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The electrostatic characterization of an n-element planar array using the singularity expansion method

机译:使用奇异展开法对n元素平面阵列进行静电表征

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In this paper, the singularity expansion method (SEM) is used to describe the electrostatic charge distribution on an array of thin linear antennas placed in a uniform electric field. The SEM, which has primarily been used to analyze transient scattering problems, decomposes the electromagnetic interaction process into various quantities such as singularities and modes. Using the SEM, the step plane wave induced transient current on the array is expanded in terms of its singularities (poles) in the Laplace transform (complex frequency domain.) The continuity equation is applied to the induced current expression to obtain the transient charge. The electrostatic charge distribution on the array is found by using the final value theorem on the transient charge expression. It is well known that the SEM factorization of a single linear element reveals that a single pole exists in the fundamental resonance region (near ωL/c = π, where L is the length of the scatterer). For a two-element array, two poles are observed in the fundamental resonance region. This trend continues such that an n-element array has n poles in the fundamental resonance region. Associated with each pole is a unique modal current and corresponding charge distribution. For example, one of the two fundamental resonance region poles of the two-element array produces half-wavelength sinusoidal current distributions whose directions are the same on one scatterer but opposite on the other. The remaining fundamental resonance region pole produces half-wavelength sinusoidal current distributions whose directions are the same on both scatterers. Corresponding to each mode is a coupling coefficient which determines how much a particular mode couples into the response. A generalization of these results for an n-element array will be given. Furthermore, the electric polarizability is derived in terms of the SEM electric charge description. The value of this research lies in the elegance and strength of the SEM to factor a problem into various quantities which depend on different variables of the problem. By using the SEM to analyze the n-element planar array, a much deeper comprehension of the fundamental aspects of the electrostatic interaction process is achieved.
机译:在本文中,奇异扩展法(SEM)用于描述放置在均匀电场中的细线性天线阵列上的静电荷分布。 SEM主要用于分析瞬态散射问题,它会将电磁相互作用过程分解为各种数量,例如奇异度和模式。使用SEM,在Laplace变换(复频域)中,根据其奇异点(极点)扩展了阵列上的阶跃波感应瞬态电流。将连续性方程应用于感应电流表达式以获得瞬态电荷。通过使用关于瞬态电荷表达的最终值定理,可以找到阵列上的静电荷分布。众所周知,单个线性元素的SEM分解显示出一个单极存在于基本共振区域中(在ωL/ c =π附近,其中L是散射体的长度)。对于两元素阵列,在基本共振区域中观察到两个极点。这种趋势继续,使得n元件阵列在基本谐振区域中具有n个极。与每个极相关的是唯一的模态电流和相应的电荷分布。例如,由两个元件组成的阵列的两个基本谐振区域极之一会产生半波长正弦电流分布,其在一个散射体上的方向相同,而在另一个散射体上的方向相反。其余的基本谐振区域极点会产生半波长正弦电流分布,其两个散射体的方向相同。与每种模式相对应的是耦合系数,该系数确定特定模式耦合到响应中的程度。将给出这些结果对n元素数组的概括。此外,电极化率是根据SEM电荷描述得出的。这项研究的价值在于SEM的高雅性和强度,可以将问题分解为各种数量,这些数量取决于问题的不同变量。通过使用SEM分析n元素平面阵列,可以更深入地理解静电相互作用过程的基本方面。

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