(c) Let gravitation field is zero at $P$ as shown in figure.
[image:8_image52.emf]
$\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \frac{Gm}{x^{2}} = \frac{G(4m)}{(r - x)^{2}}$
$\Longrightarrow \ \ \ \ \ \ \ \ \ \ {4x}^{2} = (r - x)^{2}$
$\Longrightarrow \ \ \ \ \ \ \ \ \ \ \ \ 2x = r - x$
$\Longrightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ x = \frac{r}{3}$
$\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \ V_{p} = \frac{Gm}{x} - \frac{G(4m)}{r - x}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = \ - \frac{3Gm}{r} - \frac{6Gm}{r} = - \frac{9Gm}{r}$