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首页> 外文期刊>Atomization and Sprays: Journal of the International Institutes for Liquid Atomization and Spray Systems >SPRAY CHARACTERISTICS OF A PRESSURE-SWIRL FUEL INJECTOR SUBJECTED TO A CROSSFLOW AND A COFLOW
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SPRAY CHARACTERISTICS OF A PRESSURE-SWIRL FUEL INJECTOR SUBJECTED TO A CROSSFLOW AND A COFLOW

机译:横流和顺流作用的旋流燃油喷射器的喷雾特性

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摘要

An analysis of fuel spray was conducted using flow visualization and phase Doppler particle anemometry (PDPA) in an experimental facility housed at the Propulsion Directorate of the US Air Force Research Laboratory (AFRL). In order to model typical real-world aircraft engine conditions, this test facility was equipped with a pressure-swirl injector in combination with heated crossflow air normal to the fuel (}P-8) injection and, optionally, with coflow air parallel to the primary direction of fuel injection. Results are presented for fixed fuel rate (Reynolds number for the liquid flow of 9200 and a liquid jet Weber number of 7100) and varied crossflow velocity for four momentum flux ratios. Flow visualization and coherent structure velocimetry clearly demonstrated how the crossflow reoriented the conical spray pattern and led to large spatial variation in the measured Sauter mean diameter. At locations downstream of the injector, the PDPA data demonstrated that the vertical component of velocity was relatively low for small droplets and high for large drop sizes. This bimodal behavior may be rationalized by considering the initial propagation direction of the spray, the residence time of the fuel droplets, and the shear of the surrounding flow field. The addition of a coflow stream of air to the system led to significant reductions in Sauter mean diameter of the droplets in the region of the spray cone downstream of the fuel injector. The coflow also tended to disrupt the bimodality of the drop size distribution.
机译:在美国空军研究实验室(AFRL)推进局的实验设施中,使用流动可视化和相位多普勒粒子风速计(PDPA)对燃油喷雾进行了分析。为了对典型的现实世界飞机发动机状况进行建模,该测试设备配备了压力旋流喷油器,并结合了垂直于燃料(} P-8)喷射的加热的横流空气,以及可选的平行于燃料的平行流空气。燃油喷射的主要方向。给出了固定燃油率(液体流量的雷诺数为9200,液体射流韦伯数为7100)和变化的错流速度(四个动量通量比)的结果。流动可视化和相干结构测速清楚地表明了错流如何重新定向圆锥形喷雾模式并导致所测得的Sauter平均直径发生较大的空间变化。在喷射器下游的位置,PDPA数据表明,垂直速度分量对于小液滴而言相对较低,而对于大液滴而言则较高。通过考虑喷雾的初始传播方向,燃料液滴的停留时间以及周围流场的剪切力,可以使这种双峰行为合理化。向系统中增加气流的同向流导致燃料喷射器下游喷淋锥区域中的液滴的苏特平均直径显着减小。共流还倾向于破坏液滴尺寸分布的双峰性。

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