where Eq. (1.15.6) was introduced on the right. As was emphasized in connection with the third law, any adiabatic change in deformation coordinates results in a change of temperature unless phase transitions are involved. Equations (1.15.9) and (1.15.10) show the extent of such a change in terms of quantities that are experimentally accessible.
The variation of heat capacity with pressure1 or volume at constant composition is given by , whence
(1.15.11)
and similarly ...
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