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Mode Transitions in Hall-Effect Thrusters Induced by Variable Magnetic Field Strength

机译:可变磁场强度在霍尔效应推进器中的模式转变

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摘要

Mode transitions in a 6 kW laboratory Hall-effect thruster were induced by varying the magnetic field intensity while holding all other operating parameters constant Ultrafast imaging, discharge current, and thrust measurements were used to characterize the change in discharge channel current density and thruster performance through mode transitions. The modes are described here as global oscillation mode and local oscillation mode. In global mode, the entire discharge channel is oscillating in unison and spokes are either absent or negligible with discharge current oscillation amplitude (root mean square) greater than 10% of the mean value and can even be as high as 100%. In local oscillation mode, perturbations in the discharge current density are seen to propagate in the E × B direction. Spokes are localized oscillations that are typically 10-20% of the mean discharge current density value. The discharge current oscillation amplitude and mean values are significantly lower than global mode. The mode transitions changed with operating conditions, where the transition between global mode and local mode occurred at higher relative magnetic field strengths for higher mass flow rate or higher discharge voltage. The thrust was approximately constant through the mode transition, but the thrust-to-power ratio and anode efficiency decreased significantly in global mode. The peaks in thrust to power and anode efficiency typically occur near the transition point Thruster performance maps should include variation in discharge current, discharge voltage, and magnetic field, known as I_D - V_D - B maps, at different flow rates to identify transition regions throughout the life of a thruster. These results are used to calculate a transition surface for use by operators to keep the thruster operating in an optimal mode.
机译:在保持所有其他操作参数不变的情况下,通过改变磁场强度来诱发6 kW实验室霍尔效应推进器的模式转变。超快成像,放电电流和推力测量用于表征放电通道电流密度和推进器性能的变化,包括模式转换。在此将模式描述为整体振荡模式和局部振荡模式。在全局模式下,整个放电通道会同时振荡,而轮辐不存在或可忽略不计,而放电电流的振荡幅度(均方根)大于平均值的10%,甚至可能高达100%。在局部振荡模式下,可以看到放电电流密度的扰动沿E×B方向传播。辐条是局部振荡,通常为平均放电电流密度值的10-20%。放电电流的振荡幅度和平均值明显低于全局模式。模式转换随操作条件而变化,其中全局模式和局部模式之间的转换在较高的相对磁场强度下发生,以实现更高的质量流量或更高的放电电压。在模式转换过程中,推力大致恒定,但在整体模式下,推力功率比和阳极效率显着下降。推力功率和阳极效率的峰值通常出现在过渡点附近推力器性能图应包括放电电流,放电电压和磁场的变化,称为I_D-V_D-B图,以不同的流量确定整个过渡区域推进器的寿命。这些结果用于计算过渡面,供操作员使用,以使推进器保持最佳状态。

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  • 来源
    《Journal of propulsion and power》 |2016年第4期|903-917|共15页
  • 作者单位

    University of Michigan, Ann Arbor, Michigan 48105;

    University of Michigan, Ann Arbor, Michigan 48105;

    U.S. Air Force Research Laboratory, Edwards Air Force Base, California 93524;

    Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California 91109;

    Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California 91109;

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