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Sound Waves: Resonance01:14

Sound Waves: Resonance

Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
Concept of Resonance and its Characteristics01:19

Concept of Resonance and its Characteristics

If a driven oscillator needs to resonate at a specific frequency, then very light damping is required. An example of light damping includes playing piano strings and many other musical instruments. Conversely, to achieve small-amplitude oscillations as in a car's suspension system, heavy damping is required. Heavy damping reduces the amplitude, but the tradeoff is that the system responds at more frequencies. Speed bumps and gravel roads prove that even a car's suspension system is not immune...
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...
RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
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:

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Related Experiment Video

Updated: Jun 15, 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

Unstable resonators for annular gain volume lasers.

P B Mumola, H J Robertson, G N Steinberg

    Applied Optics
    |March 4, 2010
    PubMed
    Summary

    This study details the performance of unstable resonators for annular cylindrical lasers. A half-symmetric unstable resonator with an intracavity axicon achieved near diffraction-limited laser beam quality.

    Area of Science:

    • Optics and Photonics
    • Laser Physics
    • Resonator Design

    Background:

    • Unstable resonators are crucial for high-power laser systems.
    • Controlling beam quality in lasers with annular cylindrical mode volumes presents unique challenges.
    • Previous research has explored various resonator configurations, but optimization for specific laser types remains an active area.

    Purpose of the Study:

    • To experimentally evaluate the performance of different unstable resonators for annular cylindrical mode volumes.
    • To investigate the impact of resonator component misalignments and figure errors on laser output beam quality.
    • To demonstrate a resonator design capable of achieving near diffraction-limited beam quality in a He-Xe laser.

    Main Methods:

    • Fabrication and testing of several unstable resonator configurations for annular cylindrical lasers.

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  • Characterization of laser output beam quality using standard optical metrology techniques.
  • Analysis of sensitivity to mechanical misalignments and optical surface imperfections.
  • Main Results:

    • Experimental performance data for multiple unstable resonator designs were collected.
    • The sensitivity of laser beam quality to resonator component errors was quantified.
    • A half-symmetric unstable resonator incorporating an intracavity axicon yielded near diffraction-limited beam quality.

    Conclusions:

    • The tested unstable resonators show varying degrees of suitability for annular cylindrical lasers.
    • Careful design and alignment are critical for maintaining high beam quality in these systems.
    • The demonstrated resonator configuration offers a promising approach for achieving high-quality output from annular cylindrical He-Xe lasers.