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Three-dimensional Reconstruction of the Electric Tree in Oil-impregnated Pressboard Based on Partial Discharge Location

机译:基于局部放电位置的油浸式压板中电树的三维重建

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There is still a lack of effective means of observation for electrical trees in opaque materials, which presents a great obstacle to the accurate diagnosis and prediction of partial discharge (PD) defects. As an effective tool to solve the field source, inverse problem has also been applied to the reconstruction of electrical tree. Therefore, the accuracy of solving the inverse problem of electrostatic field is verified theoretically. Firstly, the PD is equivalent to point charge, and the inverse problem equation is established, which takes the position of the point charge as the unknown quantity and the field strength of the measured point as the known quantity, and is solved by PSO. The error range of PSO can be calculated by randomly changing the position of charge source, and then 10 groups of noises (1% ~ 10%) can be added to the electric field value of the measurement point to fix the position of charge source. The influence of different noise levels on the calculation error and the variation rule of positioning error with noise level are analyzed. Through statistical analysis, it is concluded that the error range of each variable calculated by PSO is very small $(< mathbf{4.5}%)$, which verifies the accuracy of inverse problem solving; the calculation error of variables $pmb{x},pmb{y},pmb{z}, pmb{q}_{mathit{1}}$ increases gradually with the increase of noise level, and the root mean square error of each coordinate $pmb{S}_{pmb{x}} > pmb{S}_{pmb{y}} > pmb{S}_{pmb{z}}$.
机译:仍然缺乏不透明材料的电气树木观察的有效手段,这呈现了局部放电(PD)缺陷的准确诊断和预测的巨大障碍。作为解决场地源的有效工具,逆问题也已应用于电气树的重建。因此,理论上验证了求解静电场逆问题的准确性。首先,Pd等同于点电荷,并且建立了逆问题等式,这使得点电荷的位置作为所知点的未知数量和现场强度,作为已知量,并由PSO解决。 PSO的误差范围可以通过随机改变电荷源的位置来计算,然后可以将10组噪声(1%〜10%)添加到测量点的电场值以固定电荷源的位置。分析了不同噪声水平对计算误差和噪声水平定位误差的变化规律的影响。通过统计分析,得出结论,PSO计算的每个变量的误差范围非常小 $(< mathbf {4.5 } %)$ ,验证逆问题求解的准确性;变量的计算误差 $ pmb {x}, pmb {y}, pmb {z}, pmb {q} _ { mathit {1}} $ 随着噪声水平的增加而逐渐增加,每个坐标的根均方误差 $ pmb {s} _ { pmb {x}}> pmb {s} _ { pmb {y}}> pmb {s} _ { pmb {z}} $

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