$\begin{aligned}
& \text { (A) } \mathrm{G}=\frac{\mathrm{Fr}^2}{\mathrm{m}^2} \
& {[\mathrm{G}]=\frac{\left[\mathrm{MLT}^{-2}\right]\left[\mathrm{L}^2\right]}{\left[\mathrm{M}^2\right]}=\left[\mathrm{M}^{-1} \mathrm{L}^3 \mathrm{~T}^{-2}\right](\mathrm{IV})}
\end{aligned}$
(B)
$\begin{aligned}
& \text { P.E. }=\mathrm{mgh}=\left[\mathrm{MLT}^{-2} \mathrm{L}\right] \
& =\left[\mathrm{ML}^2 \mathrm{T}^{-2}\right] \text { (III) }
\end{aligned}$
(C) Gravitational Potential =rGM
=[L][M−1 L3 T−2][M]=[M0 L2 T−2]=[L2 T−2](II)
(D) Acceleration due to gravity =[g]=[LT−2](I)