An experimental investigation of the effects of nozzle operating conditions on the development of nozzle-exit boundary layers of highly heated air free jets is reported in this paper. The total pressure measurements in the nozzle-exit boundary layer were obtained at a range of jet Mach numbers from 0.1 to 0.97 and jet total temperatures up to 900 K. The analysis of results shows that the nozzle-exit laminar boundary-layer development depends only on the nozzle-exit Reynolds number. For the nozzle-exit turbulent boundary layer, however, it appears that the effects of the jet total temperature on the boundary-layer integral characteristics are independent from the effect of the nozzle-exit Reynolds number. This surprising finding has not yet been reported. Further, laminar boundary-layer profiles were compared with the Pohlhausen solution for a flat-wall converging channel and an acceptable agreement was found only for low Reynolds numbers. For turbulent boundary layers, the dependence of the shape factor on relative Mach numbers at a distance of one momentum thickness from the nozzle wall resembles Spence’s prediction. Finally, the calculated total pressure loss coefficient was found to depend on the nozzle-exit Reynolds number for the laminar nozzle-exit boundary layer, while for the turbulent exit boundary layer this coefficient appears to be constant.
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April 1992
Research Papers
An Experimental Investigation of Nozzle-Exit Boundary Layers of Highly Heated Free Jets
J. Lepicovsky
J. Lepicovsky
Sverdrup Technology, Inc., NASA Lewis Research Center Group, Brook Park, OH 44142
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J. Lepicovsky
Sverdrup Technology, Inc., NASA Lewis Research Center Group, Brook Park, OH 44142
J. Turbomach. Apr 1992, 114(2): 469-475 (7 pages)
Published Online: April 1, 1992
Article history
Received:
January 15, 1990
Online:
June 9, 2008
Citation
Lepicovsky, J. (April 1, 1992). "An Experimental Investigation of Nozzle-Exit Boundary Layers of Highly Heated Free Jets." ASME. J. Turbomach. April 1992; 114(2): 469–475. https://doi.org/10.1115/1.2929167
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