Step 1: Understanding the RLC Series Circuit.
In a series RLC circuit, the current lags behind the voltage under certain conditions, depending on the relationship between the driving frequency \( n \) and the resonant frequency \( n_r \). The resonant frequency is given by:
\[
n_r = \frac{1}{2 \pi \sqrt{LC}}
\]
When the driving frequency is less than the resonant frequency, the circuit behaves inductively, and the current lags behind the voltage.
Step 2: Analysis of options.
- (A) \( n = 0 \): If the frequency is zero, there is no oscillation, and the current will not be defined as lagging.
- (B) \( n<n_r \): When the frequency is less than the resonant frequency, the inductive reactance dominates, and the current lags behind the voltage. This is the correct answer.
- (C) \( n = n_r \): At resonance, the current and voltage are in phase, meaning there is no lag.
- (D) \( n>n_r \): When the frequency is greater than the resonant frequency, the capacitive reactance dominates, and the current leads the voltage, not lags behind it.
Step 3: Conclusion.
The current lags behind the voltage when the frequency of the source is less than the resonant frequency, making option (B) the correct answer.