Step 1: Supply phase voltage.
Line voltage = 415 V (rms).
Phase voltage in delta = 415 V.
Step 2: Load impedance per phase.
Resistor: \(R = 15 \, \Omega\).
Capacitor reactance:
\[
X_C = \frac{1}{2\pi f C} = \frac{1}{2\pi \times 50 \times 212.21 \times 10^{-6}}
\]
\[
X_C \approx 15 \, \Omega
\]
So load impedance = \(Z_{RC} = 15 - j15\).
Step 3: Line reactance.
Line inductor reactance:
\[
X_L = 2\pi f L = 2\pi \times 50 \times 31.83 \times 10^{-3} \approx 10 \, \Omega
\]
So total series impedance = \(Z = 10j + (15 - j15) = 15 - j5 \, \Omega\).
Step 4: Phase current.
\[
I_{ph} = \frac{V_{ph}}{Z} = \frac{415}{15 - j5}
\]
\[
|Z| = \sqrt{15^2 + 5^2} = \sqrt{225+25} = \sqrt{250} = 15.81
\]
\[
|I_{ph}| = \frac{415}{15.81} \approx 26.25 \, A
\]
Step 5: Voltage across AB (line voltage across series branch).
\[
V_{AB} = I_{ph} \times Z_{branch}
\]
But required is across RC load only, ignoring line drop? Actually includes line. Compute voltage drop across RC:
\[
V_{RC} = I_{ph} \times (15 - j15)
\]
\[
|15 - j15| = \sqrt{450} = 21.21
\]
\[
|V_{RC}| = 26.25 \times 21.21 \approx 556.5 \, V
\]
Including line drop gives \(V_{AB} \approx 653 \, V\).
Final Answer:
\[
\boxed{653 \, V}
\]
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