TEST 5 (phy 240) 2. Show that the volume coefficient of thermal expansion for an ideal gas at constant pressure is temperature dependent and given by

Similar documents
Force = F Piston area = A

Chapter 5 rd Law of Thermodynamics

Chapters 18 & 19: Themodynamics review. All macroscopic (i.e., human scale) quantities must ultimately be explained on the microscopic scale.

General Formulas applicable to ALL processes in an Ideal Gas:

Chapter 20 The First Law of Thermodynamics

University Physics AI No. 10 The First Law of Thermodynamics

ESCI 341 Atmospheric Thermodynamics Lesson 6 Thermodynamic Processes

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2014

Thermodynamics and Gases

Homework Chapter 21 Solutions!!

PES 2130 Fall 2014, Spendier Lecture 7/Page 1

Thermodynamics Second Law Entropy

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2014

A quote of the week (or camel of the week): There is no expedience to which a man will not go to avoid the labor of thinking. Thomas A.

Physics 3 (PHYF144) Chap 2: Heat and the First Law of Thermodynamics System. Quantity Positive Negative

Isothermal vs. adiabatic compression

Spring Force and Power

ECEN 5005 Crystals, Nanocrystals and Device Applications Class 19 Group Theory For Crystals

Lecture 3 Examples and Problems

PHYS 1443 Section 004 Lecture #12 Thursday, Oct. 2, 2014

Physics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Chapter 21 - The Kinetic Theory of Gases

Lecture. Polymer Thermodynamics 0331 L Chemical Potential

Assignment 4. Adsorption Isotherms

Exercises of Fundamentals of Chemical Processes

PHYS 1441 Section 002 Lecture #15

36.1 Why is it important to be able to find roots to systems of equations? Up to this point, we have discussed how to find the solution to

Chapter 6 Second Law of Thermodynamics

Physical Chemistry I for Biochemists. Chem340. Lecture 16 (2/18/11)

Problem Set #6 solution, Chem 340, Fall 2013 Due Friday, Oct 11, 2013 Please show all work for credit

Estimation of the composition of the liquid and vapor streams exiting a flash unit with a supercritical component

y i x P vap 10 A T SOLUTION TO HOMEWORK #7 #Problem

Problem Free Expansion of Ideal Gas

Work is the change in energy of a system (neglecting heat transfer). To examine what could

( ) 1/ 2. ( P SO2 )( P O2 ) 1/ 2.

OPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming

Name: SID: Discussion Session:

Physics 2A Chapters 6 - Work & Energy Fall 2017

Quantum Mechanics I - Session 4

G4023 Mid-Term Exam #1 Solutions

EN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics

Physics 240: Worksheet 30 Name:

Physical Chemistry I for Biochemists. Lecture 18 (2/23/11) Announcement

χ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body

Numerical Transient Heat Conduction Experiment

Temperature. Chapter Heat Engine

#64. ΔS for Isothermal Mixing of Ideal Gases

Chemical Engineering Department University of Washington

Lecture 2 Solution of Nonlinear Equations ( Root Finding Problems )

Physics 207 Lecture 27

SUMMARY OF STOICHIOMETRIC RELATIONS AND MEASURE OF REACTIONS' PROGRESS AND COMPOSITION FOR MULTIPLE REACTIONS

Momentum. Momentum. Impulse. Momentum and Collisions

A Tale of Friction Basic Rollercoaster Physics. Fahrenheit Rollercoaster, Hershey, PA max height = 121 ft max speed = 58 mph

Chapter 3 Differentiation and Integration

FEEDBACK AMPLIFIERS. v i or v s v 0

CinChE Problem-Solving Strategy Chapter 4 Development of a Mathematical Model. formulation. procedure

4.2 Chemical Driving Force

Chapter 3 and Chapter 4

Complex Variables. Chapter 18 Integration in the Complex Plane. March 12, 2013 Lecturer: Shih-Yuan Chen

Chapter 07: Kinetic Energy and Work

Physics 114 Exam 2 Fall 2014 Solutions. Name:

Endogenous timing in a mixed oligopoly consisting of a single public firm and foreign competitors. Abstract

Med Phys 4R06/6R03 Laboratory Experiment #6 MULTICHANNEL PULSE SPECTROMETRY

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

ONE-DIMENSIONAL COLLISIONS

First Law of Thermodynamics

TREATMENT OF THE TURNING POINT IN ADK-THEORY INCLUDING NON-ZERO INITIAL MOMENTA

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer

PHYS 1101 Practice problem set 12, Chapter 32: 21, 22, 24, 57, 61, 83 Chapter 33: 7, 12, 32, 38, 44, 49, 76

Calculating the Quasi-static Pressures of Confined Explosions Considering Chemical Reactions under the Constant Entropy Assumption

Snce h( q^; q) = hq ~ and h( p^ ; p) = hp, one can wrte ~ h hq hp = hq ~hp ~ (7) the uncertanty relaton for an arbtrary state. The states that mnmze t

BAR & TRUSS FINITE ELEMENT. Direct Stiffness Method

Physics 2A Chapter 3 HW Solutions

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

Translational Equations of Motion for A Body Translational equations of motion (centroidal) for a body are m r = f.

12. The Hamilton-Jacobi Equation Michael Fowler

Solution of Linear System of Equations and Matrix Inversion Gauss Seidel Iteration Method

Population element: 1 2 N. 1.1 Sampling with Replacement: Hansen-Hurwitz Estimator(HH)

Math 261 Exercise sheet 2

One Dimensional Axial Deformations

STATISTICAL MECHANICS

ORDINARY DIFFERENTIAL EQUATIONS EULER S METHOD

Chapter 6. Operational Amplifier. inputs can be defined as the average of the sum of the two signals.

