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Blundell Thermal Physics
· Problem 18.2
The third law
Physics — Statistical Mechanics · gibbs-enthalpy-third-law
Problem
Recall from eqn 16.26 that
H
=
G
−
T
(
∂
G
∂
T
)
p
.
(18.9)
H = G - T\left(\frac{\partial G}{\partial T}\right)_p. \tag{18.9}
H
=
G
−
T
(
∂
T
∂
G
)
p
.
(
18.9
)
Hence show that
Δ
G
−
Δ
H
=
T
(
∂
Δ
G
∂
T
)
p
,
(18.10)
\Delta G - \Delta H = T\left(\frac{\partial \Delta G}{\partial T}\right)_p, \tag{18.10}
Δ
G
−
Δ
H
=
T
(
∂
T
∂
Δ
G
)
p
,
(
18.10
)
and explain what happens to these terms as the temperature
T
→
0
T \to 0
T
→
0
.
Related theory
Enthalpy And Enthalpy Of Reaction
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