Concept:
For a series RC circuit, the impedance is
\[
Z=\sqrt{R^2+X_c^2},
\]
where
\[
X_c=\frac{1}{2\pi fC}.
\]
The current is given by
\[
I=\frac{V}{Z}.
\]
Since the applied voltage remains constant, any change in current is due to the change in capacitive reactance.
Step 1: Write the expression for the initial current.
Initially,
\[
I=\frac{V}{\sqrt{R^2+X_c^2}}.
\]
Step 2: Determine the new reactance when frequency is reduced.
Since
\[
X_c=\frac{1}{2\pi fC},
\]
if the frequency becomes
\[
f'=\frac{f}{3},
\]
then the new capacitive reactance is
\[
X_c'=\frac{1}{2\pi (f/3)C}=3X_c.
\]
The new current is given to be
\[
\frac{I}{2}
=
\frac{V}{\sqrt{R^2+(3X_c)^2}}
=
\frac{V}{\sqrt{R^2+9X_c^2}}.
\]
Step 3: Form the required equation.
Substituting the value of \(I\),
\[
\frac{1}{2}\cdot
\frac{V}{\sqrt{R^2+X_c^2}}
=
\frac{V}{\sqrt{R^2+9X_c^2}}.
\]
Cancelling \(V\),
\[
\sqrt{R^2+9X_c^2}
=
2\sqrt{R^2+X_c^2}.
\]
Squaring both sides,
\[
R^2+9X_c^2
=
4(R^2+X_c^2).
\]
\[
R^2+9X_c^2
=
4R^2+4X_c^2.
\]
\[
5X_c^2
=
3R^2.
\]
Hence,
\[
\frac{X_c^2}{R^2}
=
\frac{3}{5}.
\]
Therefore,
\[
\boxed{\frac{X_c}{R}
=
\left(\frac{3}{5}\right)^{1/2}}
\]