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Non-Invasive Hall Current Distribution Measurement in a Hall Effect Thruster

机译:霍尔效应推进器中的无创霍尔电流分布测量

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Currently, a direct, accurate way to measure thrust produced by a Hall thruster on orbit does not exist. A technique able to know the produced thrust will enable timely and accurate maneuvering, a capability particularly important to satellite formation flying. The means to determine thrust directly is achievable by remotely measuring the magnetic field and solving the inverse problem for the Hall current density distribution. The magnetic field was measured by employing an array of eight tunneling magnetoresistive (TMR) sensors capable of milligauss sensitivity when placed in a high background field. The array was positioned just outside the thruster channel on a 1.5 kW CSU Hall thruster equipped with a center-mounted electride cathode. In this location, the static magnetic field is approximately 30 Gauss, which is within the linear operating range of the TMR sensors. Furthermore, the induced field at this distance is approximately tens of milligauss, which is within the sensitivity range of the TMR sensors. Because of the nature of the inverse problem, the induced-field measurements do not provide the Hall current density by a simple inversion; however, a Tikhonov regularization of the induced field does provide current density distributions as a function of time that are shown in contour plots. The measured ratios between the average Hall current and the discharge current ranged from 6.1 to 7.3 over a range of operating conditions from 1.3 kW to 2.2 kW. The temporal inverse solution at 1.5 kW exhibited a breathing mode of 24 kHz, which was in agreement with temporal measurements of the discharge current.
机译:当前,尚不存在直接,准确的方法来测量霍尔推力器在轨道上产生的推力。能够知道产生的推力的技术将能够进行及时而准确的操纵,这对卫星编队飞行特别重要。通过远程测量磁场并解决霍尔电流密度分布的反问题,可以实现直接确定推力的方法。磁场是通过使用八个隧穿磁阻(TMR)传感器阵列进行测量的,这些传感器在高背景场中的灵敏度为毫微秒。该阵列位于1.5 kW CSU Hall推进器上,位于推进器通道的外部,该推进器配有中心安装的电子阴极。在此位置,静磁场约为30高斯,在TMR传感器的线性工作范围内。此外,在此距离处的感应场大约为几十毫安,这在TMR传感器的灵敏度范围内。由于反问题的性质,感应场测量无法通过简单的反演来提供霍尔电流密度;反之,反之亦然。然而,感应场的Tikhonov正则化确实提供了作为时间函数的电流密度分布,如等高线图所示。在1.3 kW至2.2 kW的工作条件范围内,测得的平均霍尔电流与放电电流之比范围为6.1至7.3。 1.5 kW的时间逆解表现出24 kHz的呼吸模式,这与放电电流的时间测量结果一致。

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