The self-preserving mixing properties of steady round nonbuoyant turbulent jets in uniform crossflows were investigated experimentally. The experiments involved steady round nonbuoyant fresh water jet sources injected into uniform and steady fresh water crossflows within the windowed test section of a water channel facility. Mean and fluctuating concentrations of source fluid were measured over cross sections of the flow using planar-laser-induced-fluorescence (PLIF). The self-preserving penetration properties of the flow were correlated successfully similar to Diez et al. [ASME J. Heat Transfer, 125, pp. 1046–1057 (2003)] whereas the self-preserving structure properties of the flow were correlated successfully based on scaling analysis due to Fischer et al. [Academic Press, New York, pp. 315–389 (1979)]; both approaches involve assumptions of no-slip convection in the cross stream direction (parallel to the crossflow) and a self-preserving nonbuoyant line puff having a conserved momentum force per unit length that moves in the streamwise direction (parallel to the initial source flow). The self-preserving flow structure consisted of two counter-rotating vortices, with their axes nearly aligned with the crossflow (horizontal) direction, that move away from the source in the streamwise direction due to the action of source momentum. Present measurements extended up to 260 and 440 source diameters from the source in the streamwise and cross stream directions, respectively, and yielded the following results: jet motion in the cross stream direction satisfied the no-slip convection approximation; geometrical features, such as the penetration of flow boundaries and the trajectories of the axes of the counter-rotating vortices, reached self-preserving behavior at streamwise distances greater than 40–50 source diameters from the source; and parameters associated with the structure of the flow, e.g., contours and profiles of mean and fluctuating concentrations of source fluid, reached self-preserving behavior at streamwise (vertical) distances from the source greater than 80 source diameters from the source. The counter-rotating vortex structure of the self-preserving flow was responsible for substantial increases in the rate of mixing of the source fluid with the ambient fluid compared to corresponding axisymmetric flows in still environments, e.g., transverse dimensions in the presence of the self-preserving counter-rotating vortex structure were 2–3 times larger than transverse dimensions in self-preserving axisymmetric flows at comparable conditions.

1.
Sangras
,
R.
,
Kwon
,
O. C.
, and
Faeth
,
G. M.
, 2002, “
Self-Preserving Properties of Unsteady Round Nonbuoyant Turbulent Starting Jets and Puffs in Still Fluids
,”
ASME J. Heat Transfer
0022-1481,
124
, pp.
460
469
.
2.
Diez
,
F. J.
,
Sangras
,
R.
,
Kwon
,
O. C.
, and
Faeth
,
G. M.
, 2003, “
Self-Preserving Properties of Unsteady Round Nonbuoyant Turbulent Starting Jets and Puffs in Still Fluids
,”
ASME J. Heat Transfer
0022-1481,
125
, pp.
204
205
.
3.
Diez
,
F. J.
,
Sangras
,
R.
,
Faeth
,
G. M.
and,
Kwon
,
O. C.
, 2003, “
Self-Preserving Properties of Unsteady Round Buoyant Turbulent Plumes and Thermals in Still Fluids
,”
ASME J. Heat Transfer
0022-1481,
125
, pp.
821
830
.
4.
Diez
,
F. J.
,
Bernal
,
L. P.
, and
Faeth
,
G. M.
, 2003, “
Round Turbulent Thermals, Puffs, Starting Plumes and Starting Jets in Uniform Crossflow
,”
ASME J. Heat Transfer
0022-1481,
125
, pp.
1046
1057
.
5.
Diez
,
F. J.
,
Bernal
,
L. P.
and
Faeth
,
G. M.
, 2004, “
Self-Preserving Mixing Properties of Steady Round Nonbuoyant Turbulent Jets in Uniform Crossflows
,” Report No. GDL/GMF-04-02,
Department of Aerospace Engineering, The University of Michigan
, Ann Arbor, Michigan.
6.
Smith
,
S. H.
, and
Mungal
,
M. G.
, 1998, “
Mixing, Structure and Scaling of the Jet in Crossflow
,”
J. Fluid Mech.
0022-1120,
357
, pp.
83
122
.
7.
Lee
J. H. W.
, and
Chu
V. H.
, 2003,
Turbulent Jets and Plumes a Lagrangian Approach
,
Kluwer Academic
, Dordrecht, The Netherlands, pp.
211
247
.
8.
Keffer
,
J. F.
, and
Baines
,
W. D.
, 1963, “
The Round Turbulent Jet in a Cross Wind
,”
J. Fluid Mech.
0022-1120,
15
, pp.
481
496
.
9.
Kamotami
,
Y.
, and
Greber
,
I.
, 1972, “
Experiments on a Turbulent Jet in Crossflow
,”
AIAA J.
0001-1452,
11
, pp.
1425
1429
.
10.
Chassaing
,
P.
,
George
,
J.
,
Claria
,
A.
, and
Sananes
,
F.
, 1974, “
Physical Characteristics of Subsonic Jets in a Cross-Stream
,”
J. Fluid Mech.
0022-1120,
64
, pp.
41
64
.
11.
Andreopoulos
,
J.
, and
Rodi
,
W.
