Chapter 2 Homework Solutions

Similar documents
University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2011

CHEM 5200 FALL Chem 5200: navigate ( Faculty Schwartz Classes)

Homework Problem Set 8 Solutions

Chpt 19: Chemical. Thermodynamics. Thermodynamics

UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING TERM TEST 2 17 MARCH First Year APS 104S

CHEM Exam 3 November 2, Version A. Constants: NA = 6.02x10 23 mol -1 R = L atm/mol K R = 8.31 J/mol K

Chemistry 123: Physical and Organic Chemistry Topic 2: Thermochemistry

Ch 10 Practice Problems

The Factors that Determine the Equilibrium State

Adiabatic Expansion/Compression

CHEM 305 Solutions for assignment #4

Thermodynamics (XI) Assignment(Solution)

Chapter 3 Homework Solutions

= 1906J/0.872deg = 2186J/deg

B 2 Fe(s) O 2(g) Fe 2 O 3 (s) H f = -824 kj mol 1 Iron reacts with oxygen to produce iron(iii) oxide as represented above. A 75.

the drink won t rise very high in the straw vacuum straw 1 atm drink

End of Year Review ANSWERS 1. Example of an appropriate and complete solution H = 70.0 g 4.19 J/g C T = 29.8 C 22.4 C 7.4 C

Useful Information to be provided on the exam: 1 atm = 760 mm Hg = 760 torr = lb/in 2 = 101,325 Pa = kpa. q = m C T. w = -P V.

Gases: Their Properties & Behavior. Chapter 09 Slide 1

THE SECOND LAW Chapter 3 Outline. HW: Questions are below. Solutions are in separate file on the course web site. Sect. Title and Comments Required?

10th edition 9th edition 8th edition

What is thermodynamics? and what can it do for us?

Free-energy change ( G) and entropy change ( S)

0 o C. H vap. H evap

First Law CML 100, IIT Delhi SS. The total energy of the system. Contribution from translation + rotation + vibrations.

Chapter 16. Thermodynamics. Thermochemistry Review. Calculating H o rxn. Predicting sign for H o rxn. Creative Commons License

Entropy Changes & Processes

Le Châtelier's Principle. Chemical Equilibria & the Application of Le Châtelier s Principle to General Equilibria. Using Le Châtelier's Principle

Chapter 19 Chemical Thermodynamics

BCIT Fall Chem Exam #2

BCIT Fall Chem Exam #2

p A = X A p A [B] = k p B p A = X Bp A T b = K b m B T f = K f m B = [B]RT G rxn = G rxn + RT ln Q ln K = - G rxn/rt K p = K C (RT) n

CHEM Exam 2 - March 3, 2017

CHEM Exam 2 - October 11, INFORMATION PAGE (Use for reference and for scratch paper)

N h (6.02x10 )(6.63x10 )

Ch 9 Practice Problems

UNIT # 06 THERMODYNAMICS EXERCISE # 1. T i. 1. m Zn

B 2, C 2, N 2. O 2, F 2, Ne 2. Energy order of the p 2p and s 2p orbitals changes across the period.

CHEM Thermodynamics. Entropy, S

Entropy Changes & Processes

NCERT THERMODYNAMICS SOLUTION

Chapter 6 Review. Part 1: Change in Internal Energy

5.2 Energy. N Goalby chemrevise.org Lattice Enthalpy. Definitions of enthalpy changes

Homework 12 (Key) First, separate into oxidation and reduction half reactions

Chemistry 1A, Spring 2008 Midterm Exam III, Version A April 14, 2008 (90 min, closed book)

Chapter 19 Chemical Thermodynamics

HOMEWORK 11-1 (pp )

Reduction: 2 H + (aq) + 2 e H2(g)

Questions 1-3 relate to the following reaction: 1. The rate law for decomposition of N2O5(g) in the reaction above. B. is rate = k[n2o5] 2

Exam 2 Solutions. for a gas obeying the equation of state. Z = PV m RT = 1 + BP + CP 2,

