Title: Animated ABC Blocks
1Chapter 5 Phase Equilibria
- Clapeyron equation
- Clausius-Claypeyron equation
- Phase rule
2? Clayperon equation
at equilibrium ?G 0
3From
(At equilibrium)
Slope of the plot between P and T
4?S/ ?V
?Vm
?Sm
gt 0 gt 0 gt 0
gt 0 gt 0 gt 0
gt 0 gt 0 gt 0
?S/ ?V lt 0
In case of H2O Vm,s gt Vm,l ?Vm lt 0
hence
5H2O
6From ?S At phase transition ?S tr We
obtain Clapeyron equation
7Example 5.1 What is the boiling temperature for
water at 2000 meter high above the sea level.
Given p p0e-gMh/RT, the barometric formular,
where g 9.81 ms-2 , M molar mass, hheight, and
T298 K and the heat of vaporization of water is
40.7 kJ/mol
?P p - p0 p0 (e-gMh/RT -1) gMh/RT
(9.81ms-2)(18x10-3 kg/mol)(2000 m)
(8.314 J/molK)(298K) 0.0152 ? ?P
(1 atm)(e-0.0152 -1) -0.0151 atm
-1528 Pa
8?V Vg Vl Vg nRT/P
(1mol)(0.082 L atm/K mol)(373K)/0.9849 atm
31.05 L/mol 31.05 x 10-3 m3/mol From Clapeyron
equation
9Clausius Clapeyron
From Clapeyron equation
If the phase transition is from l to g
then ?Htr ?Hvap
?V Vm,g - Vm,l Vm,g Using ideal
gas equation ?V RT/P
10Substitute in Clapeyron equation,
Clausius Clapeyron equation
11Example 4.2 The boiling point of benzene is
80.1C at 1 atm. Estimate the vapor pressure of
benzene at 25C
From
Here P1 1 atm and T1 80.1C
353.3 K
P2 ? and T2 25C
298 K
12Using Troutons rule
?Svap ?Hvap/Tb 88 J/Kmol
?Hvap Tb ?Svap (353.3 K)( 88
J/Kmol) ln(P2/1atm) (353.3 K)( 88
J/Kmol)(-55.1K) (8.314 J/Kmol) (353.3 K)(298
K) -1.597 P2
(1atm)e-1.597 0.141 atm
13Phase rule
- Number of free variables needed to describe the
system is called degree of freedom (F) - For single component and single phase system,
only 2 variables, P and T, are required and it
has 2 degree of freedom (F 2) - A(T,P)
- For C components, we only need C 1 variables.
- Since x1 x2 ..xc 1
- For C components and single phase,
- F (C-1) 2
- A(T, P, x1, x2 ,.,xc-1)
- For C components and P phases, there must be
- P(C-1) variables
14- There establishes equilibrium between phases,
C components
For P phases
C equations
.
For 1 component and 2 phases µa µß ?P
(?S/?V) ?T Number of free variables is 1 2
(P-1) Number of free variables is reduced by
(P-1)
15For C components and P phases, there are C
equations For each components, number of free
variables is reduced by (P-1) Overall
reduction of variables is C(P-1)
F P(C-1) 2 - C(P-1)
PC - P 2 - PC C
F C - P 2
phase rule
16 phase Component F 1 1 2 T, P
2 1 1 3 1 0 1 2 3 T, P,
x 2 2 2
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