Back to chapter

5.11:

Parallel RLC Circuits

JoVE Core
Electrical Engineering
This content is Free Access.
JoVE Core Electrical Engineering
Parallel RLC Circuits

Languages

Share

Consider a street lamp with an RLC surge protector to protect its components from sudden voltage spikes. This setup can be approximated by the simplest parallel RLC circuit with an input DC source generating a step response. When the switch is flipped on, applying Kirchhoff's current law at the top node yields a second-order differential equation. The complete solution to this equation is a combination of transient and steady-state responses. The transient response diminishes over time and resembles the source-free series RLC solutions in various damping scenarios. If the damping factor exceeds the resonant frequency, the response is overdamped. When the damping factor equals the resonant frequency, the response is critically damped. If the damping factor is less than the resonant frequency, the response is underdamped. The steady-state response corresponds to the final inductor current, matching the source current. The constants involved can be deduced from the initial conditions of the circuit. Eliminating the input source current results in solely a transient response.

5.11:

Parallel RLC Circuits

Street lamps equipped with RLC surge protectors are an excellent example of applying circuit analysis in practical scenarios. These surge protectors safeguard the lamp's components against sudden voltage spikes.

A simplified parallel RLC circuit model with a DC input source generating a step response is employed in this context. When the switch is turned on, Kirchhoff's current law is applied, leading to a second-order differential equation.

Equation1

Interestingly, this equation's solution comprises both transient and steady-state responses. The transient response gradually diminishes over time, exhibiting similarities to the source-free series RLC circuit solutions under different damping conditions. If the damping factor surpasses the resonant frequency, the response becomes overdamped.

Equation2

When these two factors match, the response is critically damped.

Equation3

The response turns underdamped if the damping factor is less than the resonant frequency.

Equation4

The steady-state response corresponds to the final inductor current, aligning with the source current. Determining the constants involved relies on the initial conditions of the circuit.

Notably, only the transient response remains when the input source current is eliminated. Parallel RLC circuits find extensive applications, particularly in communications networks and filter designs. Understanding their behavior under different damping scenarios contributes to adequate surge protection and circuit design in practical settings.