Chemistry 420/523 Chemical Thermodynamics (Spring ) Examination 1

Size: px
Start display at page:

Download "Chemistry 420/523 Chemical Thermodynamics (Spring ) Examination 1"

Transcription

1 Chemistry 420/523 Chemical hermodynamics (Sring ) Examination 1 1 Boyle temerature is defined as the temerature at which the comression factor Z m /(R ) of a gas is exactly equal to 1 For a gas obeying the equation of state P m R " µ # 2 c c show that the Boyle temerature deends only on the critical temerature From the equation of state, we have Z P m R " µ # 2 c c he right hand side is equal to unity when 0, 0, or when 14( c / ) 2 Since the first two conditions are unhysical, we get B 2 c herefore, the Boyle temerature deends only on the critical temerature 2 Using the relationshi H U +, and obtaining transformation relationshis by considering H as a function of any two of the variables (,, ), show that µ µ µ µ H U H + From H U +, differentiating with resect to temerature holding the volume constant (to get the first term in the exression) we get µ µ µ H U + (1) Considering enthaly as a function of temerature and ressure, H(,), we write µ µ H H dh d + d (2) Differentiating Eq (2) with resect to at constant, weget µ µ µ µ H H H + (3) From Eq (3), µ µ µ µ H H H Substituting for the first term on the right hand side from Eq (1), we get µ H µ U + c 1 c µ H µ

2 3 A flask initially containing benzene (C 6 H 6 ) at its freezing temerature of 2786 K is brought into contact with an ice-water bath until 1 mole of benzene is frozen For benzene, fus H 9, 832 Jmol 1 (a) Find the entroy change for the benzene (b) Find the entroy change for the ice-water bath (c) Find the entroy change for the Universe Is this rocess sontaneous? (d) If DfusH for ice is 6,025 J mol-1, how many grams of ice would melt or freeze (state which) as a result of the rocess taking lace in the flask? (a) Entroy change for the freezing rocess for the benzene: S m fush 9832 J 2786 K J K 1 (b) Entroy change for the ice-water bath: S surr q surr 9832 J K JK 1 (c) Entroy change of the Universe: S univ JK 1 Since this is ositive, the rocess is sontaneous (d) It takes 6, 025 J to melt one mole (or g) of ice herefore, the mass of ice melted as a result of 9, 832 J being exelled into the ice-water bath will be w 9832 J gmol Jmol g 4 (Chem 420) One mole of ideal gas initially at 298 K is allowed to exand adiabatically and reversibly from 100 bar to 050 bar Find the final temerature, and U, H, q, w, and S for this rocess Since this is an ideal gas, m R Also, for an adiabatic rocess, 1 γ 1 2 γ 2, where γ C,m /C,m 5/3 herefore, 2 µ 1 2 hen, the final temerature is herefore, 3/5 µ R1 1 µ 10 bar 050 bar R 5/3 2 1 (R 1 / 1 ) 5/3 Ã 3/ LbarK 1 mol 1! K 10 U C,m ( 2 1 ) 3 2R ( ) 898 J H C,m ( 2 1 ) 5 2R ( ) 1497 J q 0by definition, for an adiabatic rocess w U 898 J S 0by definition, for an adiabatic rocess L

3 4 (Chem 523) An ice cube at 0 Cweighing100gisdroedinto1kgofwaterat20 C [ fus H for ice is 6,025 J mol 1, C,m for liquid water is 753 J K 1 mol 1 ] (a) Does all of it melt? If not, how much remains? What is the final temerature? (b) What is the entroy change of the ice + water system during this rocess? (a) Let us assume that all of the ice melts and solve for the final temerature that would result If this comes out to be below 0 C, we will have to conclude that all of the ice does not melt he basic rincile of energy conservation is sufficient to find the final temerature: heat gained heat lost, or q ice q water he heat is gained by 100 g of ice which first melts and then heats u to the final temerature: q ice 100 g gmol 1 " fus H + Z f C,m d At the same time, the water sulies this heat and cools down from 20 C (29315 K) as a result: 1000 g q water gmol 1 C,m d Using the energy conservation relationshi, we have 100 g h i gmol Jmol JK 1 mol 1 ( f 27315) K herefore, all the ice does melt (b) Entroy changes: S ice Z f 1000 g h i gmol JK 1 mol 1 ( f 29315) K K " 100 g 6025 Jmol gmol JK 1 mol 1 ln # µ # µ JK g S water gmol JK 1 mol 1 ln JK 1 S ice+water JK 1 5 A gas obeys the equation of state m R + B, whereb is a constant he C,m for this gas is a constant, equal to (3/2)R (a) Starting with the first law, derive an exression for the entroy change ds m,andthus,for S m during a reversible exansion/comression (b) If B 0015 L mol 1, what is the entroy change of the system if the gas is allowed to exand in an isobaric rocess from 100 L at 298 K to 1000 L? (a) From the first law, we get du dq + dw By definition, du C,m d Since the rocess is reversible, dq rev ds he work of exansion of a gas is dw d herefore, C,m d ds d d ds m C,m + d m d C,m + R d m m B 3

