Step 1: Recall the formula for inductive reactance.
An inductor resists alternating current through its reactance:
\[
X_L = \omega L = 2\pi f L
\]
This plays the role of resistance for AC circuits, but causes no energy dissipation.
Step 2: Calculate the angular frequency.
$f = 50\,\text{Hz}$:
\[
\omega = 2\pi \times 50 = 100\pi\,\text{rad/s}
\]
Step 3: Compute the inductive reactance.
$L = 70\,\text{mH} = 70 \times 10^{-3}\,\text{H}$:
\[
X_L = 100\pi \times 70 \times 10^{-3} = 7\pi\,\Omega
\]
Step 4: Simplify using the approximation $\pi \approx 22/7$.
\[
X_L = 7 \times \frac{22}{7} = 22\,\Omega
\]
Step 5: Apply Ohm's law for AC to find rms current.
For a purely inductive circuit:
\[
I_\text{rms} = \frac{V_\text{rms}}{X_L} = \frac{220}{22} = 10\,\text{A}
\]
Step 6: State the answer.
\[
\boxed{10\,\text{A}}
\]