Answer
$\dfrac{RT}{V}, \dfrac{nT}{V},\dfrac{nR}{V}, -\dfrac{nRT}{V^2}$
Work Step by Step
Given: $P=\dfrac{nRT}{V}$
Now, $\dfrac{\partial P}{\partial n}=\dfrac{\partial }{\partial n} [\dfrac{nRT}{V}]=\dfrac{RT}{V}$
and
$\dfrac{\partial P}{\partial R}=\dfrac{\partial }{\partial R} [\dfrac{nRT}{V}]=\dfrac{nT}{V}$
and
$\dfrac{\partial P}{\partial T}=\dfrac{\partial }{\partial T} [\dfrac{nRT}{V}]=\dfrac{nR}{V}$
and $\dfrac{\partial P}{\partial V}=\dfrac{\partial }{\partial V} [\dfrac{nRT}{V}]=-\dfrac{nRT}{V^2}$
Hence, $\dfrac{RT}{V}, \dfrac{nT}{V},\dfrac{nR}{V}, -\dfrac{nRT}{V^2}$
