P = constant
$ \therefore $ Work done in time t.
$ \, \, \, \, \, \, \, \, \, \, \, \, \, \, W = Pt $
From work-energy theorem, net work done is change in kinetic energy. Therefore,
$\frac{1}{2} mv^2=pt $
or $\, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, v \propto t^{1/2}$
Integrating, we get $ s \propto t^{3/2}$