Study on the flow field and concentration characteristics of the multiple tandem jets in crossflow

The characteristics of single and multiple tandem jets (n=2, 3, 4) in crossflow have been investigated using the realizable k-ɛ model. The results of this model agree well with experimental measurements using PIV (Particle Image Velocimetry) or LIF (Laser Induced Fluorescence). We analyzed the calculated results and obtained detailed properties of velocity and concentration of the multiple jets in the pre-merging and post-merging regions. When the velocity ratio is identical, the bending degree of the leading jet is greater than that of the rear jets. The last jet penetrates deeper as the jet number increases, and the shielding effect of the front jet declines with jet spacing increase. Interaction of the jet and crossflow induces formation and development of a counter-rotating vortex pair (CVP). CVP makes the distribution of concentration appear kidney-shaped (except in the merging region), and maximum concentration is at the center of the counter-rotating vortex. Concentration at the CVP center is 1.03–1.4 times that of the local jet trajectory. Post-merging velocity and concentration characteristics differ from those of the single jet because of the shielding effect and mixing of all jets. This paper presents a unified formula of trajectory, concentration half-width and trajectory dilution, by introducing a reduction factor.

[1]  T. Shih,et al.  A new k-ϵ eddy viscosity model for high reynolds number turbulent flows , 1995 .

[2]  W. S. Lewellen,et al.  On the vorticity dynamics of a turbulent jet in a crossflow , 1986, Journal of Fluid Mechanics.

[3]  Zhenxun Gao,et al.  Numerical research on mixing characteristics of different injection schemes for supersonic transverse jet , 2011 .

[4]  Yufeng Yao,et al.  Direct Numerical Simulation of Single and Multiple Square Jets in Cross-Flow , 2011 .

[5]  Subrata Roy,et al.  NUMERICAL INVESTIGATION OF THE BLADE COOLING EFFECT GENERATED BY MULTIPLE JETS ISSUING AT AN ANGLE INTO AN INCOMPRESSIBLE HORIZONTAL CROSSFLOW , 2000 .

[6]  Shiqiang Wu,et al.  Numerical application of k-ɛ turbulence model to the flow over a backward-facing step , 2010 .

[7]  M. Davidson,et al.  Characterising strongly advected discharges in the initial dilution zone , 2007 .

[8]  F. Boysan,et al.  Renormalization Group Modeling and Turbulence Simulations. , 1993 .

[9]  Lester L. Yuan,et al.  Large-eddy simulations of a round jet in crossflow , 1999, Journal of Fluid Mechanics.

[10]  D. Zhu,et al.  Near-Field Mixing Downstream of a Multiport Diffuser in a Shallow River , 2011 .

[11]  I. Seo,et al.  Modeling the mixing of heated water discharged from a submerged multiport diffuser , 2000 .

[12]  F. Menter Two-equation eddy-viscosity turbulence models for engineering applications , 1994 .

[13]  Large-eddy simulations and vortex structures of turbulent jets in crossflow , 2007 .

[14]  P. Tamamidis,et al.  NUMERICAL INVESTIGATION OF THE BLADE COOLING EFFECT GENERATED BY MULTIPLE INCOMPRESSIBLE JETS , 1998 .

[15]  James R. Clisset,et al.  A Spreadsheet for the Mixing of a Row of Jets with a Confined Crossflow. Supplement , 2005 .

[16]  Joseph H.W. Lee,et al.  Three-Dimensional Computations of Multiple Tandem Jets in Crossflow , 2006 .

[17]  H. Fang,et al.  Influence of Vertical Resolution and Nonequilibrium Model on Three-Dimensional Calculations of Flow and Sediment Transport , 2010 .

[18]  Steven Jay Wright EFFECTS OF AMBIENT CROSSFLOWS AND DENSITY STRATIFICATION ON THE CHARACTERISTIC BEHAVIOR OF ROUND TURBULENT BUOYANT JETS. , 1977 .

[19]  Jhw Lee,et al.  Structure of a turbulent jet in a crossflow - Effect of jet-crossflow velocity , 2002 .

[20]  D. Liang,et al.  Numerical Study of Hydrodynamics of Multiple Tandem Jets in Cross Flow , 2011 .

[21]  N. Rajaratnam,et al.  DILUTION OF MULTIPLE NONBUOYANT CIRCULAR JETS IN CROSSFLOWS , 1998 .

[22]  Daeyoung Yu,et al.  Multiple Tandem Jets in Cross-Flow , 2006 .