Observations on the non-mixed length and unsteady shock motion in a two dimensional supersonic ejector

Key features that drive the operation of a supersonic ejector are the complex gasdynamic interactions of the primary and secondary flows within a variable area duct and the phenomenon of compressible turbulent mixing between them, which have to be understood at a fundamental level. An experimental study has been carried out on the mixing characteristics of a two dimensional supersonic ejector with a supersonic primary flow (air) of Mach number 2.48 and the secondary flow (subsonic) which is induced from the ambient. The non-mixed length, which is the length within the ejector for which the primary and secondary flow remain visually distinct is used to characterize the mixing in the ejector. The operating pressures, flow rates and wall static pressures along the ejector have been measured. Two flow visualization tools have been implemented—time resolved schlieren and laser scattering flow visualization. An important contribution has been the development of in-house image processing algorithms on the MATLAB...

[1]  I. Mcgregor,et al.  The vapour-screen method of flow visualization , 1961, Journal of Fluid Mechanics.

[2]  E. Spiegler,et al.  Shock-Induced Boundary Layer Separation in Over-Expanded Conical Exhaust Nozzles , 1963 .

[3]  Richard B Fancher Low-Area Ratio, Thrust-Augmenting Ejectors , 1972 .

[4]  K. R. Hedges,et al.  Compressible Flow Ejectors: Part II—Flow Field Measurements and Analysis , 1974 .

[5]  C. D. Mikkelsen,et al.  A Theoretical and Experimental Investigation of the Constant Area, Supersonic-Supersonic Ejector , 1981 .

[6]  Morton Alperin,et al.  Thrust Augmenting Ejectors, Part I , 1983 .

[7]  Morton Alperin,et al.  Thrust augmenting ejectors, II , 1983 .

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

[9]  Noel T. Clemens,et al.  A planar Mie scattering technique for visualizing supersonic mixing flows , 1991 .

[10]  Ephraim Gutmark,et al.  Mixing Enhancement in Supersonic Free Shear Flows , 1995 .

[11]  Noel T. Clemens,et al.  Large-scale structure and entrainment in the supersonic mixing layer , 1995, Journal of Fluid Mechanics.

[12]  Jayanta Panda,et al.  Shock oscillation in underexpanded screeching jets , 1998, Journal of Fluid Mechanics.

[13]  Khairul Q. Zaman,et al.  Spreading characteristics of compressible jets from nozzles of various geometries , 1999, Journal of Fluid Mechanics.

[14]  K. A. Bhaskaran,et al.  Development of design methods for short cylindrical supersonic exhaust diffuser , 2000 .

[15]  Philippe Desevaux,et al.  A method for visualizing the mixing zone between two co-axial flows in an ejector , 2001 .

[16]  Vaclav Dvorak,et al.  Supersonic flow structure in the entrance part of a mixing chamber of 2D model ejector , 2003 .

[17]  Satha Aphornratana,et al.  An experimental investigation of a steam ejector refrigerator: the analysis of the pressure profile along the ejector , 2004 .

[18]  Satha Aphornratana,et al.  Ejectors: applications in refrigeration technology , 2004 .

[19]  Yann Bartosiewicz,et al.  Numerical and Experimental Investigations on Supersonic Ejectors , 2005 .

[20]  Vaclav Dvorak,et al.  Transonic instability in entrance part of mixing chamber of high-speed ejector , 2005 .

[21]  Aristide F. Massardo,et al.  Design and Testing of Ejectors for High Temperature Fuel Cell Hybrid Systems , 2006 .

[22]  Dimitri Papamoschou,et al.  Mixing Enhancement from Severely Overexpanded Nozzles , 2010 .

[23]  Gopalan Jagadeesh,et al.  Vector Evaluated Particle Swarm Optimization (VEPSO) of Supersonic Ejector for Hydrogen Fuel Cells , 2010 .

[24]  Zhenguo Wang,et al.  The effect of secondary flows on the starting pressure for a second-throat supersonic ejector , 2011 .

[25]  Huilin Lu,et al.  Experimental investigation on starting process of supersonic single-stage air ejector , 2012 .