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Derive the following relations :

(i) \(\left(\cfrac{\partial T}{\partial p}\right)_s\) = \(\cfrac{Tv\beta}{c_p}\)

(ii) \(\left(\cfrac{\partial T}{\partial v}\right)_s\) = - \(\cfrac{T\beta}{c_vK}\) 

where β = Co-efficient of cubical expansion, and 

K = Isothermal compressibility.

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(i) Using the Maxwell relation we have

(ii) Using the Maxwell relation

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