1971
DOI: 10.1016/0022-460x(71)90381-6
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Acoustic energy in non-uniform flows

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Cited by 270 publications
(94 citation statements)
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“…The termination plane is assumed to be non-reflecting, and this is forced by requiring that reflected modal amplitudes vanish. Acoustic power is computed at the source plane and termination plane based on acoustic potential modal amplitudes by using the definition of Morfey 13 , valid in the case of irrotational acoustic perturbations on irrotational mean flow. In addition, acoustic power is computed at any specified axial location using the Morfey definition, but by post-processing the acoustic potential.…”
Section: A Fem Model For Duct Propagationmentioning
confidence: 99%
“…The termination plane is assumed to be non-reflecting, and this is forced by requiring that reflected modal amplitudes vanish. Acoustic power is computed at the source plane and termination plane based on acoustic potential modal amplitudes by using the definition of Morfey 13 , valid in the case of irrotational acoustic perturbations on irrotational mean flow. In addition, acoustic power is computed at any specified axial location using the Morfey definition, but by post-processing the acoustic potential.…”
Section: A Fem Model For Duct Propagationmentioning
confidence: 99%
“…(7), (28), (32) and taking the limit u 2 -0 while the product u 2ŝ remains finite [11], one obtains the following expression for the entropy produced by the flame at x ¼ x f :…”
Section: Methods I : Truncated Analytical Thermoacoustic Model At M A0mentioning
confidence: 99%
“…This is also the case here: Firstly, |f | 2 + |g| 2 is equal to the density of acoustic energy [32]. Secondly, as the Riemann invariants f and g propagate along the duct, summing over the coefficients (f h,0 , ..., g c,C+Q ) of the state vector (i.e.…”
Section: Non-normal Effectsmentioning
confidence: 97%