在国际单位制、海维塞德-洛伦兹制和高斯制之间转换方程的简单方法

Paul Quincey
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摘要

学校和本科生几乎总是使用一套称为 SI 的约定来学习电磁学方程。高年级学生通常会接触到不同的约定,这些约定使用高斯系统或海维斯-洛伦兹系统为相同的关系产生不同的方程。一般来说,这些方程之间的联系并不简单。不过,如果理解了每个系统的基础,将国际单位制方程转换为高斯或海维斯-洛伦兹方程就会非常简单。反向过程则不那么简单,但如果理解了两者的根本区别,就更容易理解了。本文介绍了这些过程的简单方法,使用了一种新颖的维度分析应用,不会出现 ε01/2 或 (4πε0)1/2 因子。这也表明,当不同的物理量被赋予不同的符号,并且这些符号被一致地使用时,可以看出 SI 提供了一般方程,而高斯方程和海维斯-洛伦兹方程是对它们的简化。这就不再需要 "与系统无关 "的电磁方程版本,因为不同系统中的附加参数取值不同。
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Simple methods for converting equations between the SI, Heaviside-Lorentz and Gaussian systems
School and undergraduate students are almost always taught the equations of electromagnetism using a set of conventions that are described as the SI. More advanced students are often introduced to different conventions that produce different equations for the same relationships, using either the Gaussian or Heaviside-Lorentz systems. In general, the connection between these equations is not simple. However, if the basis of each system is understood, conversion from SI equations to either Gaussian or Heaviside-Lorentz ones is very straightforward. The reverse processes are less straightforward, but more comprehensible when the fundamental differences are understood. Simple methods for these processes are presented, using a novel application of dimensional analysis, without factors of ε01/2 or (4πε0)1/2 appearing. It is also shown that when different physical quantities are given different symbols, and these are used consistently, the SI can be seen to provide general equations, with the Gaussian and Heaviside-Lorentz ones being simplifications of them. This removes any need for ‘system-