2015
DOI: 10.1016/j.proci.2014.05.053
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A theoretical study of mean azimuthal flow and asymmetry effects on thermo-acoustic modes in annular combustors

Abstract: To cite this version:Michaël Bauerheim, Michel Cazalens, Thierry Poinsot. A theoretical study of mean azimuthal flow and asymmetry effects on thermo-acoustic modes in annular combustors. Proceedings of the Combustion Institute, Elsevier, 2015, vol. 35 (n°3) AbstractThe objective of this paper is to develop an analytical model to capture two symmetry breaking effects controlling the frequency and nature (spinning, standing or mixed) of azimuthal modes appearing in annular chambers: (1) Using two different burn… Show more

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Cited by 60 publications
(45 citation statements)
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“…The frequency gap between the two components is 2M ω n , which is small compared to the pure acoustic frequency ω n . This frequency splitting due to the azimuthal flow has been previously observed experimentally in [16] and predicted from a linear stability analysis of a lumped-element description of the thermoacoustics of an annular combustor [19]. It has to be noted that the phenomenon of frequency splitting does not depend on the model adopted for the flame response.…”
Section: Symmetry Breaking Induced By the Presence Of Mean Swirlsupporting
confidence: 75%
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“…The frequency gap between the two components is 2M ω n , which is small compared to the pure acoustic frequency ω n . This frequency splitting due to the azimuthal flow has been previously observed experimentally in [16] and predicted from a linear stability analysis of a lumped-element description of the thermoacoustics of an annular combustor [19]. It has to be noted that the phenomenon of frequency splitting does not depend on the model adopted for the flame response.…”
Section: Symmetry Breaking Induced By the Presence Of Mean Swirlsupporting
confidence: 75%
“…In previous studies dealing with thermoacoustic instabilities in annular configurations, the time delay between the acoustic field and the heat release rate oscillations has been accounted for in different ways: i) by using the simple n-τ formulation (e.g. [48,19]) and its state-space equivalent [49] for modelling the linear thermoacoustic problem in time and frequency domain, ii) by using measured flame describing functions (e.g. [50,28]) for modelling the nonlinear thermoacoustic problem in frequency domain, and iii) by modelling the flame response to acoustic perturbations with a distribution of time delays [14], or by using state-space representations of experimentally measured FTFs [15,26] for simulating the nonlinear thermoacoustic problem in time domain.…”
Section: Time-delayed Thermoacoustic Feedbackmentioning
confidence: 99%
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“…Firstly, a non-zero U θ makes one of the two spinning modes rotate faster and the other slower, and makes standing modes slowly rotate with pressure and velocity nodes moving at the speed of the mean azimuthal flow. See for example Wolf et al (2010) for numerical evidence and a discussion, and refer to Bauerheim et al (2014), Bauerheim, Cazalens & Poinsot (2015) for a detailed analysis of this first effect of U θ in a linear framework. Secondly, a non-zero U θ bends the flames in the azimuthal direction, orthogonally to the burner's axis.…”
Section: Problem Geometrymentioning
confidence: 99%