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Phase Equilibria

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Phase equilibria from phase diagrams. Relation between phase and T, P. T, P and Gibbs energy ... between gas and liquid phase critical opalescence ... – PowerPoint PPT presentation

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Title: Phase Equilibria


1
Phase Equilibria
  • Lecture Note 14
  • Physical Chemistry II, 2008
  • KAIST

2
Phase equilibria from phase diagrams
  • Relation between phase and T, P
  • T, P and Gibbs energy
  • Given T,P, phase with lower G stable
  • Pressure dependence of transition T
  • Chemical potential
  • Component flows from high potential to low
    potential
  • Statistical thermodynamics expression of the
    chemical potential (in terms of q)

3
23-1. Phase diagram solid-liquid-gas behavior
A point of given T, P 1) within a region one
phase, 2) on a line two phase (vapor pressure
or melting point) 3) On a point two or more
phases (triple point or critical point)
4
At triple points, solid-liquid-gas coexist
Vapor pressure pressure of the gas phase in
equilibrium with solid and/or liquid phases (?)
5
For a pure substance, f 3 p f degree of
freedom, p number of phases
Coexistence curve gives pressure dependence of
melting and boiling points
6
A piece of cake?
7
At P lower than the triple point P, solid
sublimes.At P, T higher than the critical point,
liquid and gas are not distinguishable. (fluid)
8
Water is special, but not unique
9
Orthobaric densities and molar entropy of
vaporization (beyond the critical T, liquid and
gas become the same phase no more boiling)
Near critical point, large fluctuation of density
due to rapid change between gas and liquid phase
critical opalescence Path can be devised to go
from gas to liquid avoiding any phase transition
10
No critical points for liquid-solidMany
different solid phases possible
(I) Is normal ice, other ice phases are stable at
higher pressures
11
23-2. Gibbs energy and phase diagram are related
H(solid) lt H(liquid) lt H(gas) GH-TS, at higher
T, S dominant
12
Plot corresponds to a vertical path at a given T
near triple point
13
The phase with a lower molar G is a stable phase
14
23-3. Chemical potentials are equal for
coexisting phases of a pure substance
15
Transition proceeds in the direction of
dGlt0 sign of (µg µl) and dng opposite
16
Chemical potential is an intensive quantity
17
Clapeyron equation slope of the two-phase curve
18
Use of the Clapeyron equation
19
Melting point of ice decreases with increasing
pressure
20
Neglecting molar volume of liquid and applying
ideal gas assumption,
Vapor pressure P2 can be obtained given all
others in (23.13)
21
Use of Clausius-Claperyon equation
22
Using
Nonlinear part present
Slope is the average value in that interval
Vapor pressure of solid ammonia 146 K 195 K
23
H state function
24
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25
AU-TS
N to n using
26
Chemical potential from a partition function for
an ideal gas
Relative to the standard state
27
Use of
28
On the choice of 0 for the chemical potential
  • Set the ground state energy of the electronic
    state as energy 0
  • Then
  • For a diatomic molecule with the usual molar and
    standard state condition
  • Factor
    omitted from q of (18.39)

29
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