Preliminary Results on Coaxial Jet Spread Angles and the Effects of Variable Phase Transverse Acoustic Fields (Postprint)

Abstract : An experimental study on the jet spreading angle of N2 shear coaxial jets at sub-, near-, and supercritical pressures is presented. The jet spreading angle is an important parameter which characterizes the mixing between two flows forming a shear layer. The present results are compared with previous experimental data, CFD results, and theoretical predictions. The angle measurements are made directly from at least 20 backlit images. The shear coaxial injector used here is similar to those used in cryogenic liquid rockets. The chamber pressure ranges from 1.5 to 5.0 MPa to span subcritical to supercritical pressures. The chamber to outer jet density ratio varies from 0.17-4.8 and the momentum flux ratio between the outer and the inner jet varies from 0.37 to 30. These ratios are mainly varied by changing the temperature and flow rates of the outer jet. For the ranges of conditions studied it is found that the tangent of the jet spreading angle is roughly constant and approximately 0.19 with std. dev. of 0.02. The value is lower than those predicted by different theories for planar mixing layers of variable density for gaseous flows. The second part of the paper focuses on the initial results obtained by combining two piezo-sirens which generate a transverse acoustic field to excite the coaxial jet. The resonant frequency studied is approximately 3kHz and delta P/P varies from 1-1.6%. These two acoustic sources can have an arbitrary phase between them so the position of the jet with respect to the pressure and velocity field can be adjusted. The main parameter investigated is the length of the dark inner jet core. The initial results indicate an effect of the phase angle on the dark core length but the differences are statistically significant only in the extreme cases.

[1]  A. Roshko,et al.  The compressible turbulent shear layer: an experimental study , 1988, Journal of Fluid Mechanics.

[2]  N. Ko,et al.  Initial Region of Subsonic Coaxial Jets of High Mean-Velocity Ratio , 1981 .

[3]  G. N. Abramovich The Theory of Turbulent Jets , 2003 .

[4]  A. Roshko,et al.  On density effects and large structure in turbulent mixing layers , 1974, Journal of Fluid Mechanics.

[5]  Michel Favre-Marinet,et al.  The density field of coaxial jets with large velocity ratio and large density differences , 2001 .

[6]  Bruce Chehroudi,et al.  Dark Core Analysis of Coaxial Injectors at Sub-, Near-, and Supercritical Conditions in a Transverse Acoustic Field , 2007 .

[7]  Douglas G Talley,et al.  Visual characteristics and initial growth rates of round cryogenic jets at subcritical and supercritical pressures , 2002 .

[8]  J. Whitelaw,et al.  Turbulent Mixing in the Developing Region of Coaxial Jets , 1973 .

[9]  N. Otsu A threshold selection method from gray level histograms , 1979 .

[10]  Bruce Chehroudi,et al.  Measurements in an Acoustically-Driven Coaxial Jet Under Sub-, Near-, and Supercritical Conditions (PREPRINT) , 2005 .

[11]  Vigor Yang,et al.  Dynamics of Shear-Coaxial Cryogenic Nitrogen Jets with Acoustic Excitation under Supercritical Conditions , 2006 .

[12]  Michael Oschwald,et al.  INJECTION OF FLUIDS INTO SUPERCRITICAL ENVIRONMENTS , 2006 .

[13]  Richard D. Branam,et al.  Characterization of cryogenic injection at supercritical pressure , 2001 .

[14]  P. Dimotakis Two-dimensional shear-layer entrainment , 1986 .