2009
DOI: 10.1016/j.combustflame.2009.05.011
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Thermoacoustic limit cycles in a premixed laboratory combustor with open and choked exits

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Cited by 82 publications
(72 citation statements)
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“…Further, the essential physics of thermoacoustic instabilities are not entirely understood [6,7]. This is mostly due to the complexities involved in the interactions between premixed flames and sound waves [9,10] and, to some extent, the effects of system boundaries [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…Further, the essential physics of thermoacoustic instabilities are not entirely understood [6,7]. This is mostly due to the complexities involved in the interactions between premixed flames and sound waves [9,10] and, to some extent, the effects of system boundaries [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…Combustion response transfer functions, or §ame describing functions (FDF), describe the magnitude and phase of heat release as a function of local unsteady pressure/velocity. They have been constructed from measurements of pressure/velocity and CH * chemiluminescence, used to approximate heat release [7]. Low-amplitude §uctuations tend to have a linear response in magnitude, which concurs with the use of linear input growth rates in classical models [5,8].…”
Section: Flame Describing Functionsmentioning
confidence: 99%
“…However, the combustion response at high-amplitude §uctua-tions reaches a saturation level, which (in conjunction with increased acoustic damping) allows the development of limit cycle behavior. The shift to nonlinear behavior has generally been linked to unsteady amplitude, Reynolds number, equivalence ratio, and forcing frequency [7].…”
Section: Flame Describing Functionsmentioning
confidence: 99%
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