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A particle of mass m is moving in a circular path of constant radius r such that its centripetal acceleration a is varying with time t as a = k^(2)rt^(2) where k is a constant. What is the power delivered to the particle by the forces acting on it. |
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Answer» <P> Solution :`Asa_(c)=(v^(2)//R)so(v^(2)//r)=k^(2)rt^(2)`KINETIC energy `K = (1)/(2) mv^(2) = (1)/(2) mk^(2)r^(2)t^(2)` Now by work - Enetgy Theorem `W=DeltaK=(1)/(2)mk^(2)r^(2)t^(2)-0rArrP=(dw)/(dt)` `RARR P = (d)/(dt) = (1)/(2) mk^(2)r^(2)t^(2) =mk^(2)r^(2)t` |
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