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Small hydrogen/oxygen rocket flowfield behavior from heat flux measurements

机译:通过热通量测量得出的小型氢气/氧气火箭流场行为

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摘要

The mixing and heat transfer phenomena in small rocket flow fields with fuel film cooling is not well understood. An instrumented, water-cooled chamber with a gaseous hydrogen/gaseous oxygen injector was used to gather steady-state inner and outer wall temperature profiles. The chamber was tested at 414 kPa (60 psia) chamber pressure, from mixture ratios of 3.41 to 8.36. Sixty percent of the fuel was used for film cooling. These temperature profiles were used as boundary conditions in a finite element analysis program, MSC/NASTRAN, to calculate the local radial and axial heat fluxes in the chamber wall. The normal heat fluxes were then calculated and used as a diagnostic of the rocket's flow field behavior. The normal heat fluxes determined were on the order of 1.0 to 3.0 MW/meters squared (0.6 to 1.8 Btu/sec-inches squared). In the cases where mixture ratio was 5 or above, there was a sharp local heat flux maximum in the barrel section of the chamber. This local maximum seems to indicate a reduction or breakdown of the fuel film cooling layer, possibly due to increased mixing in the shear layer between the film and core flows. However, the flow was thought to be completely laminar, as the throat Reynolds numbers were below 50,000 for all the cases. The increased mixing in the shear layer in the higher mixture ratio cases appeared not to be due to the transition of the flow from laminar to turbulent, but rather due to increased reactions between the hydrogen film and oxidizer-rich core flows.
机译:人们对带有燃料膜冷却的小型火箭流场中的混合和传热现象还不甚了解。使用带有气态氢/气态氧气注射器的仪器化水冷室收集稳态内壁和外壁温度曲线。在414 kPa(60 psia)的腔室压力下对腔室进行测试,混合比为3.41至8.36。 60%的燃料用于薄膜冷却。这些温度曲线在有限元分析程序MSC / NASTRAN中用作边界条件,以计算腔室壁中的局部径向和轴向热通量。然后计算正常的热通量,并将其用作火箭流场行为的诊断。确定的正常热通量约为1.0-3.0 MW /米平方(0.6-1.8 Btu /秒-平方英寸)。在混合比为5或更高的情况下,在腔室的桶形部分中存在急剧的局部热通量最大值。该局部最大值似乎表明燃料膜冷却层的减少或破裂,这可能是由于在膜流和堆芯流之间的剪切层中混合增加所致。但是,由于所有情况下的喉咙雷诺数均低于50,000,因此认为流动是完全层流的。在较高混合比的情况下,剪切层中混合的增加似乎不是由于流从层流到湍流的过渡,而是由于氢膜和富氧化剂的核心流之间的反应增加。

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    Reed, Brian D.;

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  • 年度 1993
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