A particle of mass M is situated at the centre of a spherical shell of same mass and radius a. The gravitational potential at a point situated at \(\frac{a}{2}\) distance from the centre, will be : |
\(-4\frac{GM}{a}\) \(-3\frac{GM}{a}\) \(-3\frac{GM}{a}\) \(-\frac{GM}{a}\) |
\(-3\frac{GM}{a}\) |
Gravitational potential at a point \(\frac{a}{2}\) distance from centre = gravitational potential due to spherical shell + gravitational potential due to mass M Vg = \(-\frac{GM}{a} - \frac{GM}{a/2}\) = \(-3\frac{GM}{a}\) |