Abstract
A premixed ducted flame, burning in the wake of a bluff-body flame-holder, is
considered. For such a flame, interaction between acoustic waves and unsteady
combustion can lead to self-excited oscillations. The concept of a time-invariant
turbulent flame speed is used to develop a kinematic model of the response of the flame
to flow disturbances. Variations in the oncoming flow velocity at the flame-holder
drive perturbations in the flame initiation surface and hence in the instantaneous rate
of heat release. For linear fluctuations, the transfer function between heat release and
velocity can be determined analytically from the model and is in good agreement
with experiment across a wide frequency range. For nonlinear fluctuations, the model
reproduces the flame surface distortions seen in schlieren films.Coupling this kinematic flame model with an analysis of the acoustic waves generated
in the duct by the unsteady combustion enables the time evolution of disturbances
to be calculated. Self-excited oscillations occur above a critical fuel–air ratio.
The frequency and amplitude of the resulting limit cycles are in satisfactory agreement
with experiment. Flow reversal is predicted to occur during part of the limit-cycle
oscillation and the flame then moves upstream of the flame-holder, just as in experimental
visualizations. The main nonlinearity is identified in the rate of heat release,
which essentially ‘saturates’ once the amplitude of the velocity fluctuation exceeds
its mean. We show that, for this type of nonlinearity, describing function analysis can
be used to give a good estimate of the limit-cycle frequency and amplitude from a
quasi-nonlinear theory.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
337 articles.
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