10.3 Specific Heat Equations
With the help of Maxwell relations, the fundamental equations
dQ = Cv dT + l dv (10.32)
and
dQ = Cp dT + l′ dp (10.33)
can be put in a more useful form.
From Eq. 10.32 putting dT = 0,
By Maxwell's relation II,
Hence, Eq. 10.32 takes the following form
For a perfect gas,
Hence,
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