A stone of mass m tied to the end of a string revolves in a vertical circle of radius R.

Question.
A stone of mass m tied to the end of a string revolves in a vertical circle of radius R. The net forces at the lowest and highest points of the circle directed vertically downwards are: [Choose the correct alternative]


A stone of mass m tied to the end of a string revolves in a vertical circle of radius R.

$T_{1}$ and $v_{1}$ denote the tension and speed at the lowest point. $T_{2}$ and $v_{2}$ denote corresponding values at the highest point.


solution:

(a)The free body diagram of the stone at the lowest point is shown in the following figure.

A stone of mass m tied to the end of a string revolves in a vertical circle of radius R.02

According to Newton’s second law of motion, the net force acting on the stone at this point is equal to the centripetal force, i.e.,

$F_{\text {tet }}=T-m \mathrm{~g}=\frac{m v_{1}^{2}}{R} \ldots(i)$

Where, $v_{1}=$ Velocity at the lowest point

The free body diagram of the stone at the highest point is shown in the following figure.

A stone of mass m tied to the end of a string revolves in a vertical circle of radius R.03

Using Newton’s second law of motion, we have:

$T+m g=\frac{m v_{2}^{2}}{R} \ldots$

Where, $v_{2}=$ Velocity at the highest point

It is clear from equations $(i)$ and $(i i)$ that the net force acting at the lowest and the highest points are respectively $(T-m g)$ and $(T+m g)$.

Leave a comment