A spherically symmetric gravitational system of particles has a mass density
\[
\rho =
\begin{cases}
\rho_0 & \text{for } r \le R \\
0 & \text{for } r > R
\end{cases}
\]
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:
Show Hint
Inside a uniform sphere, gravitational field is proportional to distance from the centre.
Step 1: For \(r \le R\), enclosed mass \(M(r) \propto r^3\).
Step 2: Gravitational force provides centripetal force:
\[
\frac{v^2}{r} = \frac{GM(r)}{r^2}
\Rightarrow v \propto r
\]
Step 3: For \(r > R\), total mass is constant:
\[
v = \sqrt{\frac{GM}{r}} \Rightarrow v \propto \frac{1}{\sqrt{r}}
\]
Thus, velocity increases linearly inside and decreases outside.