1975
DOI: 10.1016/b978-0-12-477911-2.50007-7
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Physical Acoustics and the Method of Matched Asymptotic Expansions

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Cited by 24 publications
(16 citation statements)
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“…Due to this singularity, if not integrable, the Fourier transformation of the pressure in (26) becomes too singular to be interpreted normally and diverges for r → ∞. When we consider the incompressible problem as an inner problem of a larger compressible problem, as in [15,4,16,17], this divergent behaviour disappears as it changes into an outward radiating acoustic wave. The inverse Fourier transform for pressure p is then calculated by splitting off the singular part and interpreting the singular integral in generalised sense [18,19,8].…”
Section: Wiener-hopf Proceduresmentioning
confidence: 99%
“…Due to this singularity, if not integrable, the Fourier transformation of the pressure in (26) becomes too singular to be interpreted normally and diverges for r → ∞. When we consider the incompressible problem as an inner problem of a larger compressible problem, as in [15,4,16,17], this divergent behaviour disappears as it changes into an outward radiating acoustic wave. The inverse Fourier transform for pressure p is then calculated by splitting off the singular part and interpreting the singular integral in generalised sense [18,19,8].…”
Section: Wiener-hopf Proceduresmentioning
confidence: 99%
“…Note that this equation has a small parameter multiplied by the highest derivative in the X-direction, suggesting a singular perturbation problem [4,18,19,20] with boundary layers in X.…”
Section: The Classical Problemmentioning
confidence: 99%
“…The solution is determined by a source at entrance plane x = 0, and radiation conditions for x → ∞. Other conditions, like a reflecting impedance plane at some exit plane x = L (e.g., modeling a radiating open end [5] or a slit in the wall [4]), are also possible, but they do not essentially alter the present analysis.…”
Section: The Classical Problemmentioning
confidence: 99%
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