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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...
Deriving the Speed of Sound in a Liquid01:09

Deriving the Speed of Sound in a Liquid

As with waves on a string, the speed of sound or a mechanical wave in a fluid depends on the fluid's elastic modulus and inertia. The two relevant physical quantities are the bulk modulus and the density of the material. Indeed, it turns out that the relationship between speed and the bulk modulus and density in fluids is the same as that between the speed and the Young's modulus and density in solids.
The speed of sound in fluids can be derived by considering a mechanical wave propagating...
Sound as Pressure Waves01:17

Sound as Pressure Waves

Sound waves, which are longitudinal waves, can be modeled as the displacement amplitude varying as a function of the spatial and temporal coordinates. As a column of the medium is displaced, its successive columns are also displaced. As the successive displacements differ relatively, a pressure difference with the surrounding pressure is created. The gauge pressure varies across the medium.
The pressure fluctuation depends on the difference in displacements between the successive points in the...
Velocity and Acceleration of a Wave00:51

Velocity and Acceleration of a Wave

A wave propagates through a medium with a constant speed, known as a wave velocity. It is different from the speed of the particles of the medium, which is not constant. In addition, the velocity of the medium is perpendicular to the velocity of the wave. The variable speed of the particles of the medium implies that there must be acceleration associated with it. 
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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...
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: May 22, 2026

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations
06:51

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations

Published on: August 21, 2018

Acoustic particle velocity horns.

Dimitri M Donskoy1, Benjamin A Cray

  • 1Stevens Institute of Technology, Hoboken, New Jersey 07030, USA. ddonskoy@stevens.edu

The Journal of the Acoustical Society of America
|May 8, 2012
PubMed
Summary

Acoustic velocity horns (AVHs) amplify particle velocity for vector sensing, unlike pressure horns. These compact, open-ended devices offer directional amplification, with performance controlled by length, throat radius, and flare rate.

Area of Science:

  • Acoustics
  • Signal Processing
  • Transducer Design

Background:

  • Conventional acoustic horns amplify pressure, limiting their use in vector sensing.
  • Particle velocity amplification is crucial for advanced acoustic applications like vector sensing.

Purpose of the Study:

  • To investigate acoustic velocity horns (AVHs) for particle velocity amplification.
  • To explore AVH suitability for vector sensing applications.
  • To analyze AVH performance independent of overall size relative to acoustic wavelength.

Main Methods:

  • Derivation and analysis of Webster's one-dimensional horn equation for AVHs.
  • Modeling of single conical, exponential, and double-horn configurations.
  • Numerical verification of predicted horn amplification factors.

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Main Results:

  • AVHs provide significant velocity amplification in a compact form factor (much less than one acoustic wavelength).
  • AVH performance is primarily governed by three geometric parameters: length, throat radius, and flare rate.
  • Velocity amplification is largely frequency-independent below a specific resonance region.

Conclusions:

  • Acoustic velocity horns are effective for particle velocity amplification and directional vector sensing.
  • The open-ended configuration is key to AVH functionality, distinguishing them from pressure horns.
  • AVHs offer predictable performance based on geometric design, enabling tailored applications.