1. Step 1: The ball is moving in a horizontal circle, which means that the forces acting on it in the vertical direction (the gravitational force mg) are balanced by the vertical component of the tension in the string. The ball is subject to two forces:
Gravitational force: mg and Tension in the string: T
2. Step 2: Since the ball is in circular motion, the horizontal component of the tension T sin θ provides the centripetal force required for the circular motion. The vertical component T cos θ balances the weight of the ball.
3. Step 3: The torque about the center O of the horizontal circle is given by the cross product of the force and the radius vector. The torque τ due to the forces acting on the ball is calculated as:
τ = r × F
where r is the radius vector (the length L) and F is the force (in this case, the tension). However, since the tension is acting along the string, there is no torque about the center of the horizontal circle.
4. Step 4: Therefore, the total torque about the center is zero, because the force creating the circular motion (tension in the string) does not create any rotational effect about the center of the horizontal circle.