In my previous question Enthalpy of a Van der Waals gas, I got the expression of the enthalpy generalised, but I am still having issues finishing it since it might have some quite hard calculus...
For my Van der Waals gas with constant temperature we got to the following expression by the already mentioned question: $$dH=TdS+VdP=T(-\frac{\partial P}{\partial V}dP)+VdP=(V-\frac{\partial P}{\partial V}T)dP$$ while the Van der Waals equation is $$(P+\frac{an^2}{V^2})(V-nb)=P(V-nb)+\frac{an^2}{V}-\frac{an^3 b}{V^2}=nRT$$ and solving for $P$ to get the $\frac{\partial P}{\partial V}$ we get $$P=\frac{nRT-\frac{an^2 V-an^3 b}{V^2}}{V-nb}=\frac{nRTV^2-an^3 V-an^3 b}{(V-nb)V^2}$$ and so we can find the partial derivative term $$\frac{\partial P}{\partial V}=\frac{(2nRTV-ab^3)(V^2 (V-nb))-(nRTV^2-an^3 V-an^3 b)(3V^2-2nbV)}{(V^3-nbV^2)^2}$$ which seems already extremely large, am I on the right path or is there an easier way?