Concept:
For circular motion, the central force provides the centripetal force.
\[
F=\frac{mV^2}{R}.
\]
Given,
\[
F\propto R^{-5/2}.
\]
Step 1: Find the dependence of orbital velocity on \(R\).
Using
\[
\frac{mV^2}{R}
\propto
R^{-5/2},
\]
we get
\[
V^2
\propto
R^{-5/2}\cdot R.
\]
\[
V^2
\propto
R^{-3/2}.
\]
Therefore,
\[
V
\propto
R^{-3/4}.
\]
Step 2: Find the dependence of time period on \(R\).
For circular motion,
\[
T=\frac{2\pi R}{V}.
\]
Substituting
\[
V\propto R^{-3/4},
\]
\[
T
\propto
R^{1+\frac34}.
\]
\[
T
\propto
R^{7/4}.
\]
Step 3: Choose the correct option.
Thus,
\[
V\propto R^{-3/4}
\]
and
\[
T\propto R^{7/4}.
\]
Therefore,
\[
\boxed{
V\propto R^{-3/4},
\qquad
T\propto R^{7/4}
}
\]
\[
\boxed{\text{Answer = (A)}}
\]