Step 1: Understanding central potential.
A central potential depends only on the distance \(r\) from a fixed point (the center), i.e., \(V = V(r)\). The force is always directed toward or away from the center.
Step 2: Conservation of angular momentum.
The torque on the particle is zero because \(\vec{r} \times \vec{F} = 0\). Hence, angular momentum \(\vec{L} = \vec{r} \times \vec{p}\) is conserved in both magnitude and direction.
Step 3: Implication for motion.
Because \(\vec{L}\) is constant in direction, the position vector \(\vec{r}\) always lies in a fixed plane perpendicular to \(\vec{L}\). Therefore, the motion is confined to a plane.
Step 4: Conclusion.
The motion is restricted to a plane due to conservation of angular momentum.
