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Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Comparison between RL and RC circuits01:24

Comparison between RL and RC circuits

An RC circuit consists of resistance and capacitance, while in an RL circuit, capacitance is replaced by an inductor. RL and RC circuits are first-order differential circuits that store energy. An RC circuit stores energy in the electric field, while an RL circuit stores energy in the magnetic field. When connected to a battery, an RC circuit charges the capacitor, causing the current to decrease from maximum to zero upon being fully charged. This increases the voltage across the capacitor from...
Series RLC Circuit without Source01:21

Series RLC Circuit without Source

Within the field of electrical circuits, source-free RLC circuits present an intriguing domain. These circuits comprise a series arrangement of a resistor, inductor, and capacitor, operating independently of external energy sources. Their initiation hinges upon utilizing the initial energy stored within the capacitor and inductor to instigate their functionality. Their mathematical equation, a second-order differential equation, sets these circuits apart. This equation captures how the...
Parallel Resonance01:23

Parallel Resonance

The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
Series Resonance01:17

Series Resonance

The RLC circuit impedance is defined as the ratio of the supply voltage to the circuit current. Resonance in such a circuit occurs when the imaginary part of this impedance equals zero. This specific condition means that the inductive reactance is exactly equal to the capacitive reactance. The frequency at which this happens is known as the resonant frequency. Mathematically, the resonant frequency is inversely proportional to the square root of the product of the inductance (L) and capacitance...

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Related Experiment Video

Updated: Jun 14, 2026

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
09:46

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

Published on: August 8, 2025

A comparison of modeling methods for ring resonator circuits.

Michael Gad1, David Yevick, Paul Jessop

  • 1Physics Department, University of Waterloo, 200 University Avenue West, Waterloo, Ontario N2L 3Z1 Canada. michael_monir@yahoo.com

Journal of the Optical Society of America. A, Optics, Image Science, and Vision
|April 3, 2010
PubMed
Summary

This study benchmarks three methods for analyzing complex ring resonator circuits. Coupling of modes in time (CMT) proves accurate and fast for large waveguide circuits with multiple rings.

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Area of Science:

  • Photonics and optical engineering
  • Electromagnetics and wave propagation
  • Computational physics

Background:

  • Compound ring resonator circuits, featuring coupled ring resonator (RR) cavities, are a complex optical configuration.
  • Previous analysis utilized the coupling of modes in space (CMS) technique.
  • A need exists to benchmark different computational methods for these structures.

Purpose of the Study:

  • To compare the accuracy, simplicity, and computational time of three standard analysis methods: Finite-Difference Time-Domain (FDTD), coupling of modes in time (CMT), and coupling of modes in space (CMS).
  • To provide a more effective benchmark using a complex two-dimensional (2D) ring resonator circuit.
  • To investigate the relationship between power loss coefficients in CMS and CMT models.

Main Methods:

  • Finite-Difference Time-Domain (FDTD) method.
  • Coupling of modes in time (CMT) analysis.
  • Coupling of modes in space (CMS) analysis.
  • Application to a 2D complex ring resonator circuit.

Main Results:

  • The coupling of modes in time (CMT) method demonstrates accuracy and speed, particularly for circuits with small coupling coefficients and losses.
  • CMT is effective even for large waveguide circuits containing multiple rings.
  • The study clarifies the relationship between power loss coefficients in CMS and CMT.

Conclusions:

  • CMT offers a highly efficient and accurate method for analyzing complex, multi-ring waveguide circuits.
  • The benchmark validates CMT as a superior choice for specific design and analysis scenarios in integrated photonics.
  • Understanding the loss coefficient relationship aids in model selection and parameterization.