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Characterizing Dry Ice Particle Response for Clean SeedingPIV Applications

机译:用于清洁播种型应用的干冰颗粒响应

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Particle imaging velocimetry has been carried out in supersonic flow fields by seeding the plenum with carbon dioxide expanded from a high pressure tank through an orifice surrounded by a shroud tube. The experiment was successfully applied in two different supersonic wind tunnel facilities of different scale. For both tunnels, seeding density was sufficient for boundary layer thickness measurements. In the smaller tunnel, with a 6.3 cm by 6.3 cm cross section, mean velocity measurements leading to a characterization of particle response were carried out for Mach 3 flow over a 10-degreee ramp. The particle lag across the shock wave was quantified, and the results suggest that the particle size in the test section was consistent with particle diameters between 1 μm and 2 μm. In general, the mean velocity pattern compares favorably with expectations. Boundary layer thickness was also measured upstream of the ramp for two different stagnation pressure conditions, and the Reynolds number effect was in good agreement with theory. Boundary layer thickness and freestream velocities were also measured for the larger tunnel, which has a 15.2 cm by 15.2 cm cross section. An effort to reduce particle lag by injecting a co-flow of air within the shroud tube of the injector is documented. While the addition of co-flow did produce smaller particles exiting the shroud tube, as measured using a Malvern Spraytec particle size analyzer, the particle density achieved during the tunnel testing dropped to the point that condensate, rather than discrete particles, dominated the test section.
机译:通过将增压室播种通过由护罩管围绕的孔播种通过从高压罐膨胀的二氧化碳而在超声波流场中进行颗粒成像速度。实验成功应用于不同规模的两种不同的超音速风洞设施。对于两个隧道,播种密度足以用于边界层厚度测量。在较小的隧道中,具有6.3cm×6.3cm的横截面,对于Mach 3流量,在10-STO-STO-RAMP上流动进行了导致粒子响应表征的平均速度测量。定量了冲击波穿过冲击波的颗粒滞后,结果表明试验部分中的粒度与粒径一致,粒径在1μm和2μm之间。通常,平均速度模式与期望有利。边界层厚度也在斜坡上游测量两个不同的停滞压力条件,并且雷诺数效应与理论吻合良好。对于较大的隧道,还测量边界层厚度和自由流速度,其具有15.2cm×15.2cm的横截面。记录了在喷射器的护罩管内注入喷射空气中的共流来减少粒子滞后的努力。虽然共流的加入确实产生离开护罩管的较小颗粒,但是使用符号喷雾器粒度分析仪测量,在隧道测试期间达到的粒子密度降至冷凝物,而不是离散粒子,主导了测试部分。

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