1. The ball's horizontal circular motion implies balanced vertical forces: gravity (\(mg\)) and the string's vertical tension component. The ball experiences two forces:
Gravity: \(mg\) and String Tension: \(T\)
2. The horizontal tension component (\(T \sin \theta\)) provides the centripetal force for circular motion. The vertical component (\(T \cos \theta\)) counteracts the ball's weight.
3. Torque about the circle's center (O) is the force's cross product with the radius vector. Torque \(\tau\) is calculated as:
\(\tau = r \times F\)
where \(r\) is the radius (length \(L\)) and \(F\) is the force (tension). However, the tension acts along the string, generating no torque about the horizontal circle's center.
4. The total torque at the center is zero; the tension, causing circular motion, doesn't rotate the ball around the center.