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 stars is proportion to R1/2 , there T2 is proportional to.
When planet is revolving around a massive star in a circular orbit of radius R with a period of revolution T then centripetal force is balanced by gravitational force as
mRω2=GmMR−12
ω2=1R12
∵ω=2πT
(2πT)2=1R12
1T2∝1R12
T2∝R12