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Related Concept Videos

Shock Waves01:16

Shock Waves

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high pressures...
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...
Forced Oscillations01:06

Forced Oscillations

When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
Sound Waves: Interference00:53

Sound Waves: Interference

Sound waves can be modeled either as longitudinal waves, wherein the molecules of the medium oscillate around an equilibrium position, or as pressure waves. When two identical waves from the same source superimpose on each other, the combination of two crests or two troughs results in amplitude reinforcement known as constructive interference. If two identical waves, that are initially in phase, become out of phase because of different path lengths, the combination of crests with troughs...

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Related Experiment Video

Updated: Jul 19, 2026

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
08:19

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System

Published on: May 9, 2021

Subharmonic emissions from microbubbles: effect of the driving pulse shape.

Elena Biagi, Luca Breschi, Enrico Vannacci

    IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control
    |November 10, 2006
    PubMed
    Summary

    The shape of ultrasonic pulses significantly impacts subharmonic emissions from ultrasonic contrast agents (UCA). Smoother pulse shapes can reduce UCA subharmonic generation, demonstrating pulse-dependent nonlinear acoustic behavior.

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    Published on: June 12, 2021

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    Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
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    Multi-timescale Microscopy Methods for the Characterization of Fluorescently-labeled Microbubbles for Ultrasound-Triggered Drug Release
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    Multi-timescale Microscopy Methods for the Characterization of Fluorescently-labeled Microbubbles for Ultrasound-Triggered Drug Release

    Published on: June 12, 2021

    Area of Science:

    • Nonlinear acoustics
    • Ultrasound imaging
    • Biomedical engineering

    Background:

    • Investigating ultrasonic contrast agents (UCA) response to arbitrary-shaped pulses.
    • Focusing on subharmonic emission under varying acoustic pressures and concentrations.
    • Utilizing a custom transmission setup with an arbitrary wave generator and advanced echographic platform (FEMMINA).

    Discussion:

    • Arbitrary-shaped pulses significantly affect subharmonic emission compared to sinusoidal bursts.
    • Gaussian-shaped pulses reduced subharmonic response by up to 30 dB.
    • Composite pulses showed variations up to 21 dB, influenced by acoustic pressure and UCA concentration.

    Key Insights:

    • Transmitted pulse shape is a critical factor influencing subharmonic emission, more so than second harmonic emission.
    • Initial pulse smoothness can inhibit subharmonic generation from UCAs.
    • Subharmonic generation is dependent on pulse amplitude and UCA concentration.

    Outlook:

    • Further research into pulse shaping for optimized UCA response.
    • Exploring nonlinear mechanisms for tailored subharmonic generation.
    • Potential applications in advanced ultrasound diagnostic techniques.