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59.

Problem 13.56P (HRW)

A rigid body can turn around a vertical axis until it presses against identical rubber stoppers A and B attached to rigid walls at distances and from the axle. Initially the stoppers touch the walls, without being compressed. Then force F is applied perpendicular to the rod at a distance R from the axle. We have to find expressions for the forces compressing (a) stopper A and (b) stopper B.

Solution:             Click For PDF Version

We draw free-body diagram of the rod. When the rod presses against the stopper A it will experience force acting on it in the anti-clockwise direction and force acting on it in the clockwise direction as it compresses the stopper B. According to Newton’s third law of motion the magnitude of forces compressing stoppers A and B will be and . Conditions of static and rotational equilibrium will give algebraic equations that can be solved for and .

For static equilibrium the vector sum of forces acting on the rod has to be zero. That is

.

And, the condition of rotational equilibrium is that the vector sum of torques about the axle has to be zero. That is

.

Solving these equations for and , we find

,

and

.