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