Physics Unclassified 1 Mark
Appeared in: 2025 (3 sets)
Assertion (A) : A series LCR circuit behaves as a pure resistive circuit at resonance. Reason (R) : At resonance, $X_L = X_C$ gives $\omega = \frac{1}{\sqrt{LC}}$.
✓ Verified CBSE Marking Scheme Official Evaluation Steps & EL10 Insight

Correct Option: (a) Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of Assertion (A).

Step 1 (Governing Law & Definitions): [0.25 Mark]

In a series LCR circuit, the total impedance $Z$ is given by:

$$Z = \sqrt{R^2 + (X_L - X_C)^2}$$

Where $X_L = \omega L$ (inductive reactance) and $X_C = \frac{1}{\omega C}$ (capacitive reactance).

Step 2 (Step-by-Step Mathematical Working): [0.5 Mark]

  • At resonance, the condition is defined as $X_L = X_C$.
  • Substituting the expressions: $\omega L = \frac{1}{\omega C}$.
  • Rearranging for $\omega$: $\omega^2 = \frac{1}{LC} \implies \omega = \frac{1}{\sqrt{LC}}$.
  • Substituting $X_L = X_C$ into the impedance formula: $$Z = \sqrt{R^2 + (0)^2} = R$$

Step 3 (Final Concluded Answer): [0.25 Mark]

Since the impedance $Z$ becomes equal to the resistance $R$ ($Z = R$), the phase angle $\phi = \tan^{-1}\left(\frac{X_L - X_C}{R}\right) = 0$. Thus, the circuit behaves as a pure resistive circuit. Both statements are correct and logically linked.

💡 EL10 Concept Insight: Imagine the inductor and capacitor as two kids playing tug-of-war; at resonance, they pull with equal strength in opposite directions, effectively canceling each other out so that only the resistor is left to "feel" the current.