Let s = f(T, p)

As per Maxwell relation
\(\left(\cfrac{\partial s}{\partial p}\right)_T\) = - \(\left(\cfrac{\partial v}{\partial T}\right)_p\)
Substituting this in the above equation, we get
ds = \(\left(\cfrac{\partial s}{\partial T}\right)_p\) dT - \(\left(\cfrac{\partial v}{\partial T}\right)_p\) . dp ....(i)
The enthalpy is given by
dh = cpdT = Tds + vdp
Dividing by dT at constant pressure
\(\left(\cfrac{\partial h}{\partial T}\right)_p\) = cp = T \(\left(\cfrac{\partial s}{\partial T}\right)_p\) + 0
(as dp = 0 when pressure is constant)
Now substituting this in eqn. (i), we get

Substituting this in eqn. (ii), we get
ds = cp \(\cfrac{dT}T\) - βvdp