HEAT, WORK, AND THE FIRST LAW OF THERMODYNAMICS

Date: Hybrid Chemistry Regents Prep Ms. Hart/Mr. Kuhnau. UNIT 9: Solutions and Gases Lesson 9.2: Redox Reactions

Chapter Elements That Exist as Gases at 25 C, 1 atm. 5.2 Pressure basic physics. Gas Properties

Chapter Eighteen. Thermodynamics

CO(g) + O2(g) CO2(g) 2 mol 1 mol 2 mol 44.8 L 22.4 L 44.8 L 1.204(10) 24 molecules 6.02(10) 23 molecules 1.204(10) 24 molecules g 32.0 g 88.

1) (14.8) How does the entropy of a system change for each of the following processes?

Disorder and Entropy. Disorder and Entropy

Thermochemistry Lecture

Chemical Thermodynamics

CHAPTER 12 GASES AND KINETIC-MOLECULAR THEORY

General Chemistry 1 CHM201 Unit 3 Practice Test

Chemistry 400: General Chemistry Miller Exam II November 4, 2015 Approximately 150 points

Chemistry 163B. Thermochemistry. Chapter 4 Engel & Reid

Lecture 2. Review of Basic Concepts

Heat and Thermodynamics. February. 2, Solution of Recitation 2. Consider the first case when air is allowed to expand isothermally.

H = DATA THAT YOU MAY USE. Units Conventional Volume ml or cm 3 = cm 3 or 10-3 dm 3 Liter (L) = dm 3 Pressure atm = 760 torr = 1.

1. What is the value of the quantity PV for one mole of an ideal gas at 25.0 C and one atm?

Kinetic energy is the energy of motion (of particles). Potential energy involves stored energy (energy locked up in chemical bonds)

The Second Law of Thermodynamics (Chapter 4)

McCord CH301 Exam 5 Dec 5, 2017

Ideal Gas Law Stoichiometry

Chemistry 400: General Chemistry Miller Fall 2015 Final Exam Part Deux December 14, 2015 Approximately 150 points

CHAPTER 11 Stoichiometry Defining Stoichiometry

Saturday Study Session 1 3 rd Class Student Handout Thermochemistry

Thermodynamics Spontaneity. 150/151 Thermochemistry Review. Spontaneity. Ch. 16: Thermodynamics 12/14/2017

THE ZEROTH AND FISRT LAW OF THERMODYNAMICS. Saeda Al-Mhyawi secend Tearm 1435H

A Gas Uniformly fills any container. Easily compressed. Mixes completely with any other gas. Exerts pressure on its surroundings.

Chemistry 1105 R11 Fall 2018 Test 3

1.8 Thermodynamics. N Goalby chemrevise.org. Definitions of enthalpy changes

PUT A SQUARE BOX AROUND ALL ANSWERS

Energy, Enthalpy and Thermochemistry. Energy: The capacity to do work or to produce heat

Chapter 19: The Kinetic Theory of Gases Questions and Example Problems

Physical Chemistry I CHEM 4641 Final Exam 13 questions, 30 points

(for tutoring, homework help, or help with online classes) 1.

Thermodynamics: Entropy, Free Energy, and Equilibrium

Molar Specific Heat of Ideal Gases

12A Entropy. Entropy change ( S) N Goalby chemrevise.org 1. System and Surroundings

FORMULA SHEET (tear off)

Chem 152 Final. You will have 1 hour and 50 minutes. Do not begin the exam until you are instructed to start. Best of luck.