, 1984, “
Experimental Investigation of Jets in Crossflow
,”
J. Fluid Mech.
0022-1120,
138
, pp.
93
127
.
12.
Broadwell
,
J. E.
, and
Breidenthal
,
R. E.
, 1984, “
Structure and Mixing of a Transverse Jet in an Incompressible Flow
,”
J. Fluid Mech.
0022-1120,
148
, pp.
405
412
.
13.
Askari
,
A.
,
Bullman
,
S. J.
,
Fairwether
,
M.
, and
Swaffield
,
F.
, 1990, “
The Concentration Field of a Turbulent Jet in a Cross-Wind
,”
Combust. Sci. Technol.
0010-2202,
73
, pp.
463
478
.
14.
Kelso
,
R. M.
,
Lim
,
T. T.
, and
Perry
,
A. E.
, 1996, “
An Experimental Study of Round Jets in Crossflow
,”
J. Fluid Mech.
0022-1120,
306
, pp.
111
144
.
15.
Fischer
,
H. B.
,
List
,
E. J.
,
Koh
,
R. C.
,
Imberger
,
J.
, and
Brooks
,
N. H.
, 1979,
Mixing in Inland and Coastal Waters
,
Academic Press
, New York, pp.
315
389
.
16.
List
,
E. J.
, 1982, “
Turbulent Jets and Plumes
,”
Annu. Rev. Fluid Mech.
0066-4189,
14
, pp.
189
212
.
17.
Steckler
,
K. D.
,
Baum
,
H. R.
, and
Quintiere
,
J. G.
, 1986, “
Salt Water Modeling of Fire Induced Flows in Multicompartment Enclosures
,”
Proc. Combust. Inst.
,
21
, pp.
143
149
.
18.
Wu
,
P.-K.
,
Miranda
,
R. F.
, and
Faeth
,
G. M.
, 1995, “
Effects of Initial Flow Conditions on Primary Breakup of Nonturbulent and Turbulent Round Liquid Jets
.”
Atomization Sprays
1044-5110,
5
, pp.
175
196
.
19.
Ferrier
,
A. J.
,
Funk
,
D. R.
, and
Roberts
,
P. J. W.
, 1993, “
Application of Optical Techniques to the Study of Plumes in Stratified Fluids
,”
Dyn. Atmos. Oceans
0377-0265,
20
, pp.
155
183
.
20.
Karasso
,
P. S.
, and
Mungal
,
M. G.
, 1997, “
PLIF Measurements in Aqueous Flows Using the Nd:YAG Laser
,”
Exp. Fluids
0723-4864,
23
, pp.
382
387
.
21.
Law
,
A. W.-K.
and
Wang
,
H.
, 2000, “
Measurement of Mixing Processes With Combined Digital Particle Image Velocimetry and Planar Laser Induced Fluorescence
,”
Exp. Therm. Fluid Sci.
0894-1777,
22
, pp.
213
229
.
22.
Cowen
,
E. A.
,
Chang
,
K.-H.
, and
Liao
,
Q.
, 2001, “
A Single-Camera Coupled PTV-LIF Technique
,”
Exp. Fluids
0723-4864,
31
, pp.
63
73
.
23.
Crimaldi
,
J. P.
, and
Koseff
,
J. R.
, 2001, “
High-Resolution Measurements of the Spatial and Temporal Structure of a Turbulent Plume
,”
Exp. Fluids
0723-4864,
31
, pp.
90
102
.
24.
Webster
,
D. R.
,
Roberts
,
P. J. W.
and
Ra’ad
,
L.
, 2001, “
Simultaneous DPTV/PLIF Measurements of a Turbulent Jet
,”
Exp. Fluids
0723-4864,
30
, pp.
65
72
.
25.
Tian
,
W.
and
Roberts
,
P. J. W.
, 2003, “
A 3D LIF System for Turbulent Buoyant Jet Flows
,”
Exp. Fluids
0723-4864,
35
, pp.
636
647
.
26.
Tennekes
,
H.
, and
Lumley
,
J. L.
, 1972,
A First Course in Turbulence
,
MIT Press
, Cambridge, Massachusetts, pp.
113
124
.
27.
Dai
,
Z.
,
Tseng
,
L.-K.
, and
Faeth
,
G. M.
, 1994, “
Structure of Round, Fully-Developed, Buoyant Turbulent Plumes
,”
ASME J. Heat Transfer
0022-1481,
116
, pp.
409
417
.
28.
Dai
,
Z.
,
Tseng
,
L.-K.
, and
Faeth
,
G. M.
, 1995, “
Velocity Statistics of Round, Fully-Developed Buoyant Turbulent Plumes
,”
ASME J. Heat Transfer
0022-1481,
117
, pp.
138
145
.
29.
Turner
,
J. S.
, 1969, “
Buoyant Plumes and Thermals
.”
Annu. Rev. Fluid Mech.
0066-4189,
1
, pp.
29
44
.
30.
Dimotakis
,
P. E.
, 2000, “
The Mixing Transition in Turbulent Flows
,”
J. Fluid Mech.
0022-1120,
409
, pp.
69
98
.
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