4 Integrating both sides from initial to final states, we have µ µ 2 2 B S m C,m ln + R ln 1 B 1 (b) From the equation of state, the final temerature is given by 2 ( 2 B) Sinceremains constant R during the rocess, we may substitute for using the initial conditions: R 1 /( 1 B) herefore, 2 R 1 1 B 2 B R 2 B 1 1 B K herefore, S m 15R ln µ µ R ln JK 1 mol 1 6 A reversible Joule cycle consists of four stes: isobaric exansion, adiabatic exansion, isobaric comression and, finally, adiabatic comression Sketch the ath taken by the system in such a cycle schematically using the following coordinates: (a) (, ) (b) (U, ) (c) (,S) (d) Sketch the ath taken by the system in a Carnot cycle using (,S) for coordinates See next age for the lots 4

5 Plots for Question 6: (a) (b) (c) U S (d) S

δq T = nr ln(v B/V A )

δq T = nr ln(v B/V A ) hysical Chemistry 007 Homework assignment, solutions roblem 1: An ideal gas undergoes the following reversible, cyclic rocess It first exands isothermally from state A to state B It is then comressed adiabatically

More information

Internal Energy in terms of Properties

Internal Energy in terms of Properties Lecture #3 Internal Energy in terms of roerties Internal energy is a state function. A change in the state of the system causes a change in its roerties. So, we exress the change in internal energy in

More information

Chapter-6: Entropy. 1 Clausius Inequality. 2 Entropy - A Property

Chapter-6: Entropy. 1 Clausius Inequality. 2 Entropy - A Property hater-6: Entroy When the first law of thermodynamics was stated, the existence of roerty, the internal energy, was found. imilarly, econd law also leads to definition of another roerty, known as entroy.

More information

Lecture 13 Heat Engines

Lecture 13 Heat Engines Lecture 3 Heat Engines hermodynamic rocesses and entroy hermodynamic cycles Extracting work from heat - How do we define engine efficiency? - Carnot cycle: the best ossible efficiency Reading for this

More information

Chapter 20: Exercises: 3, 7, 11, 22, 28, 34 EOC: 40, 43, 46, 58

Chapter 20: Exercises: 3, 7, 11, 22, 28, 34 EOC: 40, 43, 46, 58 Chater 0: Exercises:, 7,,, 8, 4 EOC: 40, 4, 46, 8 E: A gasoline engine takes in.80 0 4 and delivers 800 of work er cycle. The heat is obtained by burning gasoline with a heat of combustion of 4.60 0 4.

More information

Lecture 13. Heat Engines. Thermodynamic processes and entropy Thermodynamic cycles Extracting work from heat

Lecture 13. Heat Engines. Thermodynamic processes and entropy Thermodynamic cycles Extracting work from heat Lecture 3 Heat Engines hermodynamic rocesses and entroy hermodynamic cycles Extracting work from heat - How do we define engine efficiency? - Carnot cycle: the best ossible efficiency Reading for this

More information

I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class.

I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class. Chem340 Physical Chemistry for Biochemists Exam Mar 16, 011 Your Name _ I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade

More information

Chemistry 531 Spring 2009 Problem Set 6 Solutions

Chemistry 531 Spring 2009 Problem Set 6 Solutions Chemistry 531 Sring 2009 Problem Set 6 Solutions 1. In a thermochemical study of N 2, the following heat caacity data were found: t 0 C,m d 27.2Jmol 1 K 1 f t b f C,m d 23.4Jmol 1 K 1 C,m d 11.4Jmol 1

More information

PHYS1001 PHYSICS 1 REGULAR Module 2 Thermal Physics Chapter 17 First Law of Thermodynamics

PHYS1001 PHYSICS 1 REGULAR Module 2 Thermal Physics Chapter 17 First Law of Thermodynamics PHYS1001 PHYSICS 1 REGULAR Module Thermal Physics Chater 17 First Law of Thermodynamics References: 17.1 to 17.9 Examles: 17.1 to 17.7 Checklist Thermodynamic system collection of objects and fields. If

More information

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential Chem 467 Sulement to Lectures 33 Phase Equilibrium Chemical Potential Revisited We introduced the chemical otential as the conjugate variable to amount. Briefly reviewing, the total Gibbs energy of a system

More information

I have not proofread these notes; so please watch out for typos, anything misleading or just plain wrong.

I have not proofread these notes; so please watch out for typos, anything misleading or just plain wrong. hermodynamics I have not roofread these notes; so lease watch out for tyos, anything misleading or just lain wrong. Please read ages 227 246 in Chater 8 of Kittel and Kroemer and ay attention to the first

More information

1. Read the section on stability in Wallace and Hobbs. W&H 3.53

1. Read the section on stability in Wallace and Hobbs. W&H 3.53 Assignment 2 Due Set 5. Questions marked? are otential candidates for resentation 1. Read the section on stability in Wallace and Hobbs. W&H 3.53 2.? Within the context of the Figure, and the 1st law of

More information

GEF2200 vår 2017 Løsningsforslag sett 1

GEF2200 vår 2017 Løsningsforslag sett 1 GEF2200 vår 2017 Løsningsforslag sett 1 A.1.T R is the universal gas constant, with value 8.3143JK 1 mol 1. R is the gas constant for a secic gas, given by R R M (1) where M is the molecular weight of

More information

COMPENDIUM OF EQUATIONS Unified Engineering Thermodynamics

COMPENDIUM OF EQUATIONS Unified Engineering Thermodynamics COMPENDIUM OF EQUAIONS Unified Engineering hermodynamics Note: It is with some reseration that I suly this comendium of equations. One of the common itfalls for engineering students is that they sole roblems

