2016
DOI: 10.1016/j.combustflame.2016.01.015
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Propagation and generation of acoustic and entropy waves across a moving flame front

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Cited by 71 publications
(31 citation statements)
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References 27 publications
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“…However, downstream of the flame, the density contains the influence of both acoustic and entropy waves through Gibbs' relation (26). Small entropy inhomogeneities appear in the downstream region because the acoustic fluctuations change the temperature upstream, while the mean heat release is constant in this model [212]. The entropy spots are accelerated through the nozzle and converted into indirect acoustic waves.…”
Section: Sensitivity To Passive Devicesmentioning
confidence: 93%
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“…However, downstream of the flame, the density contains the influence of both acoustic and entropy waves through Gibbs' relation (26). Small entropy inhomogeneities appear in the downstream region because the acoustic fluctuations change the temperature upstream, while the mean heat release is constant in this model [212]. The entropy spots are accelerated through the nozzle and converted into indirect acoustic waves.…”
Section: Sensitivity To Passive Devicesmentioning
confidence: 93%
“…Therefore, the heat source creates a discontinuity in the mean flow, and jump conditions can be derived by the integral form of the governing equations, accordingly. When linearized, the jump conditions at the nondimensional flame location x f read [212] ρ ū +ρu…”
Section: Helmholtz Equationmentioning
confidence: 99%
“…Recent work for highly simplified (1-D planar and zero Mach number) flames has suggested that entropy disturbances are only generated in the presence of equivalence ratio fluctuations [25, 26]. This paper investigates the transport of entropy perturbations in realistic combustor flow-fields, and does not address the issue of entropy disturbance generation itself.…”
Section: Introductionmentioning
confidence: 99%
“…We are thus left with the relation _ q / v, which substituted into equation (28) yields a source term analog to the classical Rayleigh source term @E=@t / _ q p F . The phenomenon of a flame at rest producing fluctuations in energy is referred to as ''the classical paradox of thermoacoustics'' by Bauerheim et al 54 and is also explained by Strobio Chen et al 55 The above described mechanism of creating fluctuations in heat release rate is fundamentally different from the fluctuations in heat release rate resulting from an active flame as described in The flame subsystem …”
Section: The Output Defines the Perspectivementioning
confidence: 99%