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Flowfield characteristics on a vent slot mixer in supersonic flow

机译:超声速流动中排气槽混合器的流场特性

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摘要

A research was conducted on a new mixing device referred as a "vent slot mixer", using experimental and computational methods. The experiment was conducted in a laboratory-scale supersonic wind-tunnel of Mach number 2. Inflow air was under atmospheric air condition, and hydrogen gas was used as fuel. In addition, the computational simulation approach was performed to support the experimental result. The vent slot mixer can directly entrain the main airflow into the recirculation region, inducing complex flow structures in the recirculation region. This also leads to gradual development of the shear layer to reduce the total pressure loss mainly induced by a recompression shock. Contrary to typical shear layers of step mixer, for the vent slot mixer, two-dimensional large-scale structures and weak shocks were clearly identified around the shear layer through experimental and computational methods. When the fuel was injected from one circular injector in the recirculation region, the high fuel concentration of the vent slot mixer was evenly distributed along the spanwise direction, but with the step mixer the fuel was highly concentrated along the region downstream of the injector. Therefore, the vent slot mixer is effective to uniformly spread the fuel toward the spanwise direction in the recirculation region. As the fuel injection rate increased, the shear layer downstream of the vent slot mixer grew uniformly along the spanwise direction; consequently, shock structures such as a recompression shock and weak shocks on the shear layer were significantly mitigated at J = 3.2.
机译:使用实验和计算方法,对一种称为“通风槽混合器”的新型混合设备进行了研究。该实验在马赫数为2的实验室规模的超音速风洞中进行。流入的空气处于大气条件下,氢气用作燃料。另外,执行了计算仿真方法以支持实验结果。通风槽混合器可以直接将主要气流带入再循环区域,从而在再循环区域中引发复杂的流动结构。这也导致逐渐形成剪切层以减少主要由再压缩冲击引起的总压力损失。与步进混合器的典型剪切层相反,对于排气槽混合器,通过实验和计算方法可以清楚地识别剪切层周围的二维大型结构和弱冲击。当从再循环区域中的一个圆形喷油器喷射燃油时,排气槽混合器的高燃油浓度沿翼展方向均匀分布,但使用阶梯式混合器时,燃油沿喷油器下游区域高度集中。因此,排气槽混合器有效地使燃料在再循环区域中沿翼展方向均匀地散布。随着燃料喷射速率的增加,排气槽混合器下游的剪切层沿翼展方向均匀增长;因此,在J = 3.2时,剪切层上的再压缩冲击和弱冲击等冲击结构得到了显着缓解。

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