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1. Science of Thermodynamics

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Title: 1. Science of Thermodynamics


1
1. Science of Thermodynamics
  • Concerned with knowing the physical state of a
    system at equilibrium. A concise (mathematical)
    description of the systems state at different
    conditions allows us to calculate
  • heat and work effects associated with a process
  • the maximum work obtained or minimum work
    required for such a transformation
  • whether a process can occur spontaneously
  • In CHEM 244, thermodynamics was used to derive
    relationships amongst variables (P,T)that define
    a system at equilibrium.
  • Heat engines, refrigeration cycles, steam power
    plants
  • Dealt only with closed systems of constant
    composition (usually 1-component systems such as
    H2O)

2
CHEE 311 - Thermodynamics of Mixtures
  • Thermodynamics II is concerned with the
    properties of mixtures
  • 1. Quantifying phase equilibrium behaviour
  • At a given pressure and temperature, how many
    phases exist in a system?
  • What is the composition of each phase?
  • What are the thermodynamic properties
    (U,S,Cp,Vm,) of each phase and the system as a
    whole?
  • 2. Describing systems that undergo chemical
    reactions
  • Under specified conditions, to what extent does a
    reaction take place?
  • What is the equilibrium composition of the
    system?
  • How much heat is evolved/absorbed by the reaction
    and the mixing of reactants?

3
Thermodynamic Systems
  • The first step in all problems in thermodynamics
    is to define a system, either a body or a defined
    region of space.
  • Types of Systems
  • Isolated no transfer of energy or matter across
    the system boundaries
  • Closed possible energy exchange with the
    environment but no transfer of matter
  • Open exchange of energy and matter with the
    environment
  • Phase part of a system that is spatially
    uniform in its properties (density,
    composition,...)

4
Thermodynamic Properties
  • Concerned with macroscopic properties of a body,
    not atomic properties
  • Volume, surface tension, viscosity, etc
  • Divided into two classes
  • Intensive Properties (density, pressure,)
  • specified at each point in the system
  • spatially uniform at equilibrium
  • Usually, specifying any 2 intensive variables
    defines the values of all other intensive
    variables
  • Ij f(I1, I2) (j3,4,5,,n)
  • This holds for mixtures as well, but composition
    must also be defined
  • Ij f(I1, I2, x1,x2,,xm-1) (j3,4,5,,n)
  • for an m-component mixture.

5
Thermodynamic Properties
  • Extensive Properties (volume, internal
    energy,...)
  • Additive properties, in that the system property
    is the sum of the values of the constituent parts
  • Usually, specifying any 2 intensive and one
    extensive (conveniently the system mass) defines
    the values of all other extensive variables
  • Ej m f(I1, I2, x1,x2,,xm-1) (j3,4,5,,n
    )
  • for an m-component mixture.
  • The quotient Ei / m (molar volume, molar Gibbs
    energy) is an intensive variable, often called a
    specific property

6
Phase Diagram for CO2
7
Ideal Mixture Behaviour
  • Intermediate-boiling Systems, including Raoults
    Law Behaviour

8
Non-Ideal Vapour-Liquid Equilibria (VLE)
  • Systems having a minimum boiling azeotrope
  • We also observe systems with a maximum boiling
    azeotrope.

9
Non-Ideal VLE, LLE and VLLE
  • Systems having partially miscible liquid phases

10
Phase Behaviour of Diethylether
11
1. Phase Rule for Intensive Variables SVNA-12.2
  • For a system of ? phases and N species, the
    degree of freedom is
  • F 2 - ? N
  • variables that must be specified to fix the
    intensive state of the system at equilibrium
  • Phase Rule Variables
  • The system is characterized by T, P and (N-1)
    mole fractions for each phase
  • Requires knowledge of 2 (N-1)? variables
  • Phase Rule Equations
  • At equilibrium ?i? ?i ? ?i ? for all
    N species
  • These relations provide (?-1)N equations
  • The difference is F 2 (N-1)? - (?-1)N
  • 2- ? N

12
VLE in Single Component Systems
  • For a two phase (p2) system of a single
    component (N1)
  • F 2- ? N
  • F 2- 2 1 1
  • Therefore, for the single component system,
    specifying either T or P fixes all intensive
    variables.

13
Correlation of Vapour Pressure Data
  • Pisat, or the vapour pressure of component i, is
    commonly represented by Antoines Equation
  • For acetonitrile (Component 1)
  • For nitromethane (Component 2)
  • These functions are the only component properties
    needed to characterize ideal VLE behaviour

14
VLE in Binary Systems
  • For a two phase (?2), binary system (N2)
  • F 2- 2 2 2
  • Therefore, for the binary case, two intensive
    variables must be specified to fix the state of
    the system.

15
VLE in Binary Systems
  • Alternately, we can specify a system pressure
    (often atmospheric) and examine VLE behaviour as
    a function of temperature and composition.

