Weakly nonlinear modelling of a forced turbulent axisymmetric wake
File(s)
Author(s)
Rigas, G
Morgans, AS
Morrison, JF
Type
Journal Article
Abstract
A theory is presented where the weakly nonlinear analysis of laminar g
lobally unstable
flows in the presence of external forcing is extended to the turbu
lent regime. The analysis
is demonstrated and validated using experimental results of an axis
ymmetric bluff body
wake at high Reynolds numbers,
Re
D
∼
1
.
88
×
10
5
, where forcing is applied using a
Zero-Net-Mass-Flux actuator located at the base of the blunt bo
dy. In this study we
focus on the response of antisymmetric coherent structures wit
h azimuthal wavenumbers
m
=
±
1 at a frequency
St
D
= 0
.
2, responsible for global vortex shedding. We found
experimentally that axisymmetric forcing (
m
= 0) couples nonlinearly with the global
shedding mode when the flow is forced at twice the shedding frequen
cy, resulting in
parametric subharmonic resonance through a triadic interaction b
etween forcing and
shedding. We derive simple weakly nonlinear models from the phase-av
eraged Navier-
Stokes equations and show that they capture accurately the obs
erved behaviour for
this type of forcing. The unknown model coefficients are obtained e
xperimentally by
producing harmonic transients. This approach should be applicable in
a variety of
turbulent flows to describe the response of global modes to forcin
g.
lobally unstable
flows in the presence of external forcing is extended to the turbu
lent regime. The analysis
is demonstrated and validated using experimental results of an axis
ymmetric bluff body
wake at high Reynolds numbers,
Re
D
∼
1
.
88
×
10
5
, where forcing is applied using a
Zero-Net-Mass-Flux actuator located at the base of the blunt bo
dy. In this study we
focus on the response of antisymmetric coherent structures wit
h azimuthal wavenumbers
m
=
±
1 at a frequency
St
D
= 0
.
2, responsible for global vortex shedding. We found
experimentally that axisymmetric forcing (
m
= 0) couples nonlinearly with the global
shedding mode when the flow is forced at twice the shedding frequen
cy, resulting in
parametric subharmonic resonance through a triadic interaction b
etween forcing and
shedding. We derive simple weakly nonlinear models from the phase-av
eraged Navier-
Stokes equations and show that they capture accurately the obs
erved behaviour for
this type of forcing. The unknown model coefficients are obtained e
xperimentally by
producing harmonic transients. This approach should be applicable in
a variety of
turbulent flows to describe the response of global modes to forcin
g.
Date Issued
2017-02-09
Date Acceptance
2016-12-26
Citation
Journal of Fluid Mechanics, 2017, 814, pp.570-591
ISSN
0022-1120
Publisher
Cambridge University Press (CUP)
Start Page
570
End Page
591
Journal / Book Title
Journal of Fluid Mechanics
Volume
814
Copyright Statement
© Cambridge University Press 2017
This is an Open Access article, distributed under the terms of the Creative Commons Attribution
licence (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and
reproduction in any medium, provided the original work is properly cited.
This is an Open Access article, distributed under the terms of the Creative Commons Attribution
licence (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and
reproduction in any medium, provided the original work is properly cited.
Sponsor
Engineering & Physical Science Research Council (EPSRC)
Grant Number
EP/I005684/1
Subjects
Science & Technology
Technology
Physical Sciences
Mechanics
Physics, Fluids & Plasmas
Physics
low-dimensional models
parametric instability
wakes/jets
SPATIALLY DEVELOPING FLOWS
OPEN-LOOP CONTROL
BLUFF-BODY
GLOBAL INSTABILITIES
DYNAMICS
STABILITY
BIFURCATIONS
OSCILLATIONS
CHAOS
MODES
Fluids & Plasmas
01 Mathematical Sciences
09 Engineering
Publication Status
Published