by the Al? Specific heat capacity = = 0.902 J/g.K heat lost or gained by substance (J) (mass, g)(T change, K) heat gain/lost = q = (specific heat)(mass)(DT) where DT = Tfinal - Tinitial = 37 - 310 = -273 K q = (0.902 J/g•K)(25.0 g)(-273 K) q = -6160 J negative sign of q heat is “lost by” or transferred from Al 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 6 Heat Transfer and Changes of State Changes of state involve energy Ice Water 333 J/g (Heat of Fusion) Water Vapor 2260 J/g (Heat of vaporization) 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 7 Heating/Cooling Curve for Water 3 Evaporate water 4 Heat water 1 2 Melt ice 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 8 CHEMICAL REACTIVITY • What drives chemical reactions? How do they occur? The first is answered by THERMODYNAMICS and the second by KINETICS. • In Ch. 4 we saw a number of “driving forces” for reactions that are PRODUCT-FAVORED. • formation of a precipitate • gas formation • H2O formation (acid-base reaction) 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 9 CHEMICAL REACTIVITY • Energy transfer also allows us to predict reactivity. • In general, reactions that transfer energy to their surroundings are “product-favored”. • How do we describe heat transfer in chemical processes ? 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 10 Heat Energy Transfer in Physical & Chemical Processes • CO2 (s, -78 oC) ---> CO2 (g, -78 oC) Heat flows into the SYSTEM (solid CO2) from the SURROUNDINGS in an ENDOTHERMIC process. Surroundings System heat 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 11 • ENERGY is the capacity to do work or transfer heat. • HEAT is the form of energy that flows between 2 samples because of a difference in temperature. • WORK is the form of energy that results in a macroscopic displacement of matter such as gas expansion or motion of an object (force x distance) In CO2 sublimation & expansion, the same amount of ENERGY flows from surroundings to system If expanding gas is enclosed, part of the energy transfer appears in the form of WORK OF EXPANSION wexp = - PDV (for an ideal gas) If expanding gas is not enclosed, the energy transfer appears only as HEAT (CO2 gas gets warm). 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 12 FIRST LAW OF THERMODYNAMICS heat energy transferred q = DE - w Energy change OR work done by the system DE = q + w NB - q and w positive when they are transferred FROM surroundings TO system Surroundings Heat Energy is conserved! 22 September, 1997 Chem 1A03E/1E03E System qsys > 0 THERMOCHEMISTRY (Ch. 6) Work wsys > 0 13 ENTHALPY Most chemical reactions occur at constant P, so Heat transferred at constant P is called qp with qp = DH = DE - w = DE + P DV = D(E+PV) where H H is defined as (E + PV) = enthalpy DH = heat transferred at constant P DH = change in heat content of the system DH = Hfinal - Hinitial 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 14 ENTHALPY DH = Hfinal - Hinitial If Hfinal > Hinitial then DH is positive Process is ENDOTHERMIC If Hfinal < Hinitial then DH is negative Process is EXOTHERMIC 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 15 Endo- and Exothermic Surroundings Surroundings System Heat qsys < 0 Heat qsys > 0 ENDOTHERMIC 22 September, 1997 Chem 1A03E/1E03E System EXOTHERMIC THERMOCHEMISTRY (Ch. 6) 16 USING ENTHALPY Consider the combustion of H2 to form water . . H2(g) + 1/2 O2(g) ---> H2O(g) + 242 kJ Exothermic reaction — heat is a “product”. DH = -242 kJ. This is spontaneous and proceeds readily once initiated. But the reverse reaction, the decomposition of water : H2O(g) + 242 kJ ---> H2(g) + 1/2 O2(g) Endothermic reaction — heat is a “reactant”, DH = +242 kJ. This does not occur spontaneously. BUT . . . Decomposition of water can be made to occur by coupling to another, spontaneous process . . . 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 17 LIGHT How can we make H2 gas ? w ire H2 O2 H2 O S e m ic o n d u c t o r 22 September, 1997 Me t a l Chem 1A03E/1E03E N. Lewis, American Scientist, Nov. 1995, page 534. THERMOCHEMISTRY (Ch. 6) 18 Making H2 from liquid H2O involves two steps. H2O(liq) + 44 kJ H2O(g) H2O(g) + 242 kJ H2(g) + 1/2 O2(g) --------------------------------------------------H2O(liq) + 286 kJ H2(g) + 1/2 O2(g) This is an example of HESS’S LAW — If a reaction is the sum of 2 or more others, the net DH is the sum of the DH’s of the other rxns. 