电磁场传感器工作条件下介电常数变化差对影响系数的精细计算

S. Kolmogorova, S. Biryukov, D. Baranov, A. Kolmogorov
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引用次数: 0

摘要

这是永远不会确切知道将在何处使用已开发的仪器。开发人员在设计时必须考虑运行条件,确定对测量结果的影响因素,以获得最可靠的结果。本文介绍了在外界条件下,利用介电常数的差异计算电磁场传感器校正系数的数学方法。计算进行了评估,以及其对传感器计量特性的影响,使估计使用误差成为可能。建立了一个由一组积分方程组成的数学模型。这些方程的基础是误差与敏感元件的角尺寸、传感器外壳的介电常数和环境的函数依赖关系。数学模型的基础是一个系数$\alpha$,该系数考虑了传感器外壳和环境的介电常数差异。利用建立的数学模型,根据传感器单位体积的归一化能量值(敏感电极的角尺寸$\theta_{0\mathrm{I}}$和$\theta_{02}$)以及传感器基底与环境的介电常数的不同比值,得到数据和图。在这些依赖关系的图中,可以观察到最大值。这些最大值对应于传感器的每单位体积的最大能量,其球形段的特定角度尺寸($\theta_{0\mathrm{I}}$和$\theta_{02}$)和参数$\alpha$的恒定值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Refined Calculation of the Influence Coefficient from the Changes difference in Dielectric Constant from the Operating Conditions of the Electromagnetic Field Sensors
This is never exactly known where a developed instrument will be used. The developer must take into account the operating conditions during the design and determine the influencing factors on the measurement result to obtain the most reliable result. The article describes the mathematical calculation of the correction coefficient of the electromagnetic field sensors by the difference in dielectric constant in the external conditions. The calculation is evaluated, as well as its influence on the metrological characteristics of the sensor making it possible to estimate the error of use. A new mathematical model consisting of a system of integral equations is constructed. The basis of these equations is the functional dependence of the error on the angular dimensions of the sensitive elements and the dielectric constant of the sensor housing and the environment. The basis of the mathematical model is a coefficient $\alpha$ that takes into account the difference dielectric permittivity of the sensor housing and the environment. Using constructed mathematical model, data and plots are obtained depending both on normalized energy value in unit volume of sensor from angular sizes $\theta_{0\mathrm{I}}$ and $\theta_{02}$ of its sensitive electrodes, and from different ratios of dielectric constants of sensor base and environment. In the plots of these dependencies, maxima are observed. These maxima correspond to the maximum energy per unit volume of the sensor for specific angular sizes of its spherical segments ($\theta_{0\mathrm{I}}$ and $\theta_{02}$) and for constant values of the parameter $\alpha$.
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