Re-use of this resource is governed by a Creative Commons
Attribution-
NonCommercial-ShareAlike 4.0 International
https://creativecommons.org/licenses/by-nc-sa/4.0/
Gibbs Free Energy and
Phases
Gibbs Free Energy and
Phases
For a brief reminder about free energy
curves for a single phase, click start
To go straight to an explanation about
a two phase system, click skip
The variation of G with T for a single
phase has the general form:
The free energy decreases with increasing T
The free energy is in fact governed by the master equation G = H - TS
G =
H
- TS
The intercept on the vertical axis is the enthalpy, H
(at 0K), which is equivalent to G (at 0K).
The gradient is the negative
of the entropy, −S. The entropy is always positive, therefore
the gradient is always negative, and becomes increasingly negative as
T increases.
The variation of G with T for a two
phase system
For example, in shape memory alloys the two free energy
curves represent the austenitic and martensitic phases
Above Te the austenitic phase has a lower free
energy therefore it is more stable
Plot first curve
Plot second curve
Generally the two different phases have different
enthalpies and entropies. This leads to an intersection of the curves
Where the curves intersect the phases have the same
free energy and are in equilibrium (both phases are equally stable)
The temperature at which this occurs is the equilibrium
temperature, Te
Below Te the martensitic phase has
a lower free energy therefore it is favoured thermodynamically.