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Introduction to Thermodynamics

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Title: Introduction to Thermodynamics


1
Introduction to Thermodynamics
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U internal energy
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Entropy
P
P / 2
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(Craig Counterman)
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J g-1 K-1 at 300 K
atomic number
(Craig Counterman)
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Allotropic Transition
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Q Why is Gibbs free energy called free?
A Because it is that part of the energy which is
in principle obtainable as mechanical
work. N. K. Adam, Physical Chemistry,
Clarendon Press, Oxford (1956) page 263.
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Allotropic Transition in Pure Iron
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Mechanical Mixture
free energy of
mechanical
o
m
mixture
B
G
o
m
Gibbs free energy per mole
A
x
1-x
A
B
Concentration x of B
23
entropy is a capacity property, like mass, energy
etc. Different entropies can be added S1S2S3
How does this fit with the probability picture?
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Entropy
P
w1
wvery large
P / 2
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w is not a capacity property of the system. For
example, the chance of throwing two sixes with
dice is (1/6)2, not 1/61/6. Boltzmann realised
that we should use lnw and not w to meaure
disorder.
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free energy of
mechanical
o
m
mixture
B
G
Gibbs free energy per mole
o
m
A
?G
M
Gx
free energy
of solution
A
B
x
Composition
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o
m
B
o
m
Gibbs free energy per mole
A
Gx
A
B
x
Composition
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Binary solution
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Irreversible Processes Steady State
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dissipating free energy
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Process whose direction can be changed by an
infinitesimal change in external conditions is
reversible.
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Process which dissipates energy is irreversible
to an infinitesimal change in external conditions.
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