Topic
Acoustic radiation
About: Acoustic radiation is a research topic. Over the lifetime, 1954 publications have been published within this topic receiving 26931 citations. The topic is also known as: geniculotemporal fibres & geniculotemporal fibers.
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TL;DR: In this paper, a theory on the generation mechanism of directional acoustic radiation from a supersonic jet is proposed based on the concept of instability of the shear layer at the boundary of the jet close to the nozzle.
Abstract: A theory on the generation mechanism of directional acoustic radiation from a supersonic jet is proposed. The theory is based on the concept of instability of the shear layer at the boundary of the jet close to the nozzle. Theoretical prediction of the directional wave pattern is found to agree with shadowgraphic observation.
139 citations
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TL;DR: In this paper, the thermo-acoustic mechanism of sound generation by charged particles is analyzed and the general procedure for calculating the fields of such acoustic radiation has been developed, which is in good agreement with the data of experiments on charged-particle beams.
136 citations
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TL;DR: In this article, the spectral emissivity and absorptivity of acoustic radiation were derived for three types of turbulence: free turbulence, turbulence maintained by stirring with spoons and turbulent pseudoconvection.
Abstract: We derive expressions for the spectral emissivity and absorptivity of acoustic radiation by low Mach number
(M ≪ 1) turbulent fluids. The emissivity and absorptivity depend on the manner in which the turbulence is excited. We consider three types of turbulence. The first is free turbulence, that is, turbulence which is not subject to external forces. The second and third examples are special cases of forced turbulence, turbulence maintained by stirring with spoons and turbulent pseudoconvection. Acoustic quadrupoles are the lowest order acoustic multipoles present in free turbulence, and they control both its emissivity and absorptivity. Acoustic dipoles are created in forced turbulence, and they enhance the acoustic emissivity by M^(-2) compared to that of free turbulence. The acoustic absorptivity of forced turbulence is quite subtle. The absorptivity of turbulence which is maintained by stirring is dominated by acoustic dipoles and exceeds that of free turbulence by M^(-2). The dipole absorptivity of turbulent pseudoconvection is reduced by M^2 below that of turbulence maintained by stirring. Thus, the absorptivity of turbulent pseudoconvection is no larger than that of free turbulence. We apply our results to estimate the equilibrium energies of the acoustic modes in a box filled with fluid some of which is turbulent. For both free turbulence and turbulence maintained by stirring, the most highly excited acoustic modes attain energies E ~ Mv^2, where M and v are the typical mass and velocity of an
energy bearing eddy. The quality factors, or Q's, of the modes are larger by M^(-2) in the former case than in
the latter. For turbulent pseudoconvection, the most energetic acoustic modes have equilibrium energies
E ~ Mc^2 , where c is the sound speed. Their Q's are comparable to those of modes in equilibrium with free
turbulence. We evaluate the scattering of acoustic radiation by turbulent fluids. For all types of turbulence, the scattering opacity is smaller by M^3 than the absorptive opacity for frequencies near the peak of the acoustic spectrum. Radiation scattered by free turbulence and turbulent pseudoconvection suffers frequency shifts
Δω ~ ω. The frequency shifts are much smaller, Δω ~ Mω, for radiation scattered by turbulence maintained
by stirring.
We investigate the rate at which nonlinear interactions transfer energy among the acoustic modes. If all of
the fluid in the box is turbulent, this rate is slower, by M^3 for free turbulence, by M^5 for turbulence maintained
by stirring, and by M for turbulent pseudoconvection, than the rate at which the individual acoustic
modes exchange energy with the turbulence. If only a small portion of the fluid is turbulent, the nonlinear mode interactions can be significant, especially for modes in equilibrium with turbulent pseudoconvection. Our results have potential applications to the acoustic radiation in regions of extended turbulence which often arise in nature. In particular, they should prove useful in understanding the excitation of solar oscillations.
133 citations
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14 Apr 2011TL;DR: In this paper, a first acoustic driver has a first direction of maximum acoustic radiation and a second acoustic driver having a second direction of acoustic radiation, where the first and second directions of maximum radiation are not in parallel, and where the audio device employs the first acoustic drivers or the second acoustic drivers in acoustically outputting a sound of a predetermined range of frequencies in response to the orientation of the casing of an audio device relative to the direction of the force of gravity.
Abstract: An audio device incorporates a first acoustic driver having a first direction of maximum acoustic radiation and a second acoustic driver having a second direction of maximum acoustic radiation, where the first and second directions of maximum acoustic radiation are not in parallel, and where the audio device employs the first acoustic driver or the second acoustic driver in acoustically outputting a sound of a predetermined range of frequencies in response to the orientation of the casing of the audio device relative to the direction of the force of gravity.
130 citations
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TL;DR: It is shown that full-image micro-PIV analysis in combination with images of transient particle motion is a powerful tool for experimental studies of acoustic radiation forces and acoustic streaming in microfluidic chambers under piezo-actuation in the MHz range.
Abstract: We show that full-image micro-PIV analysis in combination with images of transient particle motion is a powerful tool for experimental studies of acoustic radiation forces and acoustic streaming in microfluidic chambers under piezo-actuation in the MHz range. The measured steady-state motion of both large 5 um and small 1 um particles can be understood in terms of the acoustic eigenmodes or standing ultra-sound waves in the given experimental microsystems. This interpretation is supported by numerical solutions of the corresponding acoustic wave equation.
126 citations