(c) The metallic spheres will be at positions as shown in the figure.
[image:8_image59.emf]
$T\sin{\theta = F = \frac{GM \times M}{L^{2}}}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = \frac{{GM}^{2}}{L^{2}}$
$\ \ \ \ \ \ \ \ T\cos{\theta = Mg}$
$\therefore\ \ \ \ \ \ \ \ \tan{\theta = \frac{GM}{gL^{2}}}$
$or\ \ \ \ \ \ \ \ \ \ \ \ \ \ \theta = \tan^{- 1}\left( \frac{GM}{gL^{2}} \right)$