A spherically symmetric gravitational system of particles has a mass density
$\rho = \left\{ {\matrix{
{{\rho _0}} & {for} & {r \le R} \cr
0 & {for} & {r > R} \cr
} } \right.
Where \rho_0 is a constant. A test mass can undergo circular motion under the influence of the gravitational field of particles. Its speed V as a function of distance r(0 < r < \infty)$ from the centre of the system is represented by