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Identification of a model for thermoacoustic instabilities in a Rijke tube
IEEE Transactions on Control Systems Technology, 2002In a large class of processes characterized by the presence of a heating source placed in a finite volume, the interaction between the flow field and the heat release mechanism can lead to unsteady fluctuations, known as thermoacoustic instabilities.
Sergio Bittanti +3 more
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Mathematical modeling of a generalized Rijke tube
International Journal of Engineering Science, 1998A mathematical model of unsteady velocity sensitive thermoacoustic interactions in a heated duct (generalized Rijke tube) is developed. The model is constructed in a general way which is capable of employing any linear velocity sensitive thermoacoustic response model. A solution methodology is then constructed based on modal analysis.
Hyun-Gull Yoon +2 more
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Backstepping stabilization of a linearized ODE–PDE Rijke tube model
Automatica, 2018zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Gustavo Artur de Andrade, Daniel Pagano
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Thermoacoustic Instability in a Rijke Tube: Non-Normality and Nonlinearity
13th AIAA/CEAS Aeroacoustics Conference (28th AIAA Aeroacoustics Conference), 2007The role of non-normality and nonlinearity in thermoacoustic interaction in a Rijke tube is investigated in this paper. The heat release rate of the heating element is modeled by a modified form of King’s law. This fluctuating heat release from the heating element is treated as a compact source in the one-dimensional linear model of the acoustic field.
Balasubramanian, Koushik, Sujith, R. I.
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Experiments on heat content inside a Rijke tube with suppression of thermo-acoustics instability
The present work describes the occurrence of thermo-acoustic instability inside a horizontal Rijke tube and its suppression using an open loop active control technique. The Rijke tube is provided with a co-axial pre-mixed gas burner as the source of heat,
Nilaj Deshmukh
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Modeling of Unstable Regimes in a Rijke Tube
5th International Symposium on Fluid Structure Interaction, Aeroelasticity, and Flow Induced Vibration and Noise, 2002In the ducts with mean flows and heat sources, excitation of acoustic eigen modes is possible when unsteady heat release is coupled with pressure perturbations. The simplest device for studying the fundamental principles of thermoacoustic instabilities in the presence of a mean flow is a Rijke tube.
K. I. Matveev, F. E. C. Culick
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The Rijke tube — A thermo-acoustic device
Resonance, 2003The Rijke tube is simply a cylindrical tube with both ends openand a heat source placed inside it. The heat source may be aflame or an electrical heating element. Traditionally, the tube ispositioned vertically on a stand (or even in your hand) and theheat source is introduced from below into the tube (
Shekhar M Sarpotdar +2 more
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Electroacoustic control of Rijke tube instability
Journal of Sound and Vibration, 2017Abstract Unsteady heat release coupled with pressure fluctuation triggers the thermoacoustic instability which may damage a combustion chamber severely. This study demonstrates an electroacoustic control approach of suppressing the thermoacoustic instability in a Rijke tube by altering the wall boundary condition.
Yumin Zhang, Lixi Huang
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One-dimensional model for the Rijke tube
Journal of Fluid Mechanics, 1989We develop a simple model in which longitudinal, compressible, unsteady heat transfer between heater and gas is computed in the small-Mach-number limit. This calculation is used to determine the transfer function of the heater, which plays an important role in the stability limits of the thermoacoustic instability of the Rijke tube.
Nicoli, C., Pelcé, P.
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Active control of the noise from a rijke tube
Journal of Sound and Vibration, 1986Instabilities caused by flames or other heat sources in resonators can be suppressed with a feedback system. It consists of a microphone inside the resonator, a phase-shifter, an amplifier and a loudspeaker at one end of the resonator. The pressure field produced by the loudspeaker changes the boundary conditions at the end of the resonator.
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