Concept:
In a series \(RLC\) circuit, current is maximum at resonance:
\[
X_L=X_C
\]
So,
\[
\omega L=\frac{1}{\omega C}
\]
which gives
\[
C=\frac{1}{\omega^2 L}
\]
At resonance, impedance becomes:
\[
Z=R
\]
ip
Step 1: Find angular frequency.
\[
f=50\text{ Hz}
\]
\[
\omega=2\pi f=100\pi
\]
ip
Step 2: Find capacitance at resonance.
\[
C=\frac{1}{\omega^2L}
=
\frac{1}{(100\pi)^2(2.5)}
\]
Using \(\pi^2=10\):
\[
(100\pi)^2=10000\pi^2=100000
\]
So,
\[
C=\frac{1}{100000\times 2.5}
=\frac{1}{250000}
=4\times10^{-6}\text{ F}
\]
\[
C=4\mu\text{F}
\]
ip
Step 3: Find maximum current.
At resonance:
\[
Z=R=11.5\Omega
\]
Peak current:
\[
I_{\max}=\frac{V_0}{R}=\frac{230}{11.5}=20\text{ A}
\]
ip
Hence, the correct answer is:
\[
\boxed{(A)\ 4\mu\text{F},\ 20\text{ A}}
\]