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 19 Hess’s Law - a second example : Calc. DHrxn for S(s) + 3/2 O2(g) --> SO3(g) knowing that S(s) + O2(g) --> SO2(g) DH1 = -320.5 kJ SO2(g) + 1/2 O2(g) --> SO3(g) DH2 = -75.2 kJ S(s) + 3/2 O2(g) --> SO3(g) DH3 = -395.7 kJ The two rxns. add to give the desired rxn., so DHrxn = DH1 + DH2 = -395.7 kJ 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 20 energy S solid direct path + 3/2 O 2 DH3 = -395.7 kJ SO3 gas +O2 DH1 = -320.5 kJ SO2 gas + 1/2 O 2 DH2 = -75.2 kJ DH3 = -395.7 DH(2+3) = -320.5 + -75.2 = -395.7 S DH along one path = S DH along another path 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 21 SDH along one path = SDH along another path • This equation is valid because DH is a STATE FUNCTION • These depend only on the state of the system and not how it got there. • Other state functions include: V, T, P, energy . . — and your bank account! • Unlike V, T, and P, one cannot measure absolute H. Can only measure DH. 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 22 Standard Enthalpy Values Most DH values are labeled DHo o • • • • means measured under standard conditions P = 1 atmosphere ( = 760 torr = 101.3 kPa) Concentration = 1 mol/L T = usually 25 oC with all species in standard states e.g., C = graphite and O2 = gas 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 23 DHof = standard molar enthalpy of formation - the enthalpy change when 1 mol of compound is formed from elements under standard conditions. Values: Kotz, Table 6.2 and Appendix K By definition, DHof = 0 for elements in their standard states. H2(g) + 1/2 O2(g) --> H2O(g) DHof = -241.8 kJ/mol 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 24 Using Standard Enthalpy Values Calculate DH of reaction? In general, when ALL enthalpies of formation are known, DHorxn = S DHof (products) - SDHof (reactants) 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 25 Example: Calculate the heat of combustion of ethanol, i.e., DHorxn for C2H5OH(g) + 7/2 O2(g) 2 CO2(g) + 3 H2O(g) DHorxn = S DHof (prod) - S DHof (react) DHorxn = { 2 DHof (CO2) + 3 DHof (H2O) } - {7/2 DHof (O2) + DHof (C2H5OH)} = { 2 (-393.5 kJ) + 3 (-241.8 kJ) } - {7/2 (0 kJ) + (-235.1 kJ)} DHorxn = -1035.5 kJ per mol of ethanol 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 26 Bond Energies (Kotz, sect. 9.4, pp 418-422) • Given by D - the bond dissociation energy D = energy required to break a bond in a gas phase molecule under standard conditions • D can be derived from DHrxn for atomization . . . H e.g. CH4 (g) C (g) + 4 H (g) DHrxn = -1664 kJ = 4 * D(C-H) H D(C-H) = 416 kJ per mole of C-H bonds H H • D (C-H) (kJ/mol) varies slightly among compounds : CH4 416 C2H6 392 C3H8 380 C2H4 432 C2H2 445 C6H6 448 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 27 Bond Energies • D is similar for same bond in different molecules • Average values over many compounds are tabulated • Bond energy depends on bond order BOND D (kJ/mol) (Bond Energy) H—H 436 C—C 347 C=C 611 CC 837 N—N 159 NN 946 see table 9.5 for Dissociation Energies of other bonds. The GREATER the number of bonds (bond order) the HIGHER the bond dissociation energy 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 28 Using Bond Energies • Estimate the energy of the reaction H—H + Cl—Cl ----> 2 H—Cl Net energy = DHrxn = energy required to break bonds - energy evolved when bonds are made 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 29 Estimating DHrxn for H—H + Cl—Cl 2 H—Cl H—H = 436 kJ/mol Cl—Cl = 243 kJ/mol H—Cl = 431 kJ/mol • Sum of H-H + Cl-Cl bond energies = 436 kJ + 243 kJ = +679 kJ • 2 mol H-Cl bond energies = 862 kJ • Net = DH = +679 kJ - 862 kJ = -183 kJ THEREFORE, 22 September, 1997 DHf for H-Cl is Chem 1A03E/1E03E ??? THERMOCHEMISTRY (Ch. 6) 30 EXAMPLE 2: Estimate the energy of the reaction 2 H—O—O—H ----> O=O + 2 H—O—H • Is the reaction exo- or endothermic? • Which is larger: energy req’d to break bonds . . . or energy evolved on making bonds? Energy for bond breaking: 4 mol O—H bonds = 4 (464 kJ) 2 mol O—O bonds = 2 (138 kJ) TOTAL = 2132 kJ 22 September, 1997 Chem 1A03E/1E03E Energy from bond making : 1 mol O=O bonds = 498 kJ 4 mol O—H bonds = 4 (464 kJ) TOTAL = 2354 kJ THERMOCHEMISTRY (Ch. 6) 31 2 H—O—O—H ----> O=O + 2 H—O—H Net energy = +2132 kJ - 2354 kJ = - 222 kJ The reaction is exothermic! More energy is evolved on making bonds than is expended in breaking bonds. 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 32 Enthalpies of Reaction from Bond Energies ENDOTHERMIC EXOTHERMIC Gaseous Atoms Gaseous Atoms REACTANTS PRODUCTS PRODUCTS REACTANTS Bond Breaking costs more Bond Making releases more E than is gained by Bond Making than required for Bond Breaking 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 33 Key Concepts from Chapter 6: Thermochemistry • heat transfer - specific heat • phase transitions - heats of fusion, vaporization, etc • First law of thermodynamics DE = q - w • endothermic versus exothermic reactions • enthalpy change in chemical reactions • Hess’s law • standard molar enthalpies of formation DHrxn = S DHf(products) - S DHf (reactants) • bond energies DHrxn = S D(bonds broken) - S D(bonds made) 22 September, 1997 Chem 1A03E/1E03E THERMOCHEMISTRY (Ch. 6) 34