Step 1: Resonance condition in an LCR circuit:
At resonance, the inductive reactance (\(X_L\)) and capacitive reactance (\(X_C\)) become equal:
\[ X_L = X_C \]
Step 2: Implication for circuit impedance:
At resonance, the net reactance is zero. Hence, the impedance (\(Z\)) of the LCR circuit at resonance is purely resistive, equal to \(R\):
\[ Z = R \]
Step 3: Phase difference at resonance:
In a purely resistive circuit, voltage and current are in phase. Thus, the phase difference (\(\phi\)) between voltage and current at resonance is:
\[ \phi = 0 \]
Final Conclusion:
At resonance, the voltage and current in a series LCR circuit are in phase (phase difference = 0).
In a series LCR circuit at resonance, the inductive reactance (\( X_L \)) and capacitive reactance (\( X_C \)) are equal, i.e., \( X_L = X_C \). Therefore, the total reactance is zero, and the impedance of the circuit becomes purely resistive. At resonance, the current and voltage are in phase, meaning the phase difference between them is zero.
This is because the voltage and current reach their maximum values simultaneously, and there is no phase shift between them.
Thus, the phase difference is zero.
Find output voltage in the given circuit. 
The circuit shown in the figure contains two ideal diodes \( D_1 \) and \( D_2 \). If a cell of emf 3V and negligible internal resistance is connected as shown, then the current through \( 70 \, \Omega \) resistance (in amperes) is: 