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Analysis of Air Plasma Flows in Magnetoplasmadynamic Arcjet Testing

机译:磁等离子体动力学Arcjet测试中的空气等离子体流分析

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The influence of the electrical input power of a magnetoplasmadynamic arcjet on the flow translational temperature and velocity is investigated. From a nominal testing condition, representing the 78.8 km altitude trajectory point on the Hayabusa re-entry, the electrical power is varied from 146 kW to 189 kW and the temperature and velocity are measured using a system coupling a spectrometer and a Fabry-Perot interferometer to determine the Doppler broadening and Doppler shift of the atomic emission lines. The atomic nitrogen translational temperature is measured using four different emission lines resulting in a median temperature value of 10700 K for the nominal test condition. The atomic oxygen temperature is measured using the 777 nm triplet with a median temperature value of 16350 K. A reason for the higher temperature of the oxygen has not been determined, however, this is in line with results previously obtained on a different plasma generator. The temperatures of both the nitrogen and oxygen increase approximately linearly with electrical input power. The effect of the power increase is significantly larger on the nitrogen temperature with a measured increase of 38 K / kW (0.35 % / kW) compared to the oxygen increase of 24 K / kW (0.15 % / kW). This is thought to be due to the direct energy transfer from the arc into the nitrogen whereas the oxygen is energised through particle collisions downstream of the arc. The measured velocities were the same for nitrogen and oxygen. For the nominal condition the velocity was measured at 3350 m / s. The velocity also increases approximately linearly with the electrical power increase. The velocity increase was determined to be 22 m / s / kW (0.66 % / kW). When considered as a percentage this is a stronger effect than seen in the temperature increases.
机译:研究了磁等离子体动力电弧喷射器的电输入功率对流动平移温度和速度的影响。在标称测试条件下(代表Hayabusa再入站的78.8 km高度轨迹点),电功率从146 kW改变为189 kW,并使用结合了光谱仪和Fabry-Perot干涉仪的系统测量温度和速度确定原子发射谱线的多普勒展宽和多普勒频移。使用四个不同的发射线测量原子氮的转化温度,得出标称测试条件的中值温度值为10700K。原子氧温度是使用777 nm三重峰测量的,中值温度值为16350K。氧的较高温度的原因尚未确定,但是,这与先前在其他等离子体发生器上获得的结果一致。氮和氧的温度均随输入功率的增加而线性增加。与测得的氧气增加量24 K / kW(0.15%/ kW)相比,功率增加对氮气温度的影响显着更大,测得的增加量为38 K / kW(0.35%/ kW)。认为这是由于能量从电弧直接转移到氮气中,而氧气是通过电弧下游的粒子碰撞而激发的。氮气和氧气的测量速度相同。对于标称条件,测得的速度为3350 m / s。速度也随着电功率的增加而近似线性地增加。测得的速度增加为22 m / s / kW(0.66%/ kW)。当以百分比计时,这是比在温度升高中看到的效果更强的效果。

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