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To find the torque, we note that the applied force is perpendicular to the radius and friction is negligible, so that Solution for (a) The moment of inertia of a solid disk about this axis is given in (Figure) to be where and , so that Now, after we substitute the known values, we find the angular acceleration to be Solution for (b) We expect the angular acceleration for the system to be less in this part, because the moment of inertia is greater when the child is on the merry-go-round
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