Similar documents
3.012 PS 7 Thermo solutions Issued: Fall 2003 Graded problems due:

The Second Law of Thermodynamics (Chapter 4)

Phase Equilibria in a One-Component System I

Problem Set 10 Solutions

CHAPTER 4 Physical Transformations of Pure Substances.

Exam 3 Solutions. ClO g. At 200 K and a total pressure of 1.0 bar, the partial pressure ratio for the chlorine-containing compounds is p ClO2

Phase Diagrams. NC State University

Courtesy of Marc De Graef. Used with permission.

3.012 PS Issued: Fall 2003 Graded problems due:

Chapter 8 Phase Diagram, Relative Stability of Solid, Liquid, and Gas

For an incompressible β and k = 0, Equations (6.28) and (6.29) become:

Lecture 4-6 Equilibrium

Thermodynamic condition for equilibrium between two phases a and b is G a = G b, so that during an equilibrium phase change, G ab = G a G b = 0.

Vapor Pressure of Liquids Equilibria and Thermodynamics

B. Correct! Good work. F = C P + 2 = = 2 degrees of freedom. Good try. Hint: Think about the meaning of components and phases.

ln( P vap(s) / torr) = T / K ln( P vap(l) / torr) = T / K

Physics 408 Final Exam

3.012 PS 6 THERMODYANMICS SOLUTIONS Issued: Fall 2005 Due:

Chapter 7 PHASE EQUILIBRIUM IN A ONE-COMPONENT SYSTEM

Lecture Notes 2: Physical Equilibria Phase Diagrams

MATSCI 204 Thermodynamics and Phase Equilibria Winter Chapter #4 Practice problems

Application of Thermodynamics in Phase Diagrams. Today s Topics

CHEM-UA 652: Thermodynamics and Kinetics

X B1 X B Quiz Fall points total. 1. Thermodynamics. (50 points)

Last Name or Student ID

Chap. 3. The Second Law. Law of Spontaneity, world gets more random

Clausius Clapeyron Equation

Chemistry 360 Spring 2017 Dr. Jean M. Standard April 19, Exam points

MS212 Thermodynamics of Materials ( 소재열역학의이해 ) Lecture Note: Chapter 7

Lecture Notes 1: Physical Equilibria Vapor Pressure

CHM 112 Chapter 16 Thermodynamics Study Guide

Practice Midterm Exam 1 March, 2005

ESS 312 Geochemistry Lab # 2

At this point, we've developed the tools and basic concepts necessary to apply

A 3 Vapor pressure of volatile liquids

Chem 75 February, 2017 Practice Exam 2

WEEK 6. Multiphase systems

Lecture Phase transformations. Fys2160,

The Gibbs Phase Rule F = 2 + C - P

Sect The Slope-Intercept Form

NENG 301 Week 8 Unary Heterogeneous Systems (DeHoff, Chap. 7, Chap )

P(N,V,T) = NRT V. = P(N,V,T) dv

Basic Thermodynamics Module 1

Ch. 19 Entropy and Free Energy: Spontaneous Change

UNIVERSITY OF SOUTHAMPTON

Statistical Thermodynamics. Lecture 8: Theory of Chemical Equilibria(I)

Problem set: Constructing metamorphic phase diagrams using phase equilibria and the Clausius-Clapeyron equation

Phase Diagrams: Conditions for Equilibrium (CfE)

Chapter 10 Lecture Notes: Thermodynamics

Exam 3, Chemistry 481, 8 December 2017

Chapter 11 Solution Thermodynamics: Theory

1. Heterogeneous Systems and Chemical Equilibrium

Thermodynamics of solids 5. Unary systems. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Lecture 17. Conditions of Equilibrium

10, Physical Chemistry- III (Classical Thermodynamics, Non-Equilibrium Thermodynamics, Surface chemistry, Fast kinetics)

Chemical Equilibria. Chapter Extent of Reaction

Practice Midterm Exam 1 March, 2011

MATSCI 204 Thermodynamics and Phase Equilibria Winter Chapter #5 Practice problems

Phase Change (State Change): A change in physical form but not the chemical identity of a substance.

