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Thermoacoustic instability – a dynamical system and time domain analysis

Published online by Cambridge University Press:  24 July 2014

Taraneh Sayadi*
Affiliation:
Department of Mathematics, Imperial College London, London SW7 2AZ, UK
Vincent Le Chenadec
Affiliation:
CNRS - UPR 288, 92295, Laboratoire EM2C, Châtenay-Malabry, France École Centrale Paris, 92295 Châtenay-Malabry, France
Peter J. Schmid
Affiliation:
Department of Mathematics, Imperial College London, London SW7 2AZ, UK
Franck Richecoeur
Affiliation:
CNRS - UPR 288, 92295, Laboratoire EM2C, Châtenay-Malabry, France École Centrale Paris, 92295 Châtenay-Malabry, France
Marc Massot
Affiliation:
CNRS - UPR 288, 92295, Laboratoire EM2C, Châtenay-Malabry, France École Centrale Paris, 92295 Châtenay-Malabry, France Fédération de Mathématiques de l’École Centrale Paris, CNRS - FR 3487, 92295 Châtenay-Malabry, France
*
Email address for correspondence: sayadi@ladhyx.polytechnique.fr

Abstract

This study focuses on the Rijke tube problem, which includes features relevant to the modelling of thermoacoustic coupling in reactive flows: a compact acoustic source, an empirical model for the heat source and nonlinearities. This thermoacoustic system features both linear and nonlinear flow regimes with complex dynamical behaviour. In order to synthesize accurate time series, we tackle this problem from a numerical point of view, and start by proposing a dedicated solver designed for dealing with the underlying stiffness – in particular, the retarded time and the discontinuity at the location of the heat source. Stability analysis is performed on the limit of low-amplitude disturbances by using the projection method proposed by Jarlebring (PhD thesis, Technische Universität Braunschweig, 2008), which alleviates the problems arising from linearization with respect to the retarded time. The results are then compared with the analytical solution of the undamped system and with the results obtained from Galerkin projection methods commonly used in this setting. This analysis provides insight into the consequences of the various assumptions and simplifications that justify the use of Galerkin expansions based on the eigenmodes of the unheated resonator. We demonstrate that due to the presence of a discontinuity in the spatial domain, the eigenmodes in the heated case predicted by using Galerkin expansion show spurious oscillations resulting from the Gibbs phenomenon. Finally, time series in the fully nonlinear regime, where a limit cycle is established, are analysed and dominant modes are extracted. By comparing the modes of the linear regime to those of the nonlinear regime, we are able to illustrate the mean-flow modulation and frequency switching, which appear as the nonlinearities become significant and ultimately affect the form of the limit cycle. Analysis of the saturated limit cycles shows the presence of higher-frequency modes, which are linearly stable but become significant through nonlinear growth of the signal. This bimodal effect is not exhibited when the coupling between different frequencies is not accounted for. In conclusion, a dedicated solver for capturing thermoacoustic instability is proposed and methods for analysing linear and nonlinear regions of the resulting time series are introduced.

