Identifying optimal location for control of thermoacoustic instability through statistical analysis of saddle point trajectories
We propose a framework of Lagrangian Coherent Structures (LCS) to enable passive open-loop control of tonal sound generated during thermoacoustic instability. Experiments were performed in a laboratory-scale bluff-body stabilized turbulent combustor in the state of thermoacoustic instability. We use...
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Main Authors | , , , , , , |
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Format | Journal Article |
Language | English |
Published |
27.08.2023
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Subjects | |
Online Access | Get full text |
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Summary: | We propose a framework of Lagrangian Coherent Structures (LCS) to enable
passive open-loop control of tonal sound generated during thermoacoustic
instability. Experiments were performed in a laboratory-scale bluff-body
stabilized turbulent combustor in the state of thermoacoustic instability. We
use dynamic mode decomposition (DMD) on the flow-field to identify dynamical
regions where the acoustic frequency is dominant. We find that the separating
shear layer from the backward-facing step of the combustor envelops a
cylindrical vortex in the outer recirculation zone (ORZ), which eventually
impinging on the top wall of the combustor during thermoacoustic instability.
We track the saddle points in this shear layer emerging from the backward
facing step over several acoustic cycles. A passive control strategy is then
developed by injecting a steady stream of secondary air targeting the
identified optimal location where the saddle points spend a majority of their
time in a statistical sense.
After implementing the control action, the resultant flow-field is also
analysed using LCS to understand the key differences in flow dynamics. We find
that the shear layer emerging from the dump plane is deflected in a direction
almost parallel to the axis of the combustor after the control action. This
deflection in turn prevents the shear layer from enveloping the vortex and
impinging on the combustor walls, resulting in a drastic reduction in the
amplitude of the sound produced. |
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DOI: | 10.48550/arxiv.2308.14261 |