(i) Total impedance
The total impedance \( Z \) of an L-C-R series circuit is given by:
\[
Z = \sqrt{R^2 + \left(X_L - X_C \right)^2},
\]
where:
- \( R = 40 \, \Omega \) is the resistance,
- \( X_L = \omega L \) is the inductive reactance,
- \( X_C = \frac{1}{\omega C} \) is the capacitive reactance.
Given:
- \( L = 0.16 \, \text{H} \),
- \( C = 40 \, \mu\text{F} = 40 \times 10^{-6} \, \text{F} \),
- \( \omega = 500 \, \text{rad/s} \) (since the frequency \( f = \frac{500}{2\pi} \)).
First, calculate \( X_L \) and \( X_C \):
\[
X_L = \omega L = 500 \times 0.16 = 80 \, \Omega,
\]
\[
X_C = \frac{1}{\omega C} = \frac{1}{500 \times 40 \times 10^{-6}} = 50 \, \Omega.
\]
Now, substitute these values into the impedance formula:
\[
Z = \sqrt{40^2 + (80 - 50)^2} = \sqrt{1600 + 900} = \sqrt{2500} = 50 \, \Omega.
\]
So, the total impedance is \( Z = 50 \, \Omega \).
(ii) Power Factor:
The power factor (PF) in a series L-C-R circuit is given by:
\[
\text{PF} = \cos \phi = \frac{R}{Z},
\]
where:
- \( R = 40 \, \Omega \),
- \( Z = 50 \, \Omega \).
So, the power factor is:
\[
\text{PF} = \frac{40}{50} = 0.8.
\]
(iii) Peak Value of Current:
The peak current \( I_0 \) in the circuit is given by:
\[
I_0 = \frac{V_0}{Z},
\]
where:
- \( V_0 = 100 \, \text{V} \) is the peak voltage,
- \( Z = 50 \, \Omega \) is the total impedance.
So, the peak value of the current is:
\[
I_0 = \frac{100}{50} = 2 \, \text{A}.
\]