2021
DOI: 10.1016/j.jsv.2021.116437
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Acoustic absorption and generation in ducts of smoothly varying area sustaining a mean flow and a mean temperature gradient

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Cited by 5 publications
(3 citation statements)
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“…Because the flow is assumed to be weakly reacting, non-conductive and adiabatic, we neglect the mean-flow heat transfer. For modelling the effect of heat transfer, the reader is referred to Yeddula, Gaudron & Morgans (2021) and Yeddula, Guzmán-Iñigo & Morgans (2022). To close the linear equations, we linearize the Gibbs equation (2.10) and take the material derivative and combine the first-order terms to yield where is the perturbation to the heat-capacity ratio, which is a function of the species mass fractions, , only.…”
Section: Mathematical Modelmentioning
confidence: 99%
“…Because the flow is assumed to be weakly reacting, non-conductive and adiabatic, we neglect the mean-flow heat transfer. For modelling the effect of heat transfer, the reader is referred to Yeddula, Gaudron & Morgans (2021) and Yeddula, Guzmán-Iñigo & Morgans (2022). To close the linear equations, we linearize the Gibbs equation (2.10) and take the material derivative and combine the first-order terms to yield where is the perturbation to the heat-capacity ratio, which is a function of the species mass fractions, , only.…”
Section: Mathematical Modelmentioning
confidence: 99%
“…Yeddula & Morgans [30] derived solutions for the acoustic field in one-dimensional ducts with both arbitrarily varying cross-sectional area and temperature gradient. Further studies investigated the effects of mean flow and mean temperature gradient on acoustic absorption and generation within the duct [31]. Rani & Rani [32] derived two approximate WKB solutions for quasi-onedimensional ducts with arbitrary mean properties and mean flow, while the nonlinear temporal dynamics of acoustic oscillations was discussed by Basu [33].…”
Section: Introductionmentioning
confidence: 99%
“…Much attention has been paid to the distributed properties of unsteady heat sources [20,26,27]. However, even when the heat source is purely steady, steady temperature gradients and mean flow acceleration mean that acoustic waves can be amplified or attenuated by interaction with entropy waves [28][29][30][31][32]. This acoustic-entropy coupling consequently plays a crucial role in determining the frequencies and growth rates of thermoacoustic modes in the presence of temperature gradients [33] and mean flows [34,35].…”
Section: Introductionmentioning
confidence: 99%