Step 1: Understand the problem and given data
- Resistor, \(R = 50~\Omega\)
- Peak voltage, \(V_0 = 200\sqrt{2}~\text{V}\)
- When capacitor is removed, current lags voltage by \(37^\circ\)
- When inductor is removed, current leads voltage by \(37^\circ\)
Step 2: Interpret the phase angles
- Current lags voltage by \(37^\circ\) means the circuit is inductive with inductive reactance \(X_L\) present.
- Current leads voltage by \(37^\circ\) means the circuit is capacitive with capacitive reactance \(X_C\) present.
Step 3: Use the phase angle formula for R-L and R-C circuits
\[
\tan 37^\circ = \frac{X_L}{R} = \frac{X_C}{R}
\]
\(\tan 37^\circ \approx 0.75\)
Thus,
\[
X_L = X_C = 0.75 \times R = 0.75 \times 50 = 37.5~\Omega
\]
Step 4: Calculate the net reactance in the full LCR circuit
Since \(X_L = X_C\), the inductive and capacitive reactances cancel each other out:
\[
X = X_L - X_C = 0
\]
So the circuit behaves like a pure resistor of \(50~\Omega\).
Step 5: Calculate the RMS voltage
\[
V_{\text{rms}} = \frac{V_0}{\sqrt{2}} = \frac{200\sqrt{2}}{\sqrt{2}} = 200~\text{V}
\]
Step 6: Calculate the RMS current
\[
I_{\text{rms}} = \frac{V_{\text{rms}}}{R} = \frac{200}{50} = 4~\text{A}
\]
Step 7: Calculate power dissipated in the circuit
\[
P = I_{\text{rms}}^2 \times R = 4^2 \times 50 = 16 \times 50 = 800~\text{W}
\]
Step 8: Final conclusion
The power dissipated in the LCR circuit is \(800~\text{W}\).