静电控制大孔径反射卫星天线

J. Lang, D. Staelin
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引用次数: 1

摘要

空间中天线尺寸的一个主要实际限制是每单位反射面积的最小可行质量。为了实现低天线质量,反射器可以由金属网或金属化塑料薄膜构成。这种结构几乎没有固有的机械刚性,但刚性可以通过在许多点的表面挠度的反馈控制来实现。例如,对于具有平面的测地线反射器,对于孔径为D和焦距为D的天线,需要D/93控制点来实现rms表面公差E¿。考虑简单的静电执行器,它可以将所需的控制点数量减少10倍或更多。随着天线几何形状的调整以实现越来越精确的静电反射器图形控制,反射器将开始表现出瑞利-泰勒不稳定性。在这种不稳定状态下工作是有利的,因为可以实现D/¿,因此天线波束宽度和增益分别为M2, M-2和M4,其中M是成功稳定反射器偏转模式的数量。描述了该控制问题的起源和基本要素,并提出了一种控制方法。本文还描述了在一米见方的金属丝网上成功稳定三种模式的实验室演示,这表明小至1的静电图形天线可能实现1至10弧秒的波束宽度。
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Electrostatically-controlled large-aperture reflecting satellite antennas
A major practical limit to the size of antennas in space is the minimum feasible mass per unit reflecting area. To achieve low antenna mass the reflector could be constructed from a wire mesh or metalized plastic film. This structure has little inherent mechanical rigidity, but rigidity can be achieved by feedback control of surface deflections at many points. For geodesic reflectors with flat facets, for instance, D/93¿¿ control points are required to achieve an rms surface tolerance of E¿ for an antenna with aperture diameter D and focal length ¿D. Simple electrostatic actuators are considered which can reduce this required number of control points by a factor of 10 or more. As antenna geometry is adjusted to achieve increasingly precise electrostatic reflector figure control, the reflector will begin to exhibit Rayleigh-Taylor instabilities. It can be advantageous to operate within this unstable regime because achievable D/¿, and hence antenna beamwidth and gain, scale as M2, M-2, and M4 respectively, where M is the number of successfully stabilized reflector deflection modes. The origin and essential elements of this control problem are described and a control approach is proposed. A laboratory demonstration of three successfully stabilized modes on a meter-square wire mesh is also described which suggests that electrostatically-figured antennas with ¿ as small as 1 could perhaps achieve beamwidths of 1 to 10 arc-seconds.
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