2013
DOI: 10.1016/j.crme.2012.10.020
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Large-Eddy Simulation of combustion instabilities in a variable-length combustor

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Cited by 97 publications
(60 citation statements)
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References 33 publications
(37 reference statements)
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“…They note that the chemistry is not fast enough to anchor the flame at the injection point and the flame is instead anchored at the dump plane by the hot burnt gases in the recirculation region. 21 Guézennec et al showed that in an unstable 4.75 in case the triple flame forms at the backstep and is extinguished when it hits the wall, the time of this movement is linked to the first longitudinal mode. 22 Results in this work find that the mechanism at play in the unstable case is more complex and dynamic.…”
Section: B Baroclinic Torquementioning
confidence: 98%
See 1 more Smart Citation
“…They note that the chemistry is not fast enough to anchor the flame at the injection point and the flame is instead anchored at the dump plane by the hot burnt gases in the recirculation region. 21 Guézennec et al showed that in an unstable 4.75 in case the triple flame forms at the backstep and is extinguished when it hits the wall, the time of this movement is linked to the first longitudinal mode. 22 Results in this work find that the mechanism at play in the unstable case is more complex and dynamic.…”
Section: B Baroclinic Torquementioning
confidence: 98%
“…The existence of a triple flame structure in the combustor was also suggested as a key element in the instability mechanism. 21 Guézennec et al provided results of an unstable 4.75 in configuration showing the movement of a triple point occurred at the same frequency as the the first longitudinal mode. 22 To date no simulations of stable operating conditions have been published in the literature.…”
mentioning
confidence: 93%
“…As a consequence, the eigenmodes of the chamber can change and their stability too. Adiabatic and non-adiabatic con gurations exhibit different stability regions: this is easily observed in simulations where changing the wall heat transfer condition from adiabatic to isothermal is suf cient to trigger or damp modes [106,107] . This is a rather obvious effect due to changes in sound speeds and ame shapes which will not be discussed here.…”
Section: The Effects Of Wall Temperaturesmentioning
confidence: 99%
“…Differences in frequency or amplitude may occur when the temperature field and the FTF in the simulation only partially match those in the experiment, but the simulation can usually be used for further investigation of the thermoacoustic mode. There are numerous studies of combustion instabilities that illustrate that LES with adiabatic walls can show a reasonable agreement with experiments: the study on a lean-premixed swirl combustor by Huang et al [8] , the LES-studies on the PRECCIN-STA configuration [9][10][11] , the massively parallel LES of a realistic helicopter combustion chamber by Wolf et al [12] , LESs of model rocket combustors (Garby et al [13] , Urbano et al [14] ) or the LESstudies of bluff-body stabilized flames by Li et al [15] and Ghani et al [16] .…”
Section: Introductionmentioning
confidence: 99%
“…• Type 1: Adiabatic walls: the majority of recent LESs simply consider the walls to be adiabatic [8][9][10][11][12][13][14][15][16][19][20][21][22] .…”
Section: Introductionmentioning
confidence: 99%