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Analysis of Air Plasma Flows in Magnetoplasmadynamic Arcjet Testing

机译:磁性血管血管弧喷射试验中的空气等离子体流动分析

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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:研究了磁体上动脉弧喷射对流动平移温度和速度的影响。从名义上的测试条件,代表Hayabusa重新进入的78.8公里的高度轨迹点,电功率从146千瓦倍变化到189千瓦,并且使用耦合光谱仪和法布里 - 珀罗干涉仪测量温度和速度确定原子发射线的多普勒扩大和多普勒偏移。使用四种不同的排放线测量原子氮平移温度,导致标称试验条件的10700 k的中值温度值。使用777nm三重态度测量原子氧温度,中值温度值为16350k。尚未确定氧气较高温度的原因,然而,这与先前在不同的等离子体发生器上获得的结果一致。氮气和氧气的温度大致线性地与电输入功率增加。与24k / kW的氧增加相比,测量的氮温度增加38k / kW(0.35%/ kW)的氮温度显着较大。这被认为是由于从电弧进入氮气的直接能量转移,而氧气通过弧下游的颗粒碰撞通电。氮和氧的测量速度是相同的。对于标称情况,速度在3350 m / s中测量。速度也随着电力增加而大致线性增加。测定速度增加为22 m / s / kW(0.66%/ kW)。当被认为是百分比时,这是比温度升高的更强的效果。

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