16
Calculations using Raoults Law
  • Raoults Law for ideal phase behaviour relates
    the composition of liquid and vapour phases at
    equilibrium through the component vapour
    pressure, Pisat.
  • Deriving this expression, relating the
    composition of each phase at a given P,T at
    equilibrium, will be the objective of the next
    two weeks of the course.
  • Given the appropriate information, we can apply
    Raoults Law to the solution of 5 types of
    problems
  • Dew Point Pressure and Temperature
  • Bubble Point Pressure and Temperature
  • P,T Flash

17
Dew and Bubble Point Calculations
  • Dew Point Pressure
  • Given a vapour composition at a specified
    temperature, find the composition of the liquid
    in equilibrium
  • Given T, y1, y2,... yn find P, x1, x2, ... xn
  • Dew Point Temperature
  • Given a vapour composition at a specified
    pressure, find the composition of the liquid in
    equilibrium
  • Given P, y1, y2,... yn find T, x1, x2, ... xn
  • Bubble Point Pressure
  • Given a liquid composition at a specified
    temperature, find the composition of the vapour
    in equilibrium
  • Given T, x1, x2, ... xn find P, y1, y2,... yn
  • Bubble Point Temperature
  • Given a vapour composition at a specified
    pressure, find the composition of the liquid in
    equilibrium
  • Given P, x1, x2, ... xn find T, y1, y2,... yn

18
1. Why all the theory?
  • Parts of CHEE 311 are quite abstract (and,
    admittedly, a little dry). It is therefore
    important that the applications of thermodynamic
    theory be stressed. At the end of the course,
    you will understand the fundamental underpinning
    of thermodynamics and you will have used this
    knowledge to solve engineering problems.
  • In this lecture, three areas that draw on an
    advanced knowledge of thermodynamics are
    described and demonstrated
  • A. Describing and Predicting Phase Stability
  • B. Coping with Non-Ideal Behaviour
  • C. Extending Experimental Data to Describe
    Complex Systems

19
Phase Stability
  • Thermodynamics is concerned with the state and
    properties of a system under specific conditions.
  • The stability of a given phase is of practical
    concern as conditions are sought to affect a
    change in
  • the system.
  • Under what conditions does a phase become
    unstable, resulting in a change of state?
  • What property of the system determines phase
    stability?

20
Phase Stability
  • As an example of phase stability, consider the
    solid-vapour equilibrium of a system in contact
    with a heat bath.
  • Increased volatilization raises U and S of the
    system.
  • Increased crystallization decreases U and S.
  • We will see that the equilibrium state is
    determined by a balance of order and disorder
    (U and S), such that free energy (F or G) is
    minimized.
  • The state of a system for which the free energy
    is minimized is that for which the total entropy
    (heat bath and system of interest) is maximized.

21
Stability of Polymer Solutions
  • An issue of practical importance in polymer
    production is the recovery of material from
    solution.
  • Consider a solution of 5 wt of an
    acrylonitrile-butadiene copolymer (34 AN, Mw
    250,000) in acetone.
  • We want to separate the polymer from the solvent
    using a clean process that yields a manageable
    material.
  • What means do we have for doing so?
  • How are we generating instability in the original
    solution?
  • Acetone NBR Acetone NBR

22
Vapour Pressure of Pure Acetone and Water
  • If presented with the problem of separating water
    and acetone in the mixture by distillation, what
    would you do?
  • From the vapour pressure
  • curves (vap-liq line for a
  • pure component), it is clear
  • that acetone and water
  • have different volatility.
  • Does this guarantee that
    distillation is possible?
  • What tools do you have/need for
    design purposes?

23
Pxy diagram for Acetone-Water Mixtures 25C
  • Obviously, for distillation to be effective there
    must exist conditions where a liquid and a vapour
    exist at equilibrium, and the compositions of
    these phases must differ.
  • According to the phase
  • rule, for two phases to
  • exist in the acetone-
  • water system, we have
  • __ degrees of freedom.

24
Txy diagram for Acetone-Water Mixtures 1 bar
  • If our system were fixed at atmospheric pressure,
    we would need to vary temperature - Txy diagram
    is more appropriate.

25
Coping with Non-Ideal Behaviour
  • The phase equilibrium tool you are most familiar
    with, Raoults Law, adequately describes systems
    that behave ideally. This refers to the strength
    and nature of interactions between components in
    a mixture.
  • Few systems of practical importance are
    sufficiently ideal to warrant the use of Raoults
    Law.
  • Suppose we wanted to separate by room temperature
    distillation the acetone-water mixture that we
    created in the isolation of our polymer.
  • At 25C, between what two pressures will two
    phases exist in the acetone-water system
    containing equimolar quantities of the two
    components?
  • Raoults Law Phase Diagram
  • Pmax
  • Pmin

26
Txy diagram for Acetone-Water Mixtures 3.4 bar
  • At higher pressure, the acetone-water system
    becomes increasingly non-ideal, as illustrated by
    the Txy diagram below.
  • How do we describe these systems?
  • Can we predict complications such as azeotropes?

Note the lack of experimental data above 123C -
How can we extrapolate to higher temperatures in
an accurate manner?
27
Extending Experimental Data
  • Design exercises become increasingly
  • complex as additional components are added.
  • Suppose our polymer solution was not
  • NBRacetone, but
  • NBRacetone2-butanone.
  • How does the acetone-MEK-water
  • system behave?
  • There is limited data on ternary
    systems over a wide range of
    conditions
  • A principle objective of
  • CHEE 311 is to give
  • you the tools to handle
  • non-ideal mixtures of any
  • composition through the use of models that
    generalize phase behaviour and programs that
    carry out tedious calculations.
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