(a) When body is released from the position $p$ (inclined at angle $\theta$ from vertical) then velocity at mean position
$v = \sqrt{2gl(1 - \cos{\theta)}}$
$\therefore$ Tension at the lowest point $= mg + \frac{mv^{2}}{l}$
$= mg + \frac{m}{l}\left\lbrack 2gl\left( 1 - \cos 60 \right) \right\rbrack = mg + mg = 2mg$