Step 1: Relationship Between Root-Mean-Square (rms) Value and Peak Value.
The root-mean-square (rms) value \( V_{\text{rms}} \) of an alternating voltage is related to the peak value \( V_{\text{max}} \) by:
\[
V_{\text{rms}} = \frac{V_{\text{max}}}{\sqrt{2}}
\]
This relation holds for both current and voltage in an AC circuit.
Step 2: Inductive Reactance.
The inductive reactance \( X_L \) is given by the formula:
\[
X_L = 2 \pi f L
\]
where:
- \( f \) is the frequency of the AC supply,
- \( L \) is the inductance of the coil.
Given that \( L = 8.1 \, \text{mH} = 8.1 \times 10^{-3} \, \text{H} \), we can calculate \( X_L \) if the frequency \( f \) is provided.
Step 3: Potential Difference Across the Resistance.
The total impedance \( Z \) in an R-L circuit is given by:
\[
Z = \sqrt{R^2 + X_L^2}
\]
where:
- \( R = 10 \, \Omega \) is the resistance,
- \( X_L \) is the inductive reactance.
The potential difference across the resistance is given by:
\[
V_R = I \cdot R
\]
where \( I \) is the current in the circuit, which can be calculated using the rms voltage and the total impedance:
\[
I = \frac{V_{\text{rms}}}{Z}
\]
Substitute the values to find the potential difference across the resistance.