More information

02. Equilibrium Thermodynamics II: Engines

02. Equilibrium Thermodynamics II: Engines University of Rhode Island DigitalCommons@URI Equilibrium Statistical Physics Physics Course Materials 205 02. Equilibrium Thermodynamics II: Engines Gerhard Müller University of Rhode Island, gmuller@uri.edu

More information

Thermodynamics in combustion

Thermodynamics in combustion Thermodynamics in combustion 2nd ste in toolbox Thermodynamics deals with a equilibrium state and how chemical comosition can be calculated for a system with known atomic or molecular comosition if 2 indeendent

More information

The Second Law: The Machinery

The Second Law: The Machinery The Second Law: The Machinery Chater 5 of Atkins: The Second Law: The Concets Sections 3.7-3.9 8th Ed, 3.3 9th Ed; 3.4 10 Ed.; 3E 11th Ed. Combining First and Second Laws Proerties of the Internal Energy

More information

whether a process will be spontaneous, it is necessary to know the entropy change in both the

whether a process will be spontaneous, it is necessary to know the entropy change in both the 93 Lecture 16 he entroy is a lovely function because it is all we need to know in order to redict whether a rocess will be sontaneous. However, it is often inconvenient to use, because to redict whether

More information

THERMODYNAMICS. Prepared by Sibaprasad Maity Asst. Prof. in Chemistry For any queries contact at

THERMODYNAMICS. Prepared by Sibaprasad Maity Asst. Prof. in Chemistry For any queries contact at HERMODYNAMIS reared by Sibarasad Maity Asst. rof. in hemistry For any queries contact at 943445393 he word thermo-dynamic, used first by illiam homson (later Lord Kelvin), has Greek origin, and is translated

More information

The Second Law of Thermodynamics. (Second Law of Thermodynamics)

The Second Law of Thermodynamics. (Second Law of Thermodynamics) he Second aw of hermodynamics For the free exansion, we have >. It is an irreversible rocess in a closed system. For the reversible isothermal rocess, for the gas > for exansion and < for comression. owever,

More information

Efficiencies. Damian Vogt Course MJ2429. Nomenclature. Symbol Denotation Unit c Flow speed m/s c p. pressure c v. Specific heat at constant J/kgK

Efficiencies. Damian Vogt Course MJ2429. Nomenclature. Symbol Denotation Unit c Flow speed m/s c p. pressure c v. Specific heat at constant J/kgK Turbomachinery Lecture Notes 1 7-9-1 Efficiencies Damian Vogt Course MJ49 Nomenclature Subscrits Symbol Denotation Unit c Flow seed m/s c Secific heat at constant J/kgK ressure c v Secific heat at constant

More information

CHAPTER 3 LECTURE NOTES 3.1. The Carnot Cycle Consider the following reversible cyclic process involving one mole of an ideal gas:

CHAPTER 3 LECTURE NOTES 3.1. The Carnot Cycle Consider the following reversible cyclic process involving one mole of an ideal gas: CHATER 3 LECTURE NOTES 3.1. The Carnot Cycle Consider the following reversible cyclic process involving one mole of an ideal gas: Fig. 3. (a) Isothermal expansion from ( 1, 1,T h ) to (,,T h ), (b) Adiabatic

More information

Calculators are permitted. Computers, PDAs, and other electronic devices with a keyboard are not. Cell phones may not be used as calculators.

Calculators are permitted. Computers, PDAs, and other electronic devices with a keyboard are not. Cell phones may not be used as calculators. Chem. 30 Sring 008 Exam 3 VERSION A Professors Williams/Whetten his test is closed note/book One 8.5 x handwritten crib sheet (one sided) is ermitted. Please turn off your cell hone. Use a # encil. Calculators

More information

General Physical Chemistry I

General Physical Chemistry I General Physical Cheistry I Lecture 12 Aleksey Kocherzhenko Aril 2, 2015" Last tie " Gibbs free energy" In order to analyze the sontaneity of cheical reactions, we need to calculate the entroy changes

More information

Sec# Wave Motion - Superposition and Interference of Waves Grade# 50

Sec# Wave Motion - Superposition and Interference of Waves Grade# 50 Coordinator: Dr. A. Naqvi Saturday, August 0, 009 Page: Q. The function y(x,t) = 5.0 cos (x- 0 t) with x and y in meters and t in seconds, describes a wave on a taut string. What is the mass of one meter

More information

Liquid water static energy page 1/8

Liquid water static energy page 1/8 Liquid water static energy age 1/8 1) Thermodynamics It s a good idea to work with thermodynamic variables that are conserved under a known set of conditions, since they can act as assive tracers and rovide

More information

THE FIRST LAW OF THERMODYNAMICS

THE FIRST LAW OF THERMODYNAMICS THE FIRST LA OF THERMODYNAMIS 9 9 (a) IDENTIFY and SET UP: The ressure is constant and the volume increases (b) = d Figure 9 Since is constant, = d = ( ) The -diagram is sketched in Figure 9 The roblem

More information

ATMOS Lecture 7. The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Capacity Special Cases of the First Law

ATMOS Lecture 7. The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Capacity Special Cases of the First Law TMOS 5130 Lecture 7 The First Law and Its Consequences Pressure-Volume Work Internal Energy Heat Caacity Secial Cases of the First Law Pressure-Volume Work Exanding Volume Pressure δw = f & dx δw = F ds

More information

HEAT, WORK, AND THE FIRST LAW OF THERMODYNAMICS

HEAT, WORK, AND THE FIRST LAW OF THERMODYNAMICS HET, ORK, ND THE FIRST L OF THERMODYNMIS 8 EXERISES Section 8. The First Law of Thermodynamics 5. INTERPRET e identify the system as the water in the insulated container. The roblem involves calculating

More information

U = 4.18 J if we heat 1.0 g of water through 1 C. U = 4.18 J if we cool 1.0 g of water through 1 C.