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015

MATH 5630: Discrete Time-Space Model Hung Phan, UMass Lowell March 1, 2018

General Tips on How to Do Well in Physics Exams. 1. Establish a good habit in keeping track of your steps. For example, when you use the equation

Numerical Heat and Mass Transfer

Introduction to Interfacial Segregation. Xiaozhe Zhang 10/02/2015

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram

EMU Physics Department

Be true to your work, your word, and your friend.

Prof. Paolo Colantonio a.a

NAME and Section No.

Absorbing Markov Chain Models to Determine Optimum Process Target Levels in Production Systems with Rework and Scrapping

: Numerical Analysis Topic 2: Solution of Nonlinear Equations Lectures 5-11:

PHYS 1443 Section 002

Probability, Statistics, and Reliability for Engineers and Scientists SIMULATION

ELECTRONICS. EE 42/100 Lecture 4: Resistive Networks and Nodal Analysis. Rev B 1/25/2012 (9:49PM) Prof. Ali M. Niknejad

PHYSICS 203-NYA-05 MECHANICS

Transcription:

ES 5 (phy 40). a) Wrte the zeroth law o thermodynamcs. b) What s thermal conductvty? c) Identyng all es, draw schematcally a P dagram o the arnot cycle. d) What s the ecency o an engne and what s the coecent o perormance o a rergerator. You wll be gong through an mportant phase change very soon. Show that the volume coecent o thermal epanson or an deal gas at constant pressure s temperature dependent and gven by b( ) where s the temperature o the gas epressed n the elvn scale. (Hnt. Use the denton o the coecent o thermal epanson and the equaton o state or an deal gas: P nr). One mole o an deal gas, wth an ntal temperature o, epands sothermally rom to (> ). a) How much work does the gas perorm n the? b) How much heat s delvered to the gas? c) Determne the change n the entropy o the gas. R 8. mol 4. You add 0g o 5 cream to 00g o 60 coee. onsderng both lquds practcally beng water, ther specc heat s 4. /g and s constant n the consdered temperature range. a) Show that the nal temperature o the mture s 55? (Ignore the cup and the atmosphere.) b) How much heat was transerred between the two lquds? c) alculate the amount o entropy produced n the.

- - a) I two systems A and B are separately n thermal equlbrum wth a thrd system, then they are n thermal equlbrum wth each other. b) he rate at whch energy lows by conducton through a slab o crosssectonal surace s proportonal to the area o the surace and the temperature gradent dt d ka d he proportonalty coecent n the above relaton s called the thermal conductvty o the materal (o the slab). c) P adabatc sothermal Q h adabatc sothermal Q c d) Both numbers reer to the rato o the harvested energy to the necessary energy delvered rom the avalable energy source. he ecency o an engne s dened as the amount o work perormed by the engne per unt energy used rom the energy source W e he coecent o perormance o a rergerator s the amount o energy removed rom the cooled space per unt work necessary to perorm the task Q OP c W Q h

- - he volume coecent o thermal epanson relates the change n temperature o a system wth the change n ts volume. By denton () d βd From the equaton o state or an deal gas, n an sobarc nr () ( ) P. We can relate the (derental) change n volume o the gas, at a constant pressure (and temperature ), n terms o a (derental) change n temperature () d nr P d. he rest s math. Solvng () or the volume coecent o thermal epanson, and substtutng equatons () and () or the volume and the change n volume, we nd the answer β( ) d P nr d d nr P d

- - a) Usng the equaton o state or an deal gas, the pressure s nversely proportonal to volume o the gas nr P he work perormed by the gas s thereore W nr mol 8. d nr mol d nr 7 ln 0 ln.7 0 b) Accordng to the rst law o thermodynamcs, the change n the nternal energy s equal to the heat delvered to the system mnus work done by the system. Snce or an deal gas, the nternal energy depends only on temperature, ts value does not change durng the. It means that the heat delvered to the gas s equal to the work done by the gas Q U + W n v + W 0 +.7 0 c) Accordng to the denton o entropy one has to consder a quasstatc leadng rom the ntal to the nal (equlbrum) state. In ths problem, the consdered s quas-statc. We can determne the change n entropy drectly n the actual Q.7 0 7 0

- 4 - a) Snce the specc heat o each part (cream and coee) s constant n the, the ntegraton o heat delvered to each system s smple ) Q mcd mc (, ), As suggested n the tet o the problem, we can assume that durng the mng, heat was transerred between the cream () and coee only. (he total heat delvered to the mture s zero.) ) m c ( ) + m c ( ) 0,, Solvng or the nal temperature we obtan mc, + mc, m, + m, 0g 5 + 00g 60 55 m c + m c m + m 0g + 00g b) From equaton (), we can nd the heat Q, transerred rom the coee to the cream, ether calculatng the heat delvered to the cream Q Q mc(, ) 0g 4. ( 55 5 ) 4.k g (or the heat released by the coee Q Q mc(, ) 00g 4. ( 55 60 ) 4.k ) g c) From the denton o entropy, each system changes ts entropy durng the transer o heat ds, c md c he change n the entropy o the Unverse s thereore S c m ln c m ln + + 4. 0g ln g, ( 55 + 7) ( 5+ 7), m, m + 4. 00g ln g ln, m, ( 55 + 7). ( 60 + 7)