Chemistry 5350 Advanced Physical Chemistry Fall Semester 2013

Pressure Volume Work 2

ENTROPY HEAT HEAT FLOW. Enthalpy 3/24/16. Chemical Thermodynamics. Thermodynamics vs. Kinetics

Quiz B3: Le Chatelier s Principle Block:

Page 1 of 11. Website: Mobile:

Thermodynamics of an Ideal Gas

THERMODYNAMICS I. TERMS AND DEFINITIONS A. Review of Definitions 1. Thermodynamics = Study of the exchange of heat, energy and work between a system

Practice Midterm 1 CHEMISTRY 120 GENERAL CHEMISTRY. Examiners: Prof. B. Siwick Prof. A. Mittermaier Prof. A. Fenster

Thermochemistry HW. PSI Chemistry

CHEM 1423 Chapter 17 Homework Questions TEXTBOOK HOMEWORK

Experiment 2 Heat of Combustion: Magnesium

Transcription:

. Cl - 3 translations + rotations + vibration Chapter Homework Solutions (a) Um(rigid) = (3/)R + (/)R = (5/)R Hm(rigid) = (7/)R Cpm(rigid) = (7/)R = 9. J/mol-K (b) Um(vib) = (3/)R + (/)R + R = (7/)R Hm(vib) = (9/)R Cpm(vib) = (9/)R = 37.4 J/mol-K. C6H6 (N=) - 3 translations + 3 rotations + (3x-6) = 30 vibrations (a) Um(rigid) = (3/)R + (3/)R = 3R Hm(rigid) = 4R Cpm(rigid) = 4R = 33. J/mol-K (b) Um(vib) = (3/)R + (3/)R + 30R = 33R Hm(vib) = 34R Cpm(vib) = 34R = 8.5 J/mol-K.3 CO (N=3) - 3 translations + rotations + (3x3-5) = 4 vibrations (a) Um(rigid) = (3/)R + (/)R = (5/)R Hm(rigid) = (7/)R Cpm(rigid) = (7/)R = 9. J/mol-K (b) Um(vib) = (3/)R + (/)R + 4R = (3/)R Hm(vib) = (5/)R Cpm(vib) = (5/)R = 6.3 J/mol-K.4 =.4 L = 44.8 L = 73 K (constant) n =.00 mol (a) Reversible U = nc = H = nc = 0 m 0 pm w = nr ln( / ) = mol(8.3 J / mol K)(73 K)ln(44.8 /.4) = 570 J q = U - w = +570 J nr ( mol)(8.3 kpa L / mol K)(73 K) (b) Constant p (final pressure): p = = = 50.6 kpa 44.8 L U = H = 0 w = p( ) = 50.6 kpa(44.8 L.4 L) = 30kPa L = 30 J q = U - w = +30 J

(c) p = 0 U = H = 0 w= p ( ) = 0 q = U - w = 0.5 0.3kPa p =.00 atm = 0.3kPa atm = 300 K = 400 K p p 400 = p = p = 0.3kPa = 35.kPa 300 3 U = ncm = n R = (.0 mol)(.50)(8.3 J / mol K)(400 K 300 K) = 50 J =.5kJ w = 0 (because = constant) q = U-w = U =.5 kj.6 n =. mol = 00 o C = 373 K vaph = 40.7 kj/mol w = -P(liq - gas) +Pgas = nr = (.0 mol)(8.3 J/mol-K)(373 K) = +300 J = +3.0 kj q = H = n condh = n(- vaph) = ( mol)(-40.7 kj/mol) = -40.7 kj U = q + w = -40.7 kj + 3.0 kj = -37.6 kj.7 = 5 o C = 98 K p =.00 atm Reaction: Mg(s) + HCl(aq) MgCl(aq) + H(g) mol Mg mol H We will need n(h) below: n( H ) = 5 g Mg = 0.67 mol H 4.3 g Mg mol Mg { } { } { } w= p = p = p + p prod rct H MgCl Mg HCl H Simplificaion above because volumes of liquids/solids are negligible compared to volumes of gases. { } H H w = p = p = n R = (0.67 mol)(8.3 J / mol K)(98 K) = 530 J.5kJ.8 mol of W(s) requires mol W x 6 mol CO/ mol W = mol of CO(g). = 50 o C = 43 K w = -P - = +P = +P prod rct rct CO [Consider only gas phase reactants or products] w = -P = -n R = - mol(8.3j / mol K)(43K) = 400 J = +4. kj CO CO

