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· The behavior of the Gibbs function with temperature may
be understood from the thermodynamic relationship: dg = - s dT + v dp ·
The
slope of the g(T) curve, (dg/dT)p = -s and, since s is positive, the slope
is negative. The entropy
also increases as T increases. ·
The
curvature of the g(T) curve may be related to the specific
heat capacity
of the material: (d2g/dT2)p
= - (ds/dT)p
= - (cp / T). The specific heat is a positive quantity and, hence,
the curvature is negative and decreases as T increases. ·
For
iron,
the specific heat of the bcc phase (a,d zones)
is larger than the specific heat of the fcc phase (g) and, hence, the g(T) curve for bcc
iron has more
curvature than that of fcc
iron at any given temperature. · The greater
curvature of the bcc curve causes it to have two intersections with the fcc
curve between room temperature and the melting point. The lowest Gibbs function
gives the equilibrium phase and so two phase changes occur as T increases
from room temperature.
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