The lamp is designed for DC operation with the following specifications:
\[
V_{\mathrm{DC}} = 110 \, \mathrm{V}, \quad I = 11 \, \mathrm{A}.
\]
The power consumed by the lamp is:
\[
P = V_{\mathrm{DC}} \cdot I = 110 \cdot 11 = 1210 \, \mathrm{W}.
\]
When the lamp is connected to an AC source of $220 \, \mathrm{V}$ and $50 \, \mathrm{Hz}$ with a coil in series, the total impedance $Z$ of the circuit is given by:
\[
Z = \frac{V_{\mathrm{AC}}}{I} = \frac{220}{11} = 20 \, \Omega.
\]
The impedance of the circuit is the combination of the resistance of the lamp and the inductive reactance of the coil:
\[
Z = \sqrt{R^2 + X_L^2}.
\]
The resistance of the lamp is:
\[
R = \frac{V_{\mathrm{DC}}}{I} = \frac{110}{11} = 10 \, \Omega.
\]
The inductive reactance $X_L$ is given by:
\[
X_L = \sqrt{Z^2 - R^2}.
\]
Substituting the values:
\[
X_L = \sqrt{20^2 - 10^2} = \sqrt{400 - 100} = \sqrt{300} = 10\sqrt{3} \, \Omega.
\]
The inductive reactance is related to the inductance $L$ by:
\[
X_L = \omega L,
\]
where $\omega = 2\pi f$ is the angular frequency of the AC source. For $f = 50 \, \mathrm{Hz}$:
\[
\omega = 2\pi \cdot 50 = 100\pi \, \mathrm{rad/s}.
\]
Substituting for $L$:
\[
L = \frac{X_L}{\omega} = \frac{10\sqrt{3}}{100\pi}.
\]
Simplifying:
\[
L = \frac{\sqrt{3}}{10\pi} \, \mathrm{H}.
\]
Approximating:
\[
L \approx 0.064 \, \mathrm{H}.
\]