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A particle of mass m is moving along a trajectory given by x = x 0 + a cos ω 1 t y = y 0 + b sin ω 2 t The torque, acting on the particle about the origin , at t = 0 is :
- – m (x 0 2 2 b ω – y 0 2 1 a ω ) k ˆ
- Zero
- k ˆ a my 2 1 0 ω +
- k ˆ ) a y b x (– m 2 1 0 0 ω +
Correct answer: k ˆ a my 2 1 0 ω +
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