If ∆H is the enthalpy change
accompanying a reaction (system) the
enthalpy change of the surroundings is -∆H.
With
∆Ssurr = - ∆H
T
(4.37)
Substituting above into Eq. (4.36),
∆Stotal = ∆S - ∆H
T
(4.38)
Thus ∆Stotal is expressed in terms of the
properties of the system only. Rearranging
T ∆Stotal = ∆H - T ∆S (4.39)
Substituting in Eq. (4.35)
∆G = - T ∆Stotal (4.40)
For a spontaneous reaction Stotal > 0 and
hence, ∆G < 0. At constant temperature and
pressure Gibbs energy of the system decreases
in a spontaneous process.
The second law leads to the conditions
of spontaneity which are summarised here.
i. ∆Stotal > 0 and ∆G < 0, the process is
spontaneous.
ii. ∆Stotal < 0 and ∆G > 0, the process is
nonspontaneous.
iii. ∆Stotal = 0 and ∆G = 0, the process is at
equilibrium.
4.11.7 Sponaneity and ∆H or ∆S
From ∆G = ∆H - T ∆S (at constant T
and P).
The temperature term determines relative
contributions of ∆H and ∆S to ∆G.
- ∆H and ∆S are both negative then ∆G
will be negative only when ∆H is more
negative than T∆S. This is possible at low
temperatures only. - ∆H amd ∆S both positive ∆G will be
negative only if T∆S > ∆H. This is possible
only at high temperatures.
3. For ∆H negative and ∆S is positive it
follows that ∆G is negative regardless of
temperature.
4. For ∆H positive and ∆S is negative then
∆G is positive regardless of temperature.
Such reactions are nonspontaneous at all
temperatures.
4.11.8 Temperature of equilibrium
For equilibrium
∆G = ∆H - T∆S gives
∴ T =
∆H
∆S^ (4.41)
T is the temperature at which the change
over from spontaneous to nonspontaneous
behavior occurs. ∆H and ∆S are assumed to
be independent of temperature in Eq. (4.41).
Introducing of temperature dependence of ∆H
or ∆S would not cause significant error for
the moderate temperature range.
4.11.9 Gibbs function and equilibrium
constant : Gibbs energy change for a chemical
reaction is given by
∆G = ∆G^0 + RT ln Q (4.42)
where ∆G^0 is standard Gibbs energy change
that is, the Gibbs energy change when the
reactants and products in a reaction are in their
standard states. Q is called reaction quotient Q
is analogus to that of the equilibrium constant.
and involves nonequilibrium concentrations or
partial pressures in case of gaseous reaction.
Consider
aA + bB cC + dD
∆G = ∆G^0 + RT ln Qc
= ∆G^0 + RT ln
[C]c[D]d
[A]a [B]b^ (4.43)
or ∆G = ∆G^0 + RT ln Qp
= ∆G^0 + RT ln
PCc×PDd
PAa× PBb^ (4.44)