.9 n = mol = 5 o C = 98 K = 00 o C = 473 K Cpm = a + b a = 0.7 J/mol-K b = 0.37 J/mol-K (a) Constant Pressure [q = H] q = H = nc pm d = n ( a + b ) d = na[ ] + nb ( K ) 473 (98 K) = ( mol)(0.7 J / mol K)(473 K 98 K) + ( mol(0.37 J / mol K ) = 3530 J + 4960 J = 8490 J 8.5kJ w = p = p + p = nr + nr = nr( ) = ( mol)(8.3 J / mol K)(473 K 98 K) = 450 J.5kJ U = q + w = 8490 J +(-450 J) =7040 J 7.0 kj (b) Constant olume [q = U and w = 0] For a Perfect Gas U and H depend only upon temperature. herefore the values of U and H are the same as in part (a): U = 7040 J 7.0 kj H = 8490 J 8.5 kj Because = constant w = 0 q = U = 7040 J 7.0 kj.0 Cm = Cpm - R = 37. - 8.3 = 8.8 J/mol-K. mol n =.45 g = 0.056mol 44 g = 7 o C = 300 K = 500 cm 3 = 0.50 L = 3.00 L Let's calculate for an adiabatic expansion. We'll need R/Cm = 8.3/8.8 = 0.89 = R C m R 0.89 C m 0.50 3.00 = = (300 K) = 79 K Adiabatic Expansion: q = 0 w = U w = U = ncm = (0.056 mol)(8.8 J / mol K)(79 K 300 K) = 95 J

. n = 3.0 mol = 60 K = 85 K Cpm = 9.4 J/mol-K Let's calculate Cm: Cm = Cpm - R = 9.4-8.3. J/mol-K Because p = constant q = H q = H = nc pm = (3.0 mol)(9.4 J / mol K)(85 K 60 K) = 05 J. kj U = ncm = (3.0 mol)(. J / mol K)(85 K 60 K) = 580 J.6 kj. n =.00 mol Cm = 0.8 J/mol-K = 30 K p = 3.5 atm p =.50 atm γ nr (.0 mol)(0.08 L atm / mol K)(30 K) = = = p 3.5atm C C + R 0.8 + 8.3.40 C C 0.8 pm m = = = = m m 7.8 L γ γ γ p γ 3.5 p = p.40.40 = = 7.8 = 3.06 = p.50 /.40 = (3.06) = 9.4L = p (.50)(9.4) = 87 ()(0.08) = K nr Adiabatic: q = 0 w = U = ncm [ ] = ( mol)(0.8 J / mol K)(87 K 30 K) = 480 J 0.5kJ.3 n = 0.50 mol = 50 K vaph o = 6.0 kj/mol p = const (phase transition). herefore q = H q = H = n H o = (0.50 mol)(6.0 kj / mol) = 3.0kJ vap w = p( ) p = nr = (0.50 mol)(8.3 J / mol K)(50 K) gas liq gas = 040 J.0kJ U = q + w = +3.0 -.0 =.0 kj

.4 C6H5CH5(l) + (/) O(g) 8 CO(g) + 5 HO(l) o o o o combh = 8 f H ( CO) + 5 f H ( HO) f H ( C6H5CH5) + (/ ) 0 = 8( 393.5) + 5( 85.8) (.5) = 4564.5 kj / mol [ ]. 5 For N(g) a =.35 L -atm/mol b = 0.039 L/mol n = mol = 98 K =.00 L = 4.8 L Internal Energy ( U) U π = = na U na U = d = = = d n a n a U = ( mol).35 L atm / mol.00 / 4.8 / L mol L mol 0J = 5.8 L atm = 53. J L atm Work (w) na p + ( nb) = nr nr p = nb n a = = nr n a = + w pd d nr d n a d nb nb ln ln nb nb [ ] w = nr b + n a = nr + n a 4.8 0.039 w = ( mol)(8.3 J / mol K)(98 K)ln (.35 / ).0 0.039 + mol L atm mol.0 4.8 L L 0J = 6 90 J / mol + (5.40 L atm / mol) = 690 J + 545 J L atm = 5 745 J 5.7 kj / mol Note: Observe that the work is less negative than it would be if there were no attractive forces (i.e. if a = 0). his is because some of the work energy released in the expansion must be used to pull the attractive molecules further from each other.

