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A uniform cylinder isrotating aboutis own axis with a constant angular speed ω. Very gently it is placed on a rough horizontal surface at t1 . At t = t2 it starts rolling without slipping. The rotational kinetic energy of cylinder at t1 , t2 and t3 (>t2 ) is K1 , K2 and K3 respectively. Then

(1) K1 = K2 = K3

(2) K1 = K2 ; K2 = K3

(3) K1 > K2 > K3

(4) K2 > K1 > K3

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(2) K1 = K2 ; K2 = K3

When rotating cylinder is gently placed on rough horizontal surface at t = t1 ; it initally slips. But at t = t2 , slipping stops. There is loss of energy due to friction between horizontal surface and cylinder i.e K2 < t2 ; the cylinder moves with speed it has accquired and its energy remains same as at t = t2 i.e K2 = K3 .

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