If
\(h\) is the mass specific enthalpy,
\(s\) is the mass specific entropy,
\(P\) is the pressure,
\(T\) is the temperature,
\(C_V\) is the mass specific heat at constant volume,
\(C_P\) is the mass specific heat at constant pressure,
\(\beta\) is the coefficient of thermal expansion,
\(v\) is the mass specific volume,
\(\kappa\) is the isothermal compressibility,
then the partial derivative \(\left( \frac{\partial h}{\partial s} \right)_P\) is