(c) Weight of the body at equator $= \frac{3}{5}$ of initial weight
$\therefore g^{'} = \frac{3}{5}g$ (because mass remains constant)
$g^{'} = g - \omega^{2}R\cos^{2}{\lambda \Rightarrow \frac{3}{5}g = g - \omega^{2}R\cos^{2}{(0{^\circ})}}$
$\Rightarrow \omega^{2} = \frac{2g}{5R} \Rightarrow \omega = \sqrt{\frac{2g}{5R}} = \sqrt{\frac{2 \times 10}{5 \times 6400 \times 10^{3}}}$
$= 7.8 \times 10^{- 4}\ \frac{rad}{\sec}$