Title: Introduction to Thermodynamics
1Introduction to Thermodynamics
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3U internal energy
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9Entropy
P
P / 2
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16J g-1 K-1 at 300 K
atomic number
(Craig Counterman)
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18Allotropic Transition
19Q 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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21Allotropic Transition in Pure Iron
22Mechanical 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
23entropy is a capacity property, like mass, energy
etc. Different entropies can be added S1S2S3
How does this fit with the probability picture?
24Entropy
P
w1
wvery large
P / 2
25w 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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27free 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
28o
m
B
o
m
Gibbs free energy per mole
A
Gx
A
B
x
Composition
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35Binary solution
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46Irreversible Processes Steady State
47dissipating free energy
48Process whose direction can be changed by an
infinitesimal change in external conditions is
reversible.
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50Process which dissipates energy is irreversible
to an infinitesimal change in external conditions.
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