2015
DOI: 10.2514/1.j053230
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Two Types of Frequency-Domain Acoustic-Velocity Formulations for Rotating Thickness and Loading Sources

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Cited by 18 publications
(12 citation statements)
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“…Noise generated by aircraft, fans and others has great influence on the aeroacoustic research (Polacsek et al 1999; Greenwood and Schmitz 2014; Kingan 2014; Johnson 1980; Mao et al 2015). In these applications, the direct sound field and scattering effect are always considered to assess the acoustic impact of sound sources (Mouille 1970, 1986; Lowson 2015).…”
Section: Introductionmentioning
confidence: 99%
“…Noise generated by aircraft, fans and others has great influence on the aeroacoustic research (Polacsek et al 1999; Greenwood and Schmitz 2014; Kingan 2014; Johnson 1980; Mao et al 2015). In these applications, the direct sound field and scattering effect are always considered to assess the acoustic impact of sound sources (Mouille 1970, 1986; Lowson 2015).…”
Section: Introductionmentioning
confidence: 99%
“…To obtain acoustic pressure gradient formulations, the gradient operation is performed to Eqs. (18)(19)(20), yielding…”
Section: A Convective Fw-h Equation and Its Time-domain Solutionmentioning
confidence: 99%
“…When solving acoustic scattering problems, the key aspect is obtaining the acoustic velocity on the scattering surface to serve as the boundary condition. Recently, Ghorbaniasl et al [19] suggested the analytic formulations V1 and V1A for calculating the acoustic velocity directly in the time domain, whereas the counterpart in the frequency domain was proposed by Mao et al [20]. Given that the direct derivation of the acoustic velocity involves heavy algebraic manipulations, the acoustic pressure gradient can also be used as the boundary condition because it is related to the acoustic velocity through the acoustic velocity potential [21].…”
mentioning
confidence: 99%
“…Ghorbaniasl et al [19] developed time-domain acoustic velocity formulations for monopole and dipole sources in arbitrary motion, and Mao et al [20] deduced frequency-domain acoustic velocity formulations for rotating monopole and dipole sources with a constant angular speed. After that, acoustic intensity fields around sources [21] and scattering boundaries [22,23] were visualized to illustrate the propagation of acoustic energy.…”
Section: Introductionmentioning
confidence: 99%