U = 4.18 J if we heat 1.0 g of water through 1 C. U = 4.18 J if we cool 1.0 g of water through 1 C. CHAPER LECURE NOES he First Law of hermodynamics: he simplest statement of the First Law is as follows: U = q + w. Here U is the internal energy of the system, q is the heat and w is the work. CONVENIONS

More information

Thermodynamics (XI) Assignment(Solution)

Thermodynamics (XI) Assignment(Solution) SYLLABUS CUM COM./XI/03 4 hermodynamics (XI) Assignment(Solution) Comprehension ype Questions aragraph for Question -5 For an ideal gas, an illustration of three different paths A, (B + C) and (D + E)

More information

/ p) TA,. Returning to the

/ p) TA,. Returning to the Toic2610 Proerties; Equilibrium and Frozen A given closed system having Gibbs energy G at temerature T, ressure, molecular comosition (organisation ) and affinity for sontaneous change A is described by

More information

Actual exergy intake to perform the same task

Actual exergy intake to perform the same task CHAPER : PRINCIPLES OF ENERGY CONSERVAION INRODUCION Energy conservation rinciles are based on thermodynamics If we look into the simle and most direct statement of the first law of thermodynamics, we

More information

Non-Equilibrium Thermodynamics for Engineers

Non-Equilibrium Thermodynamics for Engineers Non-Equilibrium Thermodynamics for Engineers How do we find the otimal rocess unit? Signe Kjelstru, Chair of Engineering Thermodynamics Deartment of Process and Energy TU Delft ecture no. 7 Why is the

More information

NODIA AND COMPANY. GATE SOLVED PAPER Mechanical Engineering Thermodynamics. Copyright By NODIA & COMPANY

NODIA AND COMPANY. GATE SOLVED PAPER Mechanical Engineering Thermodynamics. Copyright By NODIA & COMPANY No art of this ublication may be reroduced or distributed in any form or any means, electronic, mechanical, hotocoying, or otherwise without the rior ermission of the author. GAE SOLVED PAPER Mechanical

More information

F = U TS G = H TS. Availability, Irreversibility S K Mondal s Chapter 5. max. actual. univ. Ns =

F = U TS G = H TS. Availability, Irreversibility S K Mondal s Chapter 5. max. actual. univ. Ns = Availability, Irreversibility S K Mondal s Chater 5 I = W W 0 max ( S) = Δ univ actual 7. Irreversibility rate = I = rate of energy degradation = rate of energy loss (Wlost) = 0 S gen for all rocesses

More information

Homework Problem Set 8 Solutions

Homework Problem Set 8 Solutions Chemistry 360 Dr. Jean M. Standard Homework roblem Set 8 Solutions. Starting from G = H S, derive the fundamental equation for G. o begin, we take the differential of G, dg = dh d( S) = dh ds Sd. Next,

More information

Unit code: H/ QCF level: 5 Credit value: 15 OUTCOME 1 - THERMODYNAMIC SYSTEMS TUTORIAL 2

Unit code: H/ QCF level: 5 Credit value: 15 OUTCOME 1 - THERMODYNAMIC SYSTEMS TUTORIAL 2 Unit 43: Plant and Process Princiles Unit code: H/60 44 QCF level: 5 Credit value: 5 OUCOME - HERMODYNAMIC SYSEMS UORIAL Understand thermodynamic systems as alied to lant engineering rocesses hermodynamic

More information

Homework Week 8 G = H T S. Given that G = H T S, using the first and second laws we can write,

Homework Week 8 G = H T S. Given that G = H T S, using the first and second laws we can write, Statistical Molecular hermodynamics University of Minnesota Homework Week 8 1. By comparing the formal derivative of G with the derivative obtained taking account of the first and second laws, use Maxwell

More information

Foundations of thermodynamics Fundamental thermodynamical concepts

Foundations of thermodynamics Fundamental thermodynamical concepts Foundations of thermodynamics Fundamental thermodynamical concets System is the macrohysical entity under consideration Surrounding is the wld outside of the system Oen system can exchange matter heat

More information

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

UNIT # 06 THERMODYNAMICS EXERCISE # 1. T i. 1. m Zn UNI # 6 HERMODYNMIS EXERISE #. m Zn.S Zn.( f i + m H O.S H O.( f i (6.8 gm (.4 J/g ( f + 8 gm (4. J/g ( f [(6.8 (.4 + 8(4.] f (6.8 (.4 ( + (8 (4. ( (6.8(.4( (8(4.( f 97. (6.8(.4 (8(4.. U q + w heat absorb