Type
Papers
Copyright
© 2014 Cambridge University Press 

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References

Balasubramanian, K. & Sujith, R. I. 2008 Thermoacoustic instability in a Rijke tube: non-normality and nonlinearity. Phys. Fluids 20, 044103.CrossRefGoogle Scholar
Boudy, F., Durox, D., Schuller, T. & Candel, S. 2013 Analysis of limit cycles sustained by two modes in the flame describing function framework. C. R. Méc 341 (1), 181190.CrossRefGoogle Scholar
Canuto, C., Hussaini, M. Y., Quarteroni, A. & Zang, T. A. 2007 Spectral Methods: Evolution to Complex Geometries and Applications to Fluid Dynamics. Springer.CrossRefGoogle Scholar
Culick, F. E. C. 1988 Combustion instabilities in liquid-fuelled propulsion system – an overview. AGARD CP 450, 173.Google Scholar
Dowling, A. P. 1995 The calculation of thermoacoustic oscillations. J. Sound Vib. 180 (4), 557581.CrossRefGoogle Scholar
Dowling, A. P. 1997 Nonlinear self-excited oscillations of a ducted flame. J. Fluid Mech. 346, 271290.CrossRefGoogle Scholar
Engelborghs, K.2000 DDE-BIFTOOL: a Matlab package for bifurcation analysis of delay differential equations. Tech. Rep., Department of Computer Science, Katholieke Universiteit Leuven.Google Scholar
Fedkiw, R. P., Aslam, T., Merriman, B. & Osher, S. 1999 A non-oscillatory Eulerian approach to interfaces in multimaterial flows (the ghost fluid method). J. Comput. Phys. 152 (2), 457492.CrossRefGoogle Scholar
Guglielmi, N. & Hairer, E. 2001 Implementing Radau IIA methods for stiff delay differential equations. Computing 67, 112.CrossRefGoogle Scholar
Heckl, M. A. 1990 Nonlinear acoustic effects in the Rijke tube. Acustica 72, 6371.Google Scholar
Heckl, M. A. & Howe, M. S. 2007 Stability analysis of the Rijke tube with a Green’s function approach. J. Sound Vib. 305 (4), 672688.CrossRefGoogle Scholar
Howe, M. S. 1998 Acoustics of Fluid–Structure Interactions. Cambridge University Press.CrossRefGoogle Scholar
Jarlebring, E.2008 The spectrum of delay differential equations: numerical methods, stability and perturbation. PhD thesis, Technische Universität Carolo-Wilhelmina zu Braunschweig.Google Scholar
Juniper, M. P. 2011 Triggering in the horizontal Rijke tube: non-normality, transient growth and bypass transition. J. Fluid Mech. 667, 272308.CrossRefGoogle Scholar
King, L. V. 1914 On the convection of heat from small cylinders in a stream of fluid. Phil. Trans. R. Soc. A 214, 373432.Google Scholar
Lighthill, M. J. 1954 The response of laminar skin friction and heat transfer to fluctuations in the stream velocity. Proc. R. Soc. A 224, 123.Google Scholar
Magri, L. & Juniper, M. P. 2013 Sensitivity analysis of a time-delayed thermoacoustic system via an adjoint-based approach. J. Fluid Mech. 719, 183202.CrossRefGoogle Scholar
Mariappan, S. & Sujith, R. I. 2011 Modelling nonlinear thermoacoustic instability in an electrically heated Rijke tube. J. Fluid Mech. 680, 511533.CrossRefGoogle Scholar
Mariappan, S., Sujith, R. & Schmid, P.2011 Non-normality of thermoacoustic interactions: an experimental investigation. In 47th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit, article no. 2011-5555. Aerospace Research Central.CrossRefGoogle Scholar
Matveev, K.2003 Themoacoustic instabilities in Rijke tube: experiments and modelling. PhD thesis, California Institute of Technology.Google Scholar
Matveev, K. I. & Culick, F. E. C. 2003a A model for combustion instability involving vortex shedding. Combust. Sci. Technol. 175 (6), 10591083.CrossRefGoogle Scholar
Matveev, K. I. & Culick, F. E. C. 2003b A study of the transition to instability in a Rijke tube with axial temperature gradient. J. Sound Vib. 264, 689706.CrossRefGoogle Scholar
Nagarajan, S., Lele, S. K. & Ferziger, J. H. 2003 A robust high-order compact method for large eddy simulation. J. Comput. Phys. 191 (2), 392419.CrossRefGoogle Scholar
Poinsot, T. & Veynante, D. 2005 Theoretical and Numerical Combustion. R. T. Edwards.Google Scholar
Raun, R. L., Beckstead, M. W., Finlinson, J. C. & Brooks, K. P. 1993 A review of Rijke tube, Rijke burners and related devices. Prog. Energy Combust. Sci. 19, 313364.CrossRefGoogle Scholar
Rayleigh, L. 1896 Theory of Sound. Macmillan and Co.Google Scholar
Rijke, P. L. 1859 On the vibration of the air in a tube open at both ends. Phil. Mag. 17, 419422.CrossRefGoogle Scholar
Sayadi, T., Schmid, P. J., Nichols, J. W. & Moin, P.2013 Dynamic mode decomposition of controlled $h$ - and $k$ -type transitions. Tech. Rep., Annual Research Briefs 2013, pp. 189–200. Center for Turbulence Research, Stanford University.Google Scholar
Schmid, P. J. 2010 Dynamic mode decomposition of numerical and experimental data. J. Fluid Mech. 656, 528.CrossRefGoogle Scholar
Schuller, T., Durox, D. & Candel, S. 2003 A unified model for the prediction of laminar flame transfer functions: comparisons between conical and ${V}$ -flame dynamics. Combust. Flame 134, 2134.CrossRefGoogle Scholar
Selimefendigil, F., Sujith, R. I. & Polifke, W. 2011 Identification of heat transfer dynamics for non-modal analysis of thermoacoustic stability. Appl. Maths Comput. 217 (11), 51345150.CrossRefGoogle Scholar
Sterling, J. D. & Zukoski, E. E. 1991 Nonlinear dynamics of laboratory combustor pressure oscillations. Combust. Sci. Technol. 77 (4–6), 225238.CrossRefGoogle Scholar
Subramanian, P., Mariappan, S., Sujith, R. I. & Wahi, P. 2010 Bifurcation analysis of thermoacoustic instability in a horizontal Rijke tube. Intl J. Spray Combust. Dyn. 2 (4), 325356.CrossRefGoogle Scholar
Subramanian, P., Sujith, R. I. & Wahi, P. 2013 Subcritical bifurcation and bistability in thermoacoustic systems. J. Fluid Mech. 715, 210238.CrossRefGoogle Scholar
Williams, F. A. 1994 Combustion Theory, 2nd edn. Westview Press.Google Scholar