A particle of mass m is moving in a circular path of constant radius r such that its centripetal acceleration ac is varying with time t as a = k2rt2 The power delivered to the particle by the forces acting on it is
Here tha tangetial acceleration also exits which requires power.
Given that ac = k2rt2 and ac = v2r ∴ v2r = k2rt2
or v2 = k2rt2 or v = krt
Tangential acceleration a = dvdt = kr
Now force F = m × a = mkr
So power P = F × v = mkr × krt = m k2r2t2