Gibb s Free Energy. This value represents the maximum amount of useful work (non PV-work) that can be obtained by a system.

Solutions to Exercises: Chapter 7

UNIVERSITY OF SOUTHAMPTON

General Chemistry I Concepts

Introduction to Chemical Thermodynamics. (10 Lectures) Michaelmas Term

Classical Thermodynamics. Dr. Massimo Mella School of Chemistry Cardiff University

Chapter 6. Phase transitions. 6.1 Concept of phase

Geology 222 Problem Geotherm

Physical Biochemistry. Kwan Hee Lee, Ph.D. Handong Global University

Phase Equilibria I. Introduction. Heat and Phase Changes

CHEMISTRY 443, Fall, 2014 (14F) Section Number: 10 Examination 2, November 5, 2014

Introduction to Chemical Thermodynamics. D. E. Manolopoulos First Year (13 Lectures) Michaelmas Term

Chapter 6 Thermodynamic Properties of Fluids

Chapter 19 Chemical Thermodynamics

Chemical Potential. Combining the First and Second Laws for a closed system, Considering (extensive properties)

Phase Equilibrium: Preliminaries

12. Heat of melting and evaporation of water

Chemistry 103 Spring Announcements 1. Ch. 16 OWL homework is active. 2. Next midterm exam on May 17 or 19.

Physics 360 Review 3

S A 0.6. Units of J/mol K S U /N

The Clausius-Clapeyron Equation

THERMODYNAMICS. Thermodynamics: (From Greek: thermos = heat and dynamic = change)


Chapter 12 PROPERTY RELATIONS. Department of Mechanical Engineering

COURSE 3.20: THERMODYNAMICS OF MATERIALS. FINAL EXAM, Dec 18, 2000

So far in talking about thermodynamics, we ve mostly limited ourselves to

THIS LAB IS CHAOS! 2. In liquids or gases? Explain.

Chapter 5. On-line resource

General Physical Chemistry I

Free energy dependence along the coexistence curve

Physical transformations of pure substances Boiling, freezing, and the conversion of graphite to diamond examples of phase transitions changes of

Phase Equilibria. G 1 =G 2, the phases are in equilibrium, e.g.

Chapter 11 Spontaneous Change and Equilibrium

3.012 PS Issued: Fall 2004 Due: pm

Entropy and Standard Free Energy:

AP CHEMISTRY 2007 SCORING GUIDELINES (Form B)

Chemistry and the material world Unit 4, Lecture 4 Matthias Lein


Thermodynamics of Solutions Partial Molar Properties

Geological Sciences 4550: Geochemistry

Chemistry 123: Physical and Organic Chemistry Topic 2: Thermochemistry

Transcription:

3.012 PS 7 3.012 Issued: 11.05.04 Fall 2004 Due: 11.12.04 THERMODYNAMICS 1. single-component phase diagrams. Shown below is a hypothetical phase diagram for a single-component closed system. Answer the following questions about this diagram: a. Apply the phase rule to each of the marked locations 1, 2, and 3, and determine whether those points on the diagram correctly mark stable equilibria. b. Is the molar volume change of transformation ΔV α gas for the transformation of solid α to the gas phase positive or negative? c. For the fixed pressure P, draw a qualitative plot of the Gibbs free energy of this material for each phase as a function of temperature over the range shown. T 2 liquid 3 T T 3 liquid 1 gas α, β, gas coexistence T 2 gas β (solid) β (solid) α (solid) T 1 α (solid) P P P (a) The Gibbs phase rule for single-component phase diagrams is: D + P = C + 2 Since the number of components C = 1, we have: D + P = 3 The number of degrees of freedom (D) added to the number of phases present (P) must be = 3 for a stable equilibrium. 3.012 PS 5 1 of 5 11/20/04

