A disc of mass m and radius R is placed over a plank of mass m. There is sufficient friction between disc and plank to prevent slipping and there is no friction between plank and ground. A horizontal force F is applied at the centre of the disc, then
Question
A disc of mass m and radius R is placed over a plank of mass m. There is sufficient friction between disc and plank to prevent slipping and there is no friction between plank and ground. A horizontal force F is applied at the centre of the disc, then
Solution
It seems like you didn't finish your question. However, I can start explaining based on what you've given.
When a horizontal force F is applied at the center of the disc, the force is distributed between the disc and the plank due to the friction between them. The force causes both the disc and the plank to move.
The force F causes the disc to rotate and translate. The frictional force between the disc and the plank provides the torque needed for the disc to rotate.
The same frictional force acts on the plank in the opposite direction, causing the plank to translate.
The motion of the system (the disc and the plank) depends on the distribution of the force between the disc and the plank, which depends on factors such as the coefficient of friction between the disc and the plank and the moment of inertia of the disc.
Please provide the rest of the question or specify what you want to know so I can give a more detailed explanation.
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