Heat (q) U = +53 J/mol w = -5745 J/mol q = U - w = +53 -(-5745) = +668 J/mol +6.3 kj/mol P (.0 atm)(.4 L).6 = 73 K nr = ( mol)(0.08 L atm / mol K) = P (.0 atm)(44.8 L) = 546 K nr = ( mol)(0.08 L atm / mol K) = P 3 3 (0.50 atm)(44.8 L) = 3 73 K nr = ( mol)(0.08 L atm / mol K) = Cm = (3 / ) R =.5(8.3 J / mol K) =.5 J / mol K C pm = Cm + R =.5 + 8.3 = 0.8 J / mol K Step (Constant Pressure) 0J w = p( ) = (.0 atm)(44.8l.4 L) =.4 L atm = 60 J L atm U = ncm = ( mol)(.5 J / mol K)(546 K 73 K) =+ 340 J q = H = nc pm = ( mol)(0.8 J / mol K)(546 K 73 K) =+ 5680 J Step 3 (Constant olume) w = 0 q = U = ncm ( 3 ) = ( mol)(.5 J / mol K)(73K 546 K) = 340 J H = nc pm 3 = ( mol)(0.8 J / mol K)(73K 546 K) = 5680 J Step 3 (Isothermal) otals: U = H = 0 w = nr3ln( / 3) = ( mol)(8.3 J / mol K)(73 K)ln(.4 / 44.8) =+ 570 J q = -w = -570 J Utot = U + U 3 + U3 = +340-340 +0 = 0 J Htot = H + H 3 + H3 = +5680-5680 +0 = 0 J wtot = w + w 3 + w3 = -60 + 0 +570 = -690 J qtot = q + q 3 + q3 = +5680-340 -570 = +700 J

Note: As expected Utot = Htot = 0 around the cycle. U and H are State Functions However qtot 0 and wtot 0 around the cycle. q and w are not State Functions o within roundoff error wtot + qtot 0 because qtot + wtot = Utot = 0.7 n =.0 mol Note: he initial temperature and pressure (required for the calculation) was not given in the problem. We ll use = 98 K p =.0 atm. nr ( mol)(0.08 L atm / mol K)(98 K) = = = p.0atm 4.4 L Cpm = (7/)R = (7/)(8.3) = 9. J/mol-K Cm = Cpm - R = 9. - 8.3 = 0.8 J/mol-K Step a: Constant volume heating to p = p = atm p = = = = (98) = 596 K p w = 0 q = U = ncm ( ) = ( mol)(0.8 J / mol K)(596 K 98 K) =+ 690 J H = nc pm = ( mol)(9. J / mol K)(596 K 98 K) =+ 8670 J Step b: Adiabatic Expansion from = 596 K back to 3 = 98 K q = 0 w = U = ncm ( 3 ) = ( mol)(0.8 J / mol K)(98 K 546 K) = 690 J H = nc pm 3 = ( mol)(9. J / mol K)(98 K 546 K) = 8670 J We ll need 3 for last step. 3 = 3 R C m 3 3 C m/ R 0.8/8.3 596 = = = 5.66 98 3 = 5.66 = 5.66(4.4) = 38.3 L

Step c: Isothermal Compression from 3 = 38.3 L to =.4 L otals: U = H = 0 w = nr ln( / 3) = ( mol)(8.3 J / mol K)ln(4.4 /38.3) =+ 4300 J q = -w = -4300 J Utot = +690-690 + 0 = 0 Htot = +8670-8670 + 0 = 0 wtot = 0-690 + 4300 = -890 J 0 qtot = +690 + 0-690 = +890 J 0