Examining the marked points on the diagram: (1) a 3-phase field- a region with two degrees of freedom (temperature and pressure can be varied independently within the field and the same equilibrium is maintained). Plugging into the phase rule: D + P = 2 + 3 = 5 thus this is definitely not a stable equilibrium. (2) Point 2 marks the intersection of three single-phase regions: it is a triple point where liquid, gas, and the solid phase b are in equilibrium at a single temperature and pressure: D + P = 0 + 3 = 3 this phase equilibrium is stable. (3) Point 3 marks liquid-solid b equilibrium, with one degree of freedom- if the temperature is changed, the pressure required to maintain the two-phase equilibrium is predetermined. Likewise, if the pressure is changed, the temperature is predetermined: D + P = 1 + 2 = 3 this is a stable phase equilibrium. (b) The Clausius-Clapeyron equation relates the slope of the pressure vs. temperature phase boundary to the enthalpy change, temperature, and volume change at a phase transition: dp dt equilibrium= ΔH trans T trans ΔV trans The enthalpy change of first-order phase transitions must be positive (remember, the entropy is always increasing with temperature for stability, and at a phase transition ΔH trans = T trans ΔS trans ; absolute temperature must be positive therefore enthalpy changes at the transition must be positive). Since the enthalpy change and Ttrans are positive, the sign on the phase transition volume change is the same as the sign of the slope of the P vs. T phase boundary. Looking at the phase diagram, we see that along the α/gas phase boundary, the pressure increases as temperature increasesdp/dt is positive. Thus, the volume change on transformation of solid α to gas is positive. (c). Using the information from the phase diagram, we can construct the following qualitative diagram: 3.012 PS 5 2 of 5 11/20/04

G α G G β G liquid G gas 0 T 1 T 2 T 3 the diagram must exhibit: (1) negative slope and curvature for each free energy curve (requirements for stability), and (2) free energy curves of phases cross at points of two-phase equilibrium; the stable phase at each temperature must exhibit the lowest free energy. T 2. Free energy behavior of solutions [DJI1][DJI2]. Shown on the following page is a diagram of free energies for a two-component A-B system at a fixed temperature of 500 K and fixed pressure of 1 atm. This system exists in 3 different phases- liquid, and two solid phases α and β. Two copies of the diagram are provided to sketch on. Use this diagram to answer the questions below: a. Using the top copy of the free energy diagram, draw common tangents that identify composition regions of two-phase equilibrium at this temperature and pressure. Draw a composition bar at the bottom of the diagram as in lecture, and denote which phases are present as a function of composition. b. At the composition marked X on the diagram, the system is in equilibrium with 2 phases in coexistence. i. What two phases are present? ii. What are the phase fractions, in terms of parameters given on the diagram? iii. What is the composition of each phase that is present? c. On the lower copy of the phase diagram, draw constructions or mark points as necessary to identify the following quantities for a system with composition X : i. The chemical potential of A in each phase, and B in each phase present. 3.012 PS 5 3 of 5 11/20/04

ii. The standard state chemical potential of A and B in each phase present. (a) See diagram below. (b) (i) Liquid and solid α. (ii) To identify the relevant compositions, points X α B and X L B are marked on the top free energy diagram below. Applying the lever rule: ( f α = X L B X' ) X L α B X B f L = ( ) X' X α ( B ) X L α ( B X B ) (iii) The compositions are given by the points where the common tangent touches each free energy curve: Liquid has composition X B L Solid a has composition X B α (c) See the diagram below. We must extrapolate the free energy curves to get the intercepts with the X B = 0 and X B = 1 axes for the standard state chemical potentials. 3.012 PS 5 4 of 5 11/20/04

Common tangents G X B α X B L G α G L G β X 0 X 1 B Compositions: α L + α L L + β β µ A,o L µ B,o L µ B,o α G µ A,o α G α G L G β µ A L = µ A α X 0 X 1 B µ B L = µ B α 3.012 PS 5 5 of 5 11/20/04