(a) The given relation is $p = \frac{\alpha T^{2}}{V}\ \ \ \therefore\ \ V = \frac{\alpha T^{2}}{P}$
As pressure is kept constant, $dV = \left( \frac{2\alpha T}{P} \right)dT$
$W = \int_{}^{}{p\ dV = \int_{T_{0}}^{2T_{0}}{p\left( \frac{2\alpha T}{p} \right)dT}}$
$= 2\alpha\left\lbrack \frac{T^{2}}{2} \right\rbrack_{T_{0}}^{2T_{0}} = 3\alpha T_{0}^{2}$