91Ó°ÊÓ

Impedance in an LRC series circuit is a key factor that helps us understand how much opposition the circuit presents to alternating current flow. It is a combination of resistance, inductance, and capacitance, creating a total effective opposition known as impedance, denoted as \( Z \).
In a circuit with resistance \( R \), inductance \( L \), and capacitance \( C \), the impedance is calculated using the formula:

• \( Z = \sqrt{R^2 + (\omega L - \frac{1}{\omega C})^2} \)

Here, \( \omega \) is the angular frequency of the AC source. For the given exercise values: \( R = 60.0 \, \Omega \), \( L = 0.800 \, \text{H} \), \( C = 3.00 \times 10^{-4} \, \text{F} \), and \( \omega = 120 \, \text{rad/s} \), we calculate the impedance.
Replacing these into the formula helps find \( Z \), which is necessary to determine how much current flows through the circuit under a given voltage.

Energy in an inductor is all about magnetic fields. When current runs through an inductor, it creates a magnetic field storing energy. The maximum energy stored in an inductor is crucial for understanding how the circuit functions during alternating current flow.
The energy stored in an inductor \( L \) with current \( I \) is expressed as:

• \( E_L = \frac{1}{2} L I^2 \)

To calculate the maximum energy, we first need to discover the maximum current, which is found using the impedance and the voltage amplitude of the AC source.

• Maximum current, \( I = \frac{V_0}{Z} \)

Here, \( V_0 \) is the voltage amplitude (90.0 V). Calculating \( I \) using the impedance we found, allows us to substitute into \( E_L = \frac{1}{2} L I^2 \) to find the maximum energy stored in the inductor. This shows the peak energy storage capability in a magnetic field for our given circuit.

Capacitors store energy electrically, unlike inductors that store it magnetically. When a capacitor is fully charged, it holds maximum energy, which is key in transitioning areas between energy states.
The energy stored in a capacitor \( C \) with voltage \( V \) is given by the formula:

• \( E_C = \frac{1}{2} C V^2 \)

In the context of an LRC circuit, when the energy in the inductor is at its maximum, the energy in the capacitor is zero, highlighting their complementary role.
To find the maximum energy stored in the capacitor, we use the same voltage amplitude \( V = V_0 = 90.0 \, \text{V} \). Plugging this into the energy formula gives the peak energy storage capability of the capacitor. This shows how energy transitions between components in the oscillatory process of the AC circuit.