Imagine a light planet revolving around a very massive star in a circular orbit of radius R with a period of revolution T. If the gravitational force of attraction between planet and star is proportional to R−52, then T2 is proportional to
R72
For revolution of planet centripetal force is provided by gravitational force of attraction
mω2R∝R−52⇒1T2∝R−72⇒T2∝R72