A ball of mass $m = 0.1$ kg hangs on a thread of length $l = 1$ m and moves uniformly in a circle in a horizontal plane. The thread makes an angle $\alpha = 60°$ with the vertical (see the figure). Find the tension $T$ in the thread and the period $\tau$ of the ball's revolution. Take $g = 10$ m/s².
The ball moves in a circle of radius $r = l\sin\alpha$ with a centripetal acceleration directed horizontally toward the axis. The forces on the ball are gravity and the thread tension.
1. There is no vertical acceleration:
$$T\cos\alpha = mg \;\Rightarrow\; T = \frac{mg}{\cos\alpha} = \frac{1}{0.5} = 2 \text{ N}$$2. Horizontally, a component of the tension provides the centripetal acceleration $a = \omega^2 r$:
$$T\sin\alpha = m\omega^2 r = m\omega^2 l\sin\alpha \;\Rightarrow\; T = m\omega^2 l$$$$\omega^2 = \frac{T}{ml} = \frac{2}{0.1 \cdot 1} = 20 \;\Rightarrow\; \omega \approx 4.47 \text{ rad/s}$$3. The period:
$$\tau = \frac{2\pi}{\omega} = \frac{2 \cdot 3.14}{4.47} \approx 1.41 \text{ s}$$The general formula is $\tau = 2\pi\sqrt{\dfrac{l\cos\alpha}{g}}$ — the period does not depend on the mass of the ball.
$T = 2$ N, $\tau \approx 1.41$ s