THERMODYNAMICS AND STATISTICAL PHYSICS 239We then obtain, from (S.4.105.2),The cross derivatives of (S.4.105.3) are equal soThe heat capacity at constant magnetic field is given byfrom which we obtainBy again exchanging the order of differentiation in (S.4.105.6) and using
the result found in (S.4.105.4), we have
Replacing M by in (S.4.105.7) yields the desired
b) For an adiabatic process, the entropy S is constant. Writing
we compose the differential
and by (S.4.105.4) and (S.4.105.5),