1994
DOI: 10.1006/jsvi.1994.1080
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Acoustic Field of a Pulsed Circular Piston

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Cited by 8 publications
(8 citation statements)
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“…In the replica pulse method [20], the diffraction effects for a plane piston are explained intuitively as the result of the edge wave. The edge wave emanates from the abrupt change in surface velocity at the aperture edge and can be avoided by apodizing the aperture.…”
Section: A Transmit Apodization Functionmentioning
confidence: 99%
“…In the replica pulse method [20], the diffraction effects for a plane piston are explained intuitively as the result of the edge wave. The edge wave emanates from the abrupt change in surface velocity at the aperture edge and can be avoided by apodizing the aperture.…”
Section: A Transmit Apodization Functionmentioning
confidence: 99%
“…In the first animation (Online resource 1), containing the pressure field evolution for the largest spot diameter (6.5 mm, flat top) the structure of the transient field can be observed best. In the beginning, it resembles the field of a pulsed circular flat piston [15], consisting of two linearly superimposable contributions: (i) the central planar compressional wave (here, the wavefront is slightly curved to match the curvature of the cornea), propagating inside the cylindrical volume representing the geometrical shadow of the source at the surface and propagating away from the source, and (ii) the so-called edge wave, emanating from the rim of the circular (piston) source in a hemi-toroidal fashion. The outer part of the edge wave has the same polarity (here positive pressure, compression) as the central wave, while the inner portion has the opposite polarity (here negative pressure, rarefaction), consistent with the simplified theory [15].…”
Section: Resultsmentioning
confidence: 99%
“…Again the exact solution cannot be obtained; hence, we cannot make a quantitative evaluation of the results and the qualitative evaluation will demonstrate the correctitude of our results. The proposed approach is solved using the Navier-Stokes equations, where the wall boundary conditions and piston source characteristics for wall-embedded pistons, Equations (15)- (16), and the outflow boundary conditions are handled using the PML and acoustic radiation conditions of Tam and Webb [23], Equations (16) and (18). Next, we study the interference of the waves of three sources when the source is characterized by low frequency (ka = 2) and high frequency (ka = 8).…”
Section: Array Of Baffled Pistonsmentioning
confidence: 99%
“…Wave generation from a vibrating circular piston is a classical acoustic problem, and has been investigated by, among others, Freedmann [18], Lele and Hamilton [19], Cleveland et al [20], Williams [21], Blackstock [22], and Cheong and Lee [12].…”
Section: Introductionmentioning
confidence: 99%