Understanding Vertical Circular Motion
Vertical circular motion occurs when an object is tied to a string and whirled in a vertical circle. Unlike horizontal circular motion, the speed of the object is not constant because gravity constantly acts upon it, altering its kinetic and potential energy.
The Critical Conditions
The motion of the particle is entirely dictated by its initial velocity at the lowest point (\(u\) or \(v_{bottom}\)):
- Completing the Loop (\(u \ge \sqrt{5gR}\)): To maintain a circular path over the top without the string going slack, the tension at the top must be at least zero. This requires a minimum velocity at the bottom of \(\sqrt{5gR}\).
- Going Slack (\(\sqrt{2gR} < u < \sqrt{5gR}\)): The particle passes the horizontal position but lacks the energy to reach the top. The tension reaches zero before the velocity does, causing the string to go slack and the particle to fall in a parabolic projectile trajectory.
- Pendulum Motion (\(u \le \sqrt{2gR}\)): The particle does not even reach the horizontal position. Its velocity reaches zero before tension reaches zero, resulting in oscillation back and forth like a pendulum.
The Mathematics of Tension
The tension (\(T\)) in the string at any angle \(\theta\) (measured from the lowest point) is determined by the centripetal force requirement and the component of gravity acting along the string:
By applying the Law of Conservation of Energy, we can find the velocity \(v\) at any angle \(\theta\):