A string of certain length used to whirl a stone in a vertical circle with certain velocity. The tension developed in the string will be
highest at the bottom of the circle
When a stone is whirled in a vertical circle using a string, the tension in the string is not constant. It changes depending on the position of the stone in the circle. This variation in the tension in string is due to the combined effect of gravity and the requirement for centripetal force.
At any point in the vertical circle, two main forces act on the stone:
For the stone to move in a circular path, there must be a net force acting towards the center of the circle. This net force provides the necessary centripetal force ($F_c = \frac{mv^2}{r}$), where $m$ is the mass, $v$ is the speed of the stone at that point, and $r$ is the radius of the circle (length of the string).
Let's consider the forces at the top and bottom of the vertical circle:
Due to gravity, the speed of the stone is not constant. The stone slows down as it moves upwards and speeds up as it moves downwards. The speed is maximum at the bottom of the circle ($v_{bottom}$) and minimum at the top ($v_{top}$). Thus, $v_{bottom} > v_{top}$.
Comparing the expressions for tension at the top and bottom:
Since $v_{bottom} > v_{top}$, the term $\frac{mv_{bottom}^2}{r}$ is greater than $\frac{mv_{top}^2}{r}$. Furthermore, $mg$ is subtracted from $\frac{mv_{top}^2}{r}$ to get $T_{top}$, while $mg$ is added to $\frac{mv_{bottom}^2}{r}$ to get $T_{bottom}$.
This clearly shows that the tension in string is highest at the bottom of the circle and least at the top of the circle.
Based on the analysis of forces and velocity in vertical circular motion, the tension in string developed when whirling a stone in a vertical circle is highest at the bottom of the circle.

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