More information

Entropy Changes & Processes

Entropy Changes & Processes Entropy Changes & Processes Chapter 4 of Atkins: he Second Law: he Concepts Section 4.3 Entropy of Phase ransition at the ransition emperature Expansion of the Perfect Gas Variation of Entropy with emperature

More information

Entransy analysis of open thermodynamic systems

Entransy analysis of open thermodynamic systems Article Engineering hermohysics August 0 Vol.57 No.: 934940 doi: 0.007/s434-0-54-x Entransy analysis of oen thermodynamic systems CHENG Xueao, WANG WenHua & LIANG XinGang * Key Laboratory for hermal Science

More information

pv m = RT + Bp The simplest equation for calculating fugacity, given an equation of state, is Z=1 + B RT p

pv m = RT + Bp The simplest equation for calculating fugacity, given an equation of state, is Z=1 + B RT p Chem 42/523 Chemical hermodynamics Homework Assignment # 5 1. *Assume O 2 gas obeys the virial equation pv m = R + Bp with B = 12.5 cm 3 mol 1 at 298.15 K. Calculate the fugacity of oxygen at p = 1. MPa

More information

Exam 1 Solutions 100 points

Exam 1 Solutions 100 points Chemistry 360 Fall 018 Dr. Jean M. Standard September 19, 018 Name KEY Exam 1 Solutions 100 points 1.) (14 points) A chunk of gold metal weighing 100.0 g at 800 K is dropped into 100.0 g of liquid water

More information

Test Date: (Saturday) Test Time: 09:45 AM to 11:45 AM

Test Date: (Saturday) Test Time: 09:45 AM to 11:45 AM Test ate: 8..5 (Saturday) Test Time: 9:5 M to :5 M Test Venue: Lajat hawan, Madhya Marg, Sector 5-, handigarh r. Sangeeta Khanna Ph. HEMISTRY OHING IRLE r. Sangeeta Khanna Ph. TEST TE: 8..5 RE THE INSTRUTIONS

More information

A short note on Reitlinger thermodynamic cycles

A short note on Reitlinger thermodynamic cycles short note on Reitlinger thermodynamic cycles melia arolina Saravigna eartment of lied Science and echnology, Politecnico di orino, orino, Italy bstract: It is well known that arnot cycle is the thermodynamic

More information

Phase transition. Asaf Pe er Background

Phase transition. Asaf Pe er Background Phase transition Asaf Pe er 1 November 18, 2013 1. Background A hase is a region of sace, throughout which all hysical roerties (density, magnetization, etc.) of a material (or thermodynamic system) are

More information

Physics 2A (Fall 2012) Chapters 11:Using Energy and 12: Thermal Properties of Matter

Physics 2A (Fall 2012) Chapters 11:Using Energy and 12: Thermal Properties of Matter Physics 2A (Fall 2012) Chaters 11:Using Energy and 12: Thermal Proerties of Matter "Kee in mind that neither success nor failure is ever final." Roger Ward Babson Our greatest glory is not in never failing,

More information

P340: Thermodynamics and Statistical Physics, Exam#2 Any answer without showing your work will be counted as zero

P340: Thermodynamics and Statistical Physics, Exam#2 Any answer without showing your work will be counted as zero P340: hermodynamics and Statistical Physics, Exam#2 Any answer without showing your work will be counted as zero 1. (15 points) he equation of state for the an der Waals gas (n = 1 mole) is (a) Find (

More information

FUGACITY. It is simply a measure of molar Gibbs energy of a real gas.

FUGACITY. It is simply a measure of molar Gibbs energy of a real gas. FUGACITY It is simly a measure of molar Gibbs energy of a real gas. Modifying the simle equation for the chemical otential of an ideal gas by introducing the concet of a fugacity (f). The fugacity is an

More information

Thermodynamics I Chapter 6 Entropy

Thermodynamics I Chapter 6 Entropy hermodynamics I hater 6 Entroy Mohsin Mohd ies Fakulti Keuruteraan Mekanikal, Uniersiti eknologi Malaysia Entroy (Motiation) he referred direction imlied by the nd Law can be better understood and quantified

More information

Entropy and the Second Law of Thermodynamics

Entropy and the Second Law of Thermodynamics Entropy and the Second Law of hermodynamics Reading Problems 6-, 6-2, 6-7, 6-8, 6-6-8, 6-87, 7-7-0, 7-2, 7-3 7-39, 7-46, 7-6, 7-89, 7-, 7-22, 7-24, 7-30, 7-55, 7-58 Why do we need another law in thermodynamics?

More information

Entropy Changes & Processes

Entropy Changes & Processes Entropy Changes & Processes Chapter 4 of Atkins: he Second Law: he Concepts Section 4.3, 7th edition; 3.3, 8th and 9th editions Entropy of Phase ransition at the ransition emperature Expansion of the Perfect

More information

Version 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1

Version 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1 Version 001 HW 15 Thermodynamics C&J sizemore 21301jtsizemore 1 This print-out should have 38 questions. Multiple-choice questions may continue on the next column or page find all choices before answering.

