Environmental Engineering Reference
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which, for only mechanical work and for an isothermal process concerning an ideal
gas, becomes (V related to 1 mol of gas)
dG =Vd p = R u T
p
d p
ð
Eq
:
5
:
22
Þ
In order to estimate the finite value of the free energy variation
G that a mole of an
ideal gas needs to isothermally pass from an initial pressure p 0 to a final pressure p ,we
integrate Equation (5.22)
Δ
ð
G= ð
2
p
R u T d p
p =R u Tln p
dG =G 2
G 1 =
Δ
ð
Eq
:
5
:
23
Þ
p 0
p 0
1
Considering a standard initial state as reference, p 0 being 1 bar, Equation (5.23) can be
written as
G=G 0 +R u Tln p
:
:
ð
Eq
5
24
Þ
where G is the free energy of 1 mol of ideal gas at pressure p (in bar!) and
temperature T, while G 0
is its free energy at the standard temperature and pressure
(298.15 K and 1 bar).
Considering the fact that the free energy is a function of state and given Equation
(5.24)), the change of the free energy for a general reaction (RX. 5.20) is expressed by
the Van
'
t Hoff equation:
G 0 +R u Tln p C p D
p a A p B
Δ
G=
Δ
ð
Eq
:
5
:
25
Þ
The argument of the logarithm in Equation (5.25) is formally analogous to the equi-
librium constant ( K p ) but has the same value only when the reaction has reached
equilibrium, i.e.,
G 0 +R u Tln K p =0
G 0 =
Δ
G=
Δ
) Δ
R u Tln K p
ð
Eq
:
5
:
26
Þ
Example 5.3 Calculation of equilibrium constants, K c and K p
In a container with a capacity of 5 L, 1 mol of SO 2 and 1 mol of O 2 react at 1000 K.
Once equilibrium has been reached, the amount of SO 3 in the container is 68 g
(0.85 mol). Find K c and K p .R u = 0.082 L.bar.K −1 .mol −1
Solution
The reaction observed is
2SO 2 +O 2 !
2SO 3
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