c05 JWBS043-Rogers September 13, 2010 11:25 Printer Name: Yet to Come
74 ENTROPY AND THE SECOND LAW
but this is not the case. There is more to think about in a chemical or physical change
than just minimization ofUorH. There is the question of order and disorder of the
reactant state and the product state.
5.1.3 Disorder
When we look at a chemical reaction
A→B
or an analogous physical change
A(l)→ A(g)
we must look at the driving force that produces the change. Part of that force comes
from the tendency to seek a minimum (water flows downhill), but part of it comes
from the universal tendency of thermodynamic systems to seek maximum disorder.
A familiar example is vaporization of a liquid such as water.
The liquid state, though not perfectly ordered, is held together by strong inter-
molecular forces. These are the very forces that we say are nonexistent or negligible
in the vapor state. The entropy change for many liquids is about 88 J K−^1 mol−^1 ,a
rule known as Trouton’s rule, that has been verified many times over for liquids as
diverse as liquid Cl 2 , HCl, chloroform, and then-alkanes. Liquids that deviate from
this rule do so, not because of any failure of the entropy concept for vaporization, but
because of abnormal forces in the liquid state. An example is water, which deviates
a little due to hydrogen bonding, and hydrogen fluoride HF, which deviates a lot.
5.2 ENTROPY CHANGES
In general, the entropy change for any change of state, including melting and change in
crystalline form in the solid state, is given by the enthalpy changeandthe temperature
appropriate to the change ortransitionconsidered:
S=
Htrans
Ttrans
5.2.1 Heating
The entropy of heating of an ideal gas is positive because thermal agitation makes
the high-temperature state more disordered than the low-temperature state. From the
expression for molar heat capacity, one has
Cp=
(
∂H
∂T
)
p