2007
DOI: 10.1016/j.jsv.2006.09.002
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Sesquipoles in aeroacoustics

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Cited by 3 publications
(5 citation statements)
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“…Chapman has proposed a transfer function between incoming gusts (i.e. the source) and flowinduced noise [26,27] (which can be measured) by using the Wiener-Hopf technique. Munt [11] and Gabarb & Astley [6] have proposed the forward model for duct acoustic problems by using the Wiener-Hopf technique, which is adopted in this work to (1) theoretically clarify the inherent principle of the forward model and to (2) rapidly provide a big volume of high-fidelity data for machine learning.…”
Section: Preliminary Knowledge (A) Statement Of the Problemsmentioning
confidence: 99%
See 1 more Smart Citation
“…Chapman has proposed a transfer function between incoming gusts (i.e. the source) and flowinduced noise [26,27] (which can be measured) by using the Wiener-Hopf technique. Munt [11] and Gabarb & Astley [6] have proposed the forward model for duct acoustic problems by using the Wiener-Hopf technique, which is adopted in this work to (1) theoretically clarify the inherent principle of the forward model and to (2) rapidly provide a big volume of high-fidelity data for machine learning.…”
Section: Preliminary Knowledge (A) Statement Of the Problemsmentioning
confidence: 99%
“…More specifically, the Wiener-Hopf method will be tried in this work to guide (supervise) neural networks to learn transfer functions between inputs (wave sources) and outputs (scattered wave fields). Chapman has studied the transfer function between incoming gusts and flowinduced noise sources [26,27] by using the Wiener-Hopf technique. In essentially the same way, the Wiener-Hopf technique can be used to produce the transfer function between fan noise sources and sensor measurements of the scattered sound waves.…”
Section: Introductionmentioning
confidence: 99%
“…The pressure field may be called the three-dimensional supersonic edgelet, since it is the sound produced by an individual point on the leading edge. This field is much simpler than the subsonic three-dimensional edgelet, given as a contour integral in [8], where it is referred to as the edgelet function E 1 ; and it is slightly simpler than the two-dimensional supersonic edgelet given in [10]. Expression (7) applies in the Mach cone |ȳ 2 +z 2 | 1/2 <x emanating downstream from the origin; elsewhere the field is zero.…”
Section: The Delta-function Gustmentioning
confidence: 99%
“…In its general form, this is a problem of some complexity, especially when account is taken of such important matters as the blade angle of attack, thickness, and camber. Substantial progress has been made over many years in related subsonic problems, of which representative work in two dimensions is [1][2] and in three dimensions is [3][4][5][6][7][8]. For the supersonic problem, the amount of published work is smaller, but important two-dimensional fields have been determined in [9][10][11], and three-dimensional fields in [12][13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…The maximum pressure is especially great when the interaction between gust and edge takes place at high speed, as in modern aeroengines. For a subsonic edge, a large body of theory has been worked out, with many three-dimensional impulsive sound fields calculated exactly [1][2][3][4][5][6][7][8][9]. For a supersonic edge, some three-dimensional impulsive fields have been calculated in [10][11][12][13], and a general theory of the generation of such fields is given in [14].…”
Section: Introductionmentioning
confidence: 99%