The three elements X, Y, and Z are connected in series across an AC source. From the previous question, we know:
- Element X is a resistor, with impedance \( Z_X = R \).
- Element Y is an inductor, with impedance \( Z_Y = j\omega L \), where \( \omega = 2\pi f \) is the angular frequency and \( L \) is the inductance.
- Element Z is a capacitor, with impedance \( Z_Z = \frac{1}{j\omega C} \), where \( C \) is the capacitance.
The total impedance \( Z_{\text{total}} \) of the series circuit is the sum of the individual impedances:
\[
Z_{\text{total}} = Z_X + Z_Y + Z_Z
\]
\[
Z_{\text{total}} = R + j\omega L + \frac{1}{j\omega C}
\]
\[
Z_{\text{total}} = R + j\left( \omega L - \frac{1}{\omega C} \right)
\]
Thus, the impedance of the series circuit is:
\[
Z_{\text{total}} = R + j \left( \omega L - \frac{1}{\omega C} \right)
\]
### Step 1: Variation of current with frequency
The current \( I \) in the series circuit is given by Ohm's law:
\[
I = \frac{V}{Z_{\text{total}}}
\]
Since \( Z_{\text{total}} \) depends on the frequency \( f \), the current will vary with \( f \).
- When \( f \) is low, the capacitive reactance \( \left( \frac{1}{\omega C} \right) \) is high, so the current is lower.
- When \( f \) increases, the inductive reactance \( (\omega L) \) increases, and the capacitive reactance decreases, so the current starts increasing until it reaches a peak.
- Beyond a certain frequency, the inductive reactance dominates, and the current decreases.
Thus, the current shows a resonant behavior with frequency, with the impedance being lowest at a certain resonant frequency \( f_0 \).
% Correct Answer
Correct Answer:}
- Impedance of the series circuit:
\[
Z_{\text{total}} = R + j \left( \omega L - \frac{1}{\omega C} \right)
\]