Q.
A small planet is revolving around a very massive star in a circular orbit of radius r with a period of revolution T . If the gravitational force between the planet and the star is proportional to r−5/2 , then T will be proportional to
Gravitational force provides the necessary centripetal force required by the given planet for circular motion. So rmv2∝r−5/2 ⇒rmv2=kr−5/2 , k = constant ∴v=mkr−3/2 T=v2πr=2πr×kr−3/2m
i.e., T∝r7/4 .