If gravitational attraction between two point masses be given by F=Gm1m2r3 Then, the period of asatellite in a circular orbit will be proportional to
r
r2
r12
independent of r
As, mv2r=Gm1m2r3 or v∝r1-32
Now, T=2πrv or T∝rv
∴ T∝rr1-32⇒T∝r1+32=r2