fa khara ny Fall 2012/2013. Level: 3 Semester: 5 Code: 230 Title: Thermodynamics 1 PHAROS UNIVERSITY FACULTY OF ENGINEERING MECHANICAL ENGINEERING Dept. Date: 24/11/2012 9th week Exam Duration: 1 Hour Steam Tables and Charts are allowed to be used. Illustrate your answer with neat sketches, whenever it is possible. 1. A rigid tank contains 10 kg of air at 150 kPa and 20oC. More air is added to the tank until the pressure and temperature rise to 250 kPa and 30oC, respectively. Show this filling process on p-V diagram and determine the amount of air added to the tank. (Take for air cp = 1.005 kJ/kg-K, cv = 0.718 kJ/kg-K) m2-m1 m1 = 10 kg p1 = 150 kPa T1 = 20 oC p2 = 250 kPa T2 = 30 oC 2. A piston-cylinder device contains 0.8 kg of steam at 300oC and 1 MPa. Steam is cooled at constant pressure until one-half of the mass condenses. Show the process on p-v and T-s phase diagrams, and then determine: (a) (b) (c) The final temperature of the steam. The volume change through the cooling process. The amount of heat rejected through this process Q 3. A piston-cylinder device, initially, contains 0.5 m3 of nitrogen gas at 400 kPa and 27°C. An electric heater within the device is turned on and is allowed to pass a current of 2A for 5 min from a 120-V source. Nitrogen expands at constant pressure, and a heat loss of 2800 J occurs during the process. Represent this process on p-v and T-s diagrams and determine: 2800 J 2A 120 V a) Mass of gas inside the cylinder. b) The added heat by electric heater. c) The final temperature. ( Take for nitrogen gas: Cp = 1.039 kJ/kg.K, Cv = 0.743 kJ/kg.K) Exam Committee : 1. Prof Dr M. G. Wasel 2. Page 1 of 4 fa khara ny Problem 1 Given: V1=V2, m1=10 kg, p1=150 kPa, T1=293 K, p2=250 kPa, T2=303 K, Cp=1.005 kJ/kg.K, Cv=0.718 kJ/kg.K p Required: βm = m2 – m1 p2 Solution: π = πΆπ − πΆπ£ = 1.005 − 0.718 = 0.287 Since ππ½ ππ πΎ π1 π1 = π1 π π1 Then p1 π1 π π1 10 × 0.287 × 293 = = 5.61 π3 π1 150 Since V2=V1 π1 = v 1= v 2 Then, applying equation of state at the end of filling process yields to: π2 = π2 π2 250 × 5.61 = = 16.12 ππ π π2 0.287 × 303 Mass of added air βm = m2 - m1 = 16.12 - 10 = 6.12 kg Page 2 of 4 v fa khara ny Problem 2 p Given: m=0.8 kg, T1=300°C, p1=10 bar, p2=p1=10 bar, mf,2=0.5 kg, mtotal, x2=0.5 T1 =300oC Required: p-V and T-s diagrams, T2, βV=V2-V1 from tables (B): 0. and 1 2 = bar, T2 =180oC x Solution: At p1=10 10 bar 5 Ts@p=10bar=179.9°C v Since T1 > Ts , then the steam at condition 1 is superheated steam. From table (C) at p1=10 bar and T1=300°C: 3 condition dryness fraction = 1 300oC v1=0.258 m /kg. Considering T 2, ππ by definition of 180oC 10 bar 2 , the steam at condition 2 is wet steam and its dryness fraction x2=0.5. 0.5 From Tables (B) at p2=10 bar: x= ππ +ππ and T2=Ts=179.9°C and vf=0.0011 m3/kg s 3 vg=0.1943 m /kg Accordingly; π£2 = (1 − π₯2 )π£π + π₯2 π£π = 0.5(0.0011) + 0.5(0.1943) = 0.0977π3 /ππ The change of volume through this cooling process: βπ = π2 − π1 = π(π£2 − π£1 ) = 0.8(0.0977 − 0.258) = −0.128π3 Problem 3 Page 3 of 4 fa khara ny Given: V1 = 0.5 m3, p1 = p2 = 400 kPa, T1 = 27°C, I = 2 A, Volt = 120 V, t = 5 min., Qlost = 2800 J =2.8 kJ, Required: a) mgas b) Qelectric πΆπ = 1.039 ππ½ ππ.πΎ , πΆπ£ = 0.743 ππ½ ππ.πΎ c) T2 Solution: (a) π = πΆπ − πΆπ£ = 1.039 − 0.743 = 0.296 2800 J 2A ππ½ ππ. πΎ 120 V π1 π1 = π π π1 π= π1 π1 π π1 = 400×0.5 0.296×(273+27) = 2.252 ππ (b) ππππππ‘πππ = π × πΌ × π‘ = 2 × 120 × (5 × 60) = 72000 π½ = 72 ππ½ p 400 kPa 1 2 (c) v π12 − π12 = π2 − π1 π12 = ππππππ‘πππ − ππππ π‘ = 72 − 2.8 = 69.2 ππ½ 2 π12 = ∫ π ππ = π(π2 − π1 ) T 2 1 π12 = π12 + (π2 − π1 ) = π»2 − π»1 = π πΆπ (π2 − π1 ) 1 69.2 = 2.252 × 1.039 × (π2 − 300) s π2 = 329.6 πΎ = 56.6 °πΆ Page 4 of 4