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.