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采用实验加仿真方法研究了等离子体合成射流对超声速混合层的影响. 使用基于纳米粒子的平面激光散射技术(nanoparticle-based planar laser scattering, NPLS)、粒子图像测速技术 (particle image velocimetry, PIV)以及纹影手段获取了单次脉冲对混合层的影响. 采用二维数值仿真对布置在不同位置的高频激励器的混合效果以及激励器的性能进行了研究. 通过对比有扰动和无扰动的NPLS、PIV以及纹影实验结果, 发现等离子体合成射流对超声速混合层有明显的扰动, 射流喷出时会产生较强的斜激波. 对数值仿真结果的分析表明, 等离子体合成射流可以有效地增强混合层的厚度. 对比激励器布置在不同位置工况下的混合层厚度, 可以看出在激励器隔板末端对混合层的扰动效果最好, 混合层对在隔板末端的激励器扰动响应也是最快的. 对等离子体合成射流激励器的性能分析表明, 在隔板末端的激励器输出的能量最多. 通过分析等离子体合成射流的作用过程, 可以看出激励器在隔板上下表面布置的作用形式是通过作用来流进而影响混合层, 在隔板尾端布置的等离子体合成射流激励器直接作用在混合层上, 实现混合增强.Mixing enhancement for supersonic mixing layer is of great importance for developing scramjet engine. The growth rate of supersonic mixing layer is smaller than that of subsonic mixing layer. As the compressibility increases, the mixing enhancement becomes more difficult. Plasma synthetic jet is regarded as a promising flow control technology. The plasma synthetic jet generator can produce high energy jet. This generator has no moving parts and does not need additional gas source. It is the first time that plasma synthetic jet has been used to enhance the mixing in supersonic mixing layers. The influence of plasma synthetic jet on the supersonic mixing layer is investigated experimentally and numerically. The experiments are conducted in the low noise supersonic mixing layer wind tunnel. The Mach number of upper stream and lower stream are 1.37 and 2.39 respectively. The convective Mach number of this wind tunnel is 0.32. The plasma synthetic jet actuators are installed in the splitter plate. The distance between the jet hole and the splitter plate end is 15 mm. The nanoparticle-based planar laser scattering (NPLS), particle image velocimetry (PIV) and schlieren are used to obtain the response of the supersonic mixing layer to single pulse plasma synthetic jet perturbation. The NPLS successfully captures the large-scaled vortex structures induced by the plasma synthetic jet in the supersonic mixing layers. The effect of plasma synthetic jet is remarkable. The schlieren images show the process of the perturbation. An oblique shock wave is generated when the jet is ejected. The PIV is employed to obtain the influence of plasma synthetic jet on the velocity field. The y-velocity standard deviation increases due to the perturbation. The actuators’ mixing enhancement effects and actuators’ performances at three locations are investigated by two-dimensional numerical simulation. The three actuators are located on the upper, bottom and end surface of splitter plate respectively. The numerical simulation results show that the mixing layer thickness is increased by the plasma synthetic jet perturbation. There are two mechanisms of perturbations while actuators are located at different positions. The actuators installed on the upper and bottom surface of splitter plate influence the mixing layer through perturbing the upper and lower stream respectively. The actuator installed at the end of splitter plate affects the mixing layer directly. The response time of supersonic mixing layers to the perturbation of the actuator installed at the end of splitter plate is shorter than those of the others. The performance of each actuator is sensitive to the location.
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Keywords:
- mixing enhancement /
- plasma synthetic jet /
- flow control /
- supersonic mixing layers








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