Solution :
When string makes an angle $$\theta $$ with the vertical in a vertical circle, then balancing the force we get
$$T - mg\cos \theta = \frac{{m{v^2}}}{l}$$

$${\text{or}}\,T = mg\cos \theta + \frac{{m{v^2}}}{l}$$
Tension is maximum when $$\cos \theta = + 1$$
i.e. $$\theta = 0$$
Thus, $$\theta $$ is zero at lowest point $$B.$$ At this point tension is maximum. So, string will break at point $$B.$$
NOTE
The critical speed of a body on circular path, $${v_c} = \sqrt {Rg} ,R = $$ radius of path.
If at the highest point, the speed is less than this, the string would become slack and the body would leave the circular path.