More information

Maximum Power Output of Quantum Heat Engine. with Energy Bath

Maximum Power Output of Quantum Heat Engine. with Energy Bath Maximum Power Outut of Quantum Heat Engine with Energy Bath Shengnan Liu, Congjie Ou, College of Information Science and Engineering, Huaqiao University, Xiamen 360, China; 30008003@hqu.edu.cn Corresondence:

More information

Class XI Chapter 6 Thermodynamics Question 6.1: Choose the correct answer. A thermodynamic state function is a quantity (i) used to determine heat changes (ii) whose value is independent of path (iii)

More information

FINITE TIME THERMODYNAMIC MODELING AND ANALYSIS FOR AN IRREVERSIBLE ATKINSON CYCLE. By Yanlin GE, Lingen CHEN, and Fengrui SUN

FINITE TIME THERMODYNAMIC MODELING AND ANALYSIS FOR AN IRREVERSIBLE ATKINSON CYCLE. By Yanlin GE, Lingen CHEN, and Fengrui SUN FINIE IME HERMODYNAMIC MODELING AND ANALYSIS FOR AN IRREVERSIBLE AKINSON CYCLE By Yanlin GE, Lingen CHEN, and Fengrui SUN Performance of an air-standard Atkinson cycle is analyzed by using finite-time

More information

Lecture. Polymer Thermodynamics 0331 L First and Second Law of Thermodynamics

Lecture. Polymer Thermodynamics 0331 L First and Second Law of Thermodynamics 1 Prof. Dr. rer. nat. habil. S. Enders Faculty III for Process Science Institute of Chemical Engineering Department of hermodynamics Lecture Polymer hermodynamics 0331 L 337 2.1. First Law of hermodynamics

More information

The extreme case of the anisothermal calorimeter when there is no heat exchange is the adiabatic calorimeter.

The extreme case of the anisothermal calorimeter when there is no heat exchange is the adiabatic calorimeter. .4. Determination of the enthaly of solution of anhydrous and hydrous sodium acetate by anisothermal calorimeter, and the enthaly of melting of ice by isothermal heat flow calorimeter Theoretical background

More information

Review of classical thermodynamics

Review of classical thermodynamics Review of classical thermodynamics Fundamental Laws, Properties and Processes (2) Entropy and the Second Law Concepts of equilibrium Reversible and irreversible processes he direction of spontaneous change

More information

Basic Thermodynamic Relations

Basic Thermodynamic Relations Basic herodynaic Relations Isolated syste: this is a syste that does not exchange energy with the surrounding edia. First Postulate (equilibriu theore) : Isolated syste always reaches the equilibriu state

More information

Chapter 6. Thermodynamics and the Equations of Motion

Chapter 6. Thermodynamics and the Equations of Motion Chater 6 hermodynamics and the Equations of Motion 6.1 he first law of thermodynamics for a fluid and the equation of state. We noted in chater 4 that the full formulation of the equations of motion required

More information

REAL GASES. (B) pv. (D) pv. 3. The compressibility factor of a gas is less than unity at STP. Therefore, molar volume (V m.

REAL GASES. (B) pv. (D) pv. 3. The compressibility factor of a gas is less than unity at STP. Therefore, molar volume (V m. SINGLE ORRET ANSWER REAL GASES 1. A real gas is suosed to obey the gas equation ( b) = at STP. If one mole of a gas occuies 5dm 3 volume at STP, then its comressibility factor is (b=.586 L mol 1F) (A)

More information

PV/T = k or PV = kt Describe the difference between an ideal gas and a real gas.

PV/T = k or PV = kt Describe the difference between an ideal gas and a real gas. 10.1 Thermodynamics 10.2 Processes 10 10.3 The second law of thermodynamics and entroy 10.1 Thermodynamics From the combined gas laws, we determined that: P/T = k or P = kt 10.1.1 State the equation of

More information

Chapter 9 Practical cycles

Chapter 9 Practical cycles Prof.. undararajan Chater 9 Practical cycles 9. Introduction In Chaters 7 and 8, it was shown that a reversible engine based on the Carnot cycle (two reversible isothermal heat transfers and two reversible

More information

Unit 7 (B) Solid state Physics

Unit 7 (B) Solid state Physics Unit 7 (B) Solid state Physics hermal Properties of solids: Zeroth law of hermodynamics: If two bodies A and B are each separated in thermal equilibrium with the third body C, then A and B are also in

More information

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

UNIVERSITY OF TORONTO FACULTY OF APPLIED SCIENCE AND ENGINEERING TERM TEST 2 17 MARCH First Year APS 104S UNIERSIY OF ORONO Please mark X to indicate your tutorial section. Failure to do so will result in a deduction of 3 marks. U 0 U 0 FACULY OF APPLIED SCIENCE AND ENGINEERING ERM ES 7 MARCH 05 U 03 U 04

More information

Lecture Thermodynamics 9. Entropy form of the 1 st law. Let us start with the differential form of the 1 st law: du = d Q + d W

Lecture Thermodynamics 9. Entropy form of the 1 st law. Let us start with the differential form of the 1 st law: du = d Q + d W Lecture hermodnamics 9 Entro form of the st law Let us start with the differential form of the st law: du = d Q + d W Consider a hdrostatic sstem. o know the required d Q and d W between two nearb states,

More information

4. A Brief Review of Thermodynamics, Part 2

4. A Brief Review of Thermodynamics, Part 2 ATMOSPHERE OCEAN INTERACTIONS :: LECTURE NOTES 4. A Brief Review of Thermodynamics, Part 2 J. S. Wright jswright@tsinghua.edu.cn 4.1 OVERVIEW This chater continues our review of the key thermodynamics

More information

Week 8 lectures. ρ t +u ρ+ρ u = 0. where µ and λ are viscosity and second viscosity coefficients, respectively and S is the strain tensor:

Week 8 lectures. ρ t +u ρ+ρ u = 0. where µ and λ are viscosity and second viscosity coefficients, respectively and S is the strain tensor: Week 8 lectures. Equations for motion of fluid without incomressible assumtions Recall from week notes, the equations for conservation of mass and momentum, derived generally without any incomressibility

More information

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

THE ZEROTH AND FISRT LAW OF THERMODYNAMICS. Saeda Al-Mhyawi secend Tearm 1435H H ZROH AND FISR LAW OF HRMODYNAMIS Saeda Al-Mhyawi secend earm 435H HAR II H ZROH AND FISR LAW OF HRMODYNAMIS Lecture () Outline Introduction he Zeroth Law of hermodynamics he First Law of hermodynamics

More information

THERMODYNAMICS CONTENTS

THERMODYNAMICS CONTENTS 1. Introduction HERMODYNAMICS CONENS. Maxwell s thermodynamic equations.1 Derivation of Maxwell s equations 3. Function and derivative 3.1 Differentiation 4. Cyclic Rule artial Differentiation 5. State

More information

T ice T water T water = T ice =0 0 C. e =1

T ice T water T water = T ice =0 0 C. e =1 Given 1 kg of water at 100 0 C and a very large (very very large) block of ice at 0 0 C. A reversible heat engine absorbs heat from the water and expels heat to the ice until work can no longer be extracted

More information

df da df = force on one side of da due to pressure

df da df = force on one side of da due to pressure I. Review of Fundamental Fluid Mechanics and Thermodynamics 1. 1 Some fundamental aerodynamic variables htt://en.wikiedia.org/wiki/hurricane_ivan_(2004) 1) Pressure: the normal force er unit area exerted

More information

Handout 12: Thermodynamics. Zeroth law of thermodynamics

Handout 12: Thermodynamics. Zeroth law of thermodynamics 1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures

More information

Ideal Gas Law. September 2, 2014

Ideal Gas Law. September 2, 2014 Ideal Gas Law Setember 2, 2014 Thermodynamics deals with internal transformations of the energy of a system and exchanges of energy between that system and its environment. A thermodynamic system refers

More information

Supplemental Activities. Module: Thermodynamics. Section: Second Law of Thermodynamics Key

Supplemental Activities. Module: Thermodynamics. Section: Second Law of Thermodynamics Key Supplemental Activities Module: Thermodynamics Section: Second Law of Thermodynamics Key Spontaneity ACTIVITY 1 The purpose of this activity is to practice your understanding of the concept of spontaneous

More information

CY1001 BASIC CONCEPTS

CY1001 BASIC CONCEPTS CY1001 BASIC CONCES Lecture 1. radeep 22574208 pradeep@iitm.ac.in Atomists and ionists 9/6/2010 1 1. Chemical thermodynamics 2. Statistical thermodynamics 3. Kinetics 4. Surface science Books: 1. G. W.

More information

Problem: Calculate the entropy change that results from mixing 54.0 g of water at 280 K with 27.0 g of water at 360 K in a vessel whose walls are

Problem: Calculate the entropy change that results from mixing 54.0 g of water at 280 K with 27.0 g of water at 360 K in a vessel whose walls are Problem: Calculate the entropy change that results from mixing 54.0 g of water at 280 K with 27.0 g of water at 360 K in a vessel whose walls are perfectly insulated from the surroundings. Is this a spontaneous

More information

AT 25 C! CH10090 Thermodynamics (part 2) Enthalpy changes during reactions. Let s remember what we did in CH10089

AT 25 C! CH10090 Thermodynamics (part 2) Enthalpy changes during reactions. Let s remember what we did in CH10089 CH10090 hermodynamics (art ) Let s remember what we did in CH10089 Enthaly changes during reactions o o o H98 ( reaction) = νi Hf, 98( roducts) νi Hf, 98( reactants) ν i reresents the stoichiometric coefficient.

More information

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?

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? 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? 1. The Dispersal of Energy YES 2. Entropy YES We won

More information

Equations: q trans = 2 mkt h 2. , Q = q N, Q = qn N! , < P > = kt P = , C v = < E > V 2. e 1 e h /kt vib = h k = h k, rot = h2.

Equations: q trans = 2 mkt h 2. , Q = q N, Q = qn N! , < P > = kt P = , C v = < E > V 2. e 1 e h /kt vib = h k = h k, rot = h2. Constants: R = 8.314 J mol -1 K -1 = 0.08206 L atm mol -1 K -1 k B = 0.697 cm -1 /K = 1.38 x 10-23 J/K 1 a.m.u. = 1.672 x 10-27 kg 1 atm = 1.0133 x 10 5 Nm -2 = 760 Torr h = 6.626 x 10-34 Js For H 2 O

More information

First law of thermodynamics (Jan 12, 2016) page 1/7. Here are some comments on the material in Thompkins Chapter 1

First law of thermodynamics (Jan 12, 2016) page 1/7. Here are some comments on the material in Thompkins Chapter 1 First law of thermodynamics (Jan 12, 2016) age 1/7 Here are some comments on the material in Thomkins Chater 1 1) Conservation of energy Adrian Thomkins (eq. 1.9) writes the first law as: du = d q d w

More information

Session 12 : Monopropellant Thrusters

Session 12 : Monopropellant Thrusters Session 12 : Monoroellant Thrusters Electrothermal augmentation of chemical rockets was the first form of electric roulsion alied in sace vehicles. In its original imlementation, resistojets were used

More information

Chemistry 452 July 23, Enter answers in a Blue Book Examination

Chemistry 452 July 23, Enter answers in a Blue Book Examination Chemistry 45 July 3, 014 Enter answers in a Blue Book Examination Midterm Useful Constants: 1 Newton=1 N= 1 kg m s 1 Joule=1J=1 N m=1 kg m /s 1 Pascal=1Pa=1N m 1atm=10135 Pa 1 bar=10 5 Pa 1L=0.001m 3 Universal

More information

SPONTANEOUS PROCESSES AND THERMODYNAMIC EQUILIBRIUM

SPONTANEOUS PROCESSES AND THERMODYNAMIC EQUILIBRIUM 13 CHAPER SPONANEOUS PROCESSES AND HERMODYNAMIC EQUILIBRIUM 13.1 he Nature of Spontaneous Processes 13.2 Entropy and Spontaneity: A Molecular Statistical Interpretation 13.3 Entropy and Heat: Macroscopic

More information

CHEM Introduction to Thermodynamics Fall Entropy and the Second Law of Thermodynamics

CHEM Introduction to Thermodynamics Fall Entropy and the Second Law of Thermodynamics CHEM2011.03 Introduction to Thermodynamics Fall 2003 Entropy and the Second Law of Thermodynamics Introduction It is a matter of everyday observation that things tend to change in a certain direction.

More information

Example problems. Chapter 2: Temperature, heat, and the 1 st law of Thermodynamic. Homework: 2, 3, 4, 5, 6, 10, 15, 19, 21 (pages )

Example problems. Chapter 2: Temperature, heat, and the 1 st law of Thermodynamic. Homework: 2, 3, 4, 5, 6, 10, 15, 19, 21 (pages ) Examle roblems Chater : emerature, heat, and the 1 st law of hermodynamic Homework:,, 4, 5, 6, 1, 15, 19, 1 (ages 5-51) . (Page 5) wo constant-volume gas thermometers are assembled, one with nitrogen and

More information

Work, heat and the first law of thermodynamics

Work, heat and the first law of thermodynamics Chapter 3 Work, heat and the first law of thermodynamics 3.1 Mechanical work Mechanical work is defined as an energy transfer to the system through the change of an external parameter. Work is the only

More information

The Second Law of Thermodynamics (Chapter 4)

The Second Law of Thermodynamics (Chapter 4) The Second Law of Thermodynamics (Chapter 4) First Law: Energy of universe is constant: ΔE system = - ΔE surroundings Second Law: New variable, S, entropy. Changes in S, ΔS, tell us which processes made

More information

Chemistry 163B Winter 2013 notes for lecture 4

Chemistry 163B Winter 2013 notes for lecture 4 Chemistry 163B Lecture 4 Winter 013 Challenged enmanship Notes 1 st Law recapitulation U internal energy du = dq + dw + dn sys sys sys sys sys surr du du energy conserved (n=number of moles; dn=0 for closed

More information

Problem Set 10 Solutions

Problem Set 10 Solutions Chemistry 360 Dr Jean M Standard Problem Set 10 Solutions 1 Sketch (roughly to scale) a phase diagram for molecular oxygen given the following information: the triple point occurs at 543 K and 114 torr;

More information

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

First Law CML 100, IIT Delhi SS. The total energy of the system. Contribution from translation + rotation + vibrations. Internal Energy he total energy of the system. Contribution from translation + rotation + vibrations. Equipartition theorem for the translation and rotational degrees of freedom. 1/ k B Work Path function,

More information

Atmospheric Thermodynamics

Atmospheric Thermodynamics Atmosheric hermodynamics 3 he theory of thermodynamics is one of the cornerstones and crowning glories of classical hysics. It has alications not only in hysics, chemistry, and the Earth sciences, but

More information

1. Foundations of thermodynamics 1.1. Fundamental thermodynamical concepts. Introduction. Summary of contents:

1. Foundations of thermodynamics 1.1. Fundamental thermodynamical concepts. Introduction. Summary of contents: Introduction hermodynamics: henomenological descrition of equilibrium bulk roerties of matter in terms of only a few state variables thermodynamical laws Statistical hysics: microscoic foundation of thermodynamics

More information

Thermodynamic Properties are Measurements p,t,v, u,h,s - measure directly -measure by change

Thermodynamic Properties are Measurements p,t,v, u,h,s - measure directly -measure by change Thermodynamic Proerties are Measurements,T,, u,h,s - measure directly -measure by change s Tables T T Proerty Data Cure its Tables Correlation's, Boyles Law Tables c@tc limited hand calculations Equations

More information

Grain elevator. You need to convince your boss that this is a very inefficient system.

Grain elevator. You need to convince your boss that this is a very inefficient system. Grain elevator You are working for a grain storage comany over the summer, and they have a roblem with the grain elevator, that kees breaking down. This morning, your boss woke u feeling like a genius

More information