A rod of mass n and length l is hinged at one of its end A as shown in figure. A force F is applied at distance x from A. The instantaneous acceleration of center of mass a varies with x as
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Explanation:
Let the force F be applied at a distance x from the hinged point.
Hence, τ==Iα=3mL2α ...(1)
Since the cm is at a distance 2L from the hinged end, its acceleration a=2Lα
⇒α=L2a
Substituting α in (1)
Fx=3mL2α=3mL2L2a
⇒a=2mL3Fx
⇒a=(constant)x
The above is equation of a straight line.
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