• At resonance, the inductive reactance $X_L$ = capacitive reactance $X_C$, so $V_{RMS}$ across R is $I \cdot R$, and current $I = \frac{V_{source}}{R}$.
• Voltage across capacitor: $V_C = I \cdot X_C$.
• Series resonance voltage across L or C can exceed source voltage (series resonance phenomenon).
• Using $V_C = I \cdot X_C = V \frac{X_C}{R} = 80 \cdot \frac{X_C}{160}$.
• After calculating $X_C = \frac{1}{2 \pi f C}$ and plugging in, $V_C = 88$ V.
• Hence, voltage across capacitor = 88 V.