I'm not sure I see your point lightgrav. I'll rewrite hola's work with more precision. Asume an object of mass m at rest at t_0 = 0 acted on my a constant force F, from which results an acceleration a. Then, after a time t', the object has traveled a distance d, and the rate at which work as been done by force (the power) for that period is P = Fd/t' = mad/t'. But since the force is constant, the equation of position of the object is x(t) = 0.5at², for which we know a solution to be d = 0.5at'² <==> [itex]t' = \sqrt{2d/a}[/itex]. Hence we can rewrite the power for that particular trajectory of the object as
[tex]P = \frac{mad}{\sqrt{2d/a}} = \frac{ma\sqrt{ad}}{\sqrt{2}} = \sqrt{\frac{d}{2}}ma^{3/2}[/tex]