Radial & Tangential Acceleration for Non Uniform Circular Motion
A particle of...
Question
A particle of mass m is moving in a circular path of constant radius r such that centripetal acceleration is varying with time t as k2rt2, where k is a constant. The power delivered to the particle by the force acting on it is
A
m2k2r2t2
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B
mk2r2t
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C
mk2rt2
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D
mkr2t
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Solution
The correct option is Bmk2r2t Given that,
Centripetal acceleration, ac=k2rt2
Where, ac=v2r ⇒v2r=k2rt2 ⇒v=krt.......(1)
The work done by the centripetal force is zero because the direction of centripetal force is perpendicular to the velocity.
Tangential acceleration of the particle, at=dvdt=kr..........(2)
Tangential force acting on the particle, F=mat=mkr
The power delivered to the particle is P=→F.→v=Fvcosθ ∴P=Fv=(mkr)×krt(∵θ=0∘) ⇒P=mk2r2t