Given Form Kepler;s III law,
T∝ r \(\frac{3}{2}\)
T is also function of g and R
⇒ T∝r\(\frac{3}{2}\)Rygx= kr\(\frac{3}{2}\)Rygx
[k = dimension less constant of proportionality]
Substituting dimensionless in each term-
∴ [L0M0T-1] = k[L3/2M0T0][L1M0T-2]x [L]y
= k[Lx+y+3/2T-2x]
For L, 0 = \(\frac{3}{2}\)+x+y
For T, 1 = 0 – 2x
⇒ x = \(-\frac{1}{2}\)
Therefore, 0 = \(\frac{3}{2}\) \(-\frac{1}{2}\)+ y
⇒ y = -1
Thus,
T = kr3/2g−1/2 R-1
=\(\frac{k}{R}\sqrt\frac{r^3}{g}\)