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中国物理学会期刊

脉冲电弧等离子体激励控制超声速平板边界层转捩实验

CSTR: 32037.14.aps.69.20200216

Experimental study on supersonic plate boundary layer transition under pulsed arc plasma excitation control

CSTR: 32037.14.aps.69.20200216
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  • 脉冲电弧等离子体激励器具有局部加热效应强、扰动范围广等特点, 在超声速流动控制中具有广阔的应用前景. 本文运用电参数测量系统和高速纹影技术研究了脉冲电弧等离子体激励器在Ma = 3来流条件下的电特性和流场特性; 采用纳米粒子平面激光散射技术对超声速平板边界层的流动结构进行了精细测量, 并对不同等离子体激励频率下的边界层转捩特性进行了研究. 实验结果表明, 脉冲电弧放电会产生速度较高的前驱冲击波和温度较高的热沉积区, 给边界层施加连续不断的扰动. 施加扰动的脉冲电弧等离子体激励能够促进超声速平板边界层转捩. 并且脉冲放电的高频冲击效应可以促进转捩提前发生, 且频率越高, 效果越好, 当施加激励频率为60 kHz时, 转捩区长度为0, 湍流边界层厚度为25 mm. 脉冲电弧等离子体激励器可以用来促进超声速边界层转捩.

     

    Pulsed arc plasma excitation is characterized by strong local heating effect and wide disturbance range, and it has a broad application prospect in supersonic flow control. In this paper, by using electrical parameter measurement system and high speed schlieren technique, we study the electrical and flow field characteristics of pulsed arc plasma excitation under the condition of Ma = 3 incoming flow. The nano-particle planar laser scattering (NPLS) is used to investigate the flow structure of the supersonic flat boundary layer, and the transition characteristics of the boundary layer at different plasma excitation frequencies are studied. The experimental results show that in the flow field with Ma = 3 and the total incoming pressure P0 = 1 atm (1 atm = 1.01 × 105 Pa), the peak voltage of the pulsed arc plasma actuator discharge is 6 kV, the peak current is 70 A, the time scale of the discharge is about 300 ns, the single discharge energy is 70 mJ; the pulsed arc discharge will produce the precursor shock wave with higher velocity and the thermal deposition zone with higher temperature, which will exert continuously disturbance on the boundary layer. The pulsed arc plasma excitation with perturbation can promote the transition of supersonic plate boundary layer. Moreover, the high-frequency impact effect of pulsed discharge can promote the transition to occur ahead of time, and the higher the frequency, the better the effect is. As the excitation frequency increases, the transition position of the boundary layer of the supersonic flat plate moves forward, and the length of the transition area of the boundary layer becomes shorter as the excitation frequency increases. When the excitation frequency is 60 kHz, the length of transition zone is 0 and the thickness of turbulent boundary layer is 25 mm. When a high frequency is applied (f = 40, 60 kHz), the transition path of the boundary layer is that the shock wave generated by the plasma excitation triggers the unstable wave, and the development of unstable waves directly skips the linear growth stage, passes through the bypass and transitions into turbulent flow. The pulsed arc plasma excitation can be used to promote supersonic boundary layer transition.

     

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