(c) From work-energy theorem
$\mathrm{\Delta}\ KE\ = W_{net}$
or $K_{f} - K_{i} = \int_{}^{}{Pd}$
or $\frac{1}{2}mv^{2} = \int_{0}^{2}{\left( \frac{3}{2}t^{2} \right)dt}$
$v^{2} = \left\lbrack \frac{t^{3}}{2} \right\rbrack_{0}^{2}$
$v = 2\ ms^{- 1}$