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Dynamics of robust structures in turbulent swirling reacting flows

Published online by Cambridge University Press:  08 March 2017

S. Roy*
Affiliation:
Spectral Energies, LLC, 5100 Springfield Street, Suite 301, Dayton, OH 45431, USA
T. Yi
Affiliation:
Spectral Energies, LLC, 5100 Springfield Street, Suite 301, Dayton, OH 45431, USA
N. Jiang
Affiliation:
Spectral Energies, LLC, 5100 Springfield Street, Suite 301, Dayton, OH 45431, USA
G. H. Gunaratne*
Affiliation:
Department of Physics, University of Houston, Houston, TX 77204, USA
I. Chterev
Affiliation:
Ben T. Zinn Combustion Laboratory, Georgia Institute of Technology, Atlanta, GA 30332, USA
B. Emerson
Affiliation:
Ben T. Zinn Combustion Laboratory, Georgia Institute of Technology, Atlanta, GA 30332, USA
T. Lieuwen*
Affiliation:
Ben T. Zinn Combustion Laboratory, Georgia Institute of Technology, Atlanta, GA 30332, USA
A. W. Caswell
Affiliation:
Aerospace Systems Directorate, Air Force Research Laboratory, Wright-Patterson AFB, OH 45433, USA
J. R. Gord*
Affiliation:
Aerospace Systems Directorate, Air Force Research Laboratory, Wright-Patterson AFB, OH 45433, USA

Abstract

High-speed synchronized stereo particle-imaging velocimetry and OH planar laser-induced fluorescence (PIV/OH-PLIF) measurements are performed on multiple $R{-}\unicode[STIX]{x1D703}$ planes downstream of a high-Reynolds-number swirling jet. Dynamic-mode decomposition (DMD) – a frequency-resolved data-reduction technique – is used to identify and characterize recurrent flow structures. Illustrative results are presented in a swirling flow field for two cases – the nominal flow dynamics and where self-excited combustion driven oscillations provide strong axisymmetric narrowband forcing of the flow. The robust constituent of the nominal reacting swirl flow corresponds to a helical shear-layer disturbance at a Strouhal number ($St$) of ${\sim}0.30$, $St=fD/U_{0}$, where $f$, $D$ and $U_{0}$ denote the precessing vortex core (PVC) frequency (${\sim}800~\text{Hz}$), the swirler exit diameter (19 mm) and the bulk velocity at the swirler exit ($50~\text{m}~\text{s}^{-1}$) respectively. Planar projections of the PVC reveal a pair of oscillating skew-symmetric regions of velocity, vorticity and OH-PLIF intensity that rotate in the same direction as the mean tangential flow. During combustion instabilities, the large-amplitude acoustics-induced axisymmetric forcing of the flow results in a fundamentally different flow response dominated by a nearly axisymmetric disturbance and almost complete suppression of the large-scale helical shear-layer disturbances dominating the nominal flow. In addition, reverse axial flows around the centreline are significantly reduced. Time traces of the robust constituent show reverse axial flows around the centreline and negative axial vorticity along the inner swirling shear layer when the planar velocity is in the same direction as the mean tangential flow. For both stable and unstable combustion, recurrent flow structures decay rapidly downstream of the air swirler, as revealed by the decreasing amplitude of the velocity, axial vorticity and OH-PLIF intensity.

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Papers
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© Cambridge University Press 2017. This is a work of the U.S. Government and is not subject to copyright protection in the United States. 

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