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−52, then T would be proportional to
Given, the gravitational force between the planet and the star is
F∝1R52
For motion of planet in a circular orbit,
mRω2=kR52(k is constant)
mR(2πT)2=kR52(∵ω=2πT)
4π2T2=k/mR72⇒T2=4π2k/mR72
T2∝R72
or, T∝R74