An Instructor’s Solutions Manual to Accompany FUNDAMENTALS OF CHEMICAL ENGINEERING THERMODYNAMICS KEVIN D. DAHM AND DONALD P. VISCO, JR. © 2015 Cengage Learning ISBN-13: 978-1-133-59845-9 ISBN-10: 1-133-59845-5 ALL RIGHTS RESERVED. 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This Agreement will be Supplement may be provided to your students IN PRINT FORM governed by and construed pursuant to the laws of the State of ONLY in connection with your instruction of the Course, so long New York, without regard to such State’s conflict of law rules. as such students are advised that they may not copy or distribute any portion of the Supplement to any third party. Test Thank you for your assistance in helping to safeguard the integrity banks and other testing materials may be made available in the of the content contained in this Supplement. We trust you find the classroom and collected at the end of each class session, or Supplement a useful teaching tool. Printed in the United States of America 1 2 3 4 5 6 7 16 15 14 13 I ' S NSTRUCTOR S OLUTIONS M ANUAL A TO CCOMPANY FUNDAMENTALS OF CHEMICAL ENGINEERING THERMODYNAMICS FIRST EDITION KEVIN D. DAHM AND DONALD P. VISCO, JR. CONTENTS Chapter Page 1. Introduction ……………………………………………………………... 1 2. The Physical Properties of Pure Compounds …………………………… 19 3. Material and Energy Balances ………………………………………….. 55 4. Entropy ……………………………………………………………… …. 119 5. Thermodynamic Processes and Cycles …………………………………. 185 6. Thermodynamic Models of Real, Pure Compounds ……………………. 253 7. Equations of State ………………………………………………………. 321 8. Modeling Phase Equilibrium for Pure Compounds ………………………395 9. An Introduction to Mixtures ……………………………………………. 437 10. Vapor-Liquid Equilibrium ……………………………………………… 475 11. Theories and Models for ………………………………………………… 509 Vapor–Liquid Equilibrium of Mixtures: Modified Raoult’s Law Approaches 12. Theories and Models for ………………………………………………… 561 Vapor–Liquid Equilibrium of Mixtures: Using Equations of State 13. Liquid-Liquid, Vapor-Liquid-Liquid, …………………………………… 623 and Solid-Liquid Equilibrium 14. Fundamentals of Chemical Reaction Equilibrium ………………………. 651 15. Synthesis of Thermodynamic Principles ………………………………… 689 Chapter 1: Introduction 1-16) The value g = 9.81 m/s2 is specific to the force of gravity on the surface of the earth. The universal formula for the force of gravitational attraction is: (cid:5)(cid:6)(cid:5)(cid:7) (cid:1) = G (cid:7) Where m and m are the masses of the two(cid:8) objects, r is the distance between the 1 2 centers of the two objects, and G is the universal gravitation constant, G = 6.674 × 10-11 N(m/kg)2. A) Research the diameters and masses of the Earth and Jupiter. B) Demonstrate that F = m(9.81 m/s2) is a valid relationship on the surface of the earth. C) Determine the force of gravity acting on a 1000 kg satellite that is 2000 miles above the surface of the Earth. D) One of the authors of this book has a mass of 200 lb . If he was on the surface m of Jupiter, what gravitational force in lb would be acting on him? f Solution: A) Measurements obtained from different sources will vary slightly. D ~ 12,742 km D ~ 142,000 km Earth Jupiter Mass = 5.97 × 1024kg Mass = 1.90 × 1027kg earth jupiter B) Mass = 5.97 × 1024kg Radius = 6.371 × 106 meters earth Earth (cid:1) /0 1 (cid:9)(cid:10)(cid:9)(cid:11) (cid:28)(cid:6)(cid:6)(cid:29)(cid:30)(cid:11) "#.$%×(cid:6)&(cid:11)'(cid:31) ( (cid:20)234(cid:11)! (cid:1) = G (cid:12)(cid:11) (cid:1) = m(cid:14)(cid:15)(cid:16)(cid:17)(cid:18)(cid:19)(cid:20)6.674 × 10 (cid:31) (cid:11) !(*.+%×(cid:6)&, (cid:30))(cid:11).((cid:6) (cid:29))5 (cid:1) 7 6 = 7(8.9:;<=>) C) 2000 miles = 3218.68 km = 3218680 m (cid:11) (cid:11)' (cid:28)(cid:6)(cid:6)(cid:29)(cid:30) (#.$%×(cid:6)& AB) (cid:1) = 1000kg(cid:20)6.674 × 10 (cid:31) (cid:11) !(*+%(cid:6)&&&(cid:9)C+(cid:7)(cid:6)D*D&(cid:9) )(cid:11) = EFE9 G 1 © 2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part. Chapter 1: Introduction D) Radius = 66854000 m Mass = 1.898 × 1027 kg 200lb = 90.7 kg Jupiter Jupiter m kg m (cid:7) (cid:7)% K (cid:7)O (cid:28)(cid:6)(cid:6)Nm (1.90×10 kg) sec (cid:1) = 90.7 kg.6.674 × 10 (cid:7) 5 % (cid:7)J P = >>9: G kg (7.10×10 m) (1 N) 1-17) A gas at T=300 K and P=1 bar is contained in a rigid, rectangular vessel that is 2 meters long, 1 meter wide and 1 meter deep. How much force does the gas exert on the walls of the container? Solution: 1 Bar = 100,000 Pa AreaTUVWX(cid:18)(cid:17) = (2×W×H)+(2×W×L)+(2×H×L) Force = Pressure × Area N (cid:20) (cid:7)! m Force = (100000Pa)(2×1m×1m+2×1m×2m+2×1m×2m)b c Pa e Force = :×:d G 1-18) A car weighs 3000 lb , and is travelling 60 mph when it has to make an emergency m stop. The car comes to a stop 5 seconds after the brakes are applied. A) Assuming the rate of deceleration is constant, what force is required? B) Assuming the rate of deceleration is constant, how much distance is covered before the car comes to a stop? Solution: A) (cid:6)lV #(cid:7)D&W(cid:19) W(cid:19) Force = mass×acceleration 60mph(cid:20)+*&&m(cid:17)(cid:18)!(cid:20)(cid:6)(cid:30)no(cid:17)! = 88m(cid:17)(cid:18) velocityWnsXo −velocitynsn(cid:19)nXo Acceleration = time ft 88 −0 sec a = 5 sec ft a = 17.6 (cid:7) sec 2 © 2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part. Chapter 1: Introduction ft Force = 17.6 (cid:7) ×3000lb(cid:30) sec z{7|} F orce = y>ydd > ;<= B) (cid:11) X(cid:18)(cid:18)(cid:17)o(cid:17)VX(cid:19)n(cid:14)s∗(cid:19)n(cid:30)(cid:17) PositionWnsXo = (cid:7) +velocitynsn(cid:19)Xo ×time+positionns(cid:19)nXo (cid:127)€ (cid:11) (cid:20)(cid:28)(cid:6)%.*234(cid:11)!(#m(cid:17)(cid:18)) W(cid:19) PositionWnsXo = (cid:7) +(cid:20)88m(cid:17)(cid:18) !(5sec)+0 PositionWnsXo = >>d |} 1-19) Solar panels are installed on a rectangular flat roof. The roof is 15 feet by 30 feet, and the mass of the panels and framing is 900 lb . m A) Assuming the weight of the panels is evenly distributed over the roof, how much pressure does the solar panel array place on the roof? B) The density of fallen snow varies; here assume its ~30% of the density of liquid water. Estimate the total pressure on the roof if 4 inches of snow fall on top of the solar panels. Solution: A) (cid:129)(cid:14)V(cid:18)(cid:17) Pressure = ‚V(cid:17)X Area = Length×Width Force = Mass×Acceleration ft (900lb(cid:30))(cid:20)32.2 (cid:7)! 1lbW sec Pressure = b c (15ft)(30ft) lb(cid:30)ft 32.2 (cid:7) sec z{| P ressure = > > |} B) o(cid:15)1 o(cid:15)1 Densityms(cid:14)† = (30%)63.3 W(cid:19)ˆ = 19.0 W(cid:19)ˆ Forcems(cid:14)† = Volumems(cid:14)† ×Densityms(cid:14)† ×gravity Forcems(cid:14)† +ForceŠXs(cid:17)om Pressure = Area 4inches = 0.333ft 3 © 2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part. Chapter 1: Introduction Pressure ft lb(cid:30) ft .(900lb(cid:30))(cid:20)32.2 (cid:7)!5+"(15ft)(30ft)(0.333ft)((cid:20)19.0 +!(cid:20)32.2 (cid:7)! sec ft sec 1lbW = b c (15ft)(30ft) lb(cid:30)ft 32.2 (cid:7) sec z{| P ressure = 9.FF > |} 1-20) A box has a mass of 20 kg, and a building has a height of 15 meters. A) Find the force of gravity acting on the box. B) Find the work required to lift the box from the ground to the roof of the building. C) Find the potential energy of the box when it is on the roof of the building. D) If the box is dropped off the roof of the building, find the kinetic energy and velocity of the box when it hits the ground. Solution: A) (cid:30) Force = (20kg)(cid:20)9.81m(cid:17)(cid:18)(cid:11)! = :8e.> G B) Work = Force×Distance Work = (196.2N)(15m) = >8EFG7 = >8EF ‹ C) Potential Energy = Mass×Height×Gravity m Potential Energy = (20kg)(15m)(cid:20)9.81 (cid:7)! = >8EFG7 = >8EF ‹ sec D) We know that Energy is conserved, so if the box is dropped from a height of 15 meters, its Kinetic Energy at Height = 0 meters will be the same as its potential energy at Height = 15 meters. Kinetic Energy = >8EFG7 To find the object’s velocity as it hits the ground: (cid:6) (cid:7) K inetic Energy = (cid:20)(cid:7)!Mass×Velocity (cid:6) (cid:7) 2943Nm = (cid:20)(cid:7)!(20kg)×V kg m (cid:7) (cid:7) Nm sec m (cid:7) K294.3 Ob c = 294.3. (cid:7)5 = V kg 1N sec 4 © 2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part. Chapter 1: Introduction 7 V = :Ž.:e ;<= 1-21) 100 kg of steam is enclosed in a piston-cylinder device, initially at 300°C and 5 bar. It expands and cools to 200°C and 1 bar. A) What is the change in internal energy of the steam in this process? B) If the external pressure is constant at 1 bar, how much work was done by the steam on the surroundings? C) Research and briefly describe at least two examples of machines, either historical or currently in use, that harness the energy in steam and convert it into work. Any form of work is acceptable; you needn’t confine your research to expansion work (which was examined in parts A and B). Initial State Final State T = 300°C T = 200°C 1 2 P = 5 bar P = 1 bar 1 2 Solution: Define the gas as the system. A) From steam tables: kJ (cid:143)(cid:144)(cid:6) = 2803.2 kg kJ (cid:143)(cid:144)(cid:7) = 2658.2 kg So (cid:31)– Δ(cid:143) = “"(cid:143)(cid:144)(cid:7) −(cid:143)(cid:144)(cid:6)( = (100 ”•)(cid:20)2658.2−2803.2 (cid:31) ! = −:E,ydd ˜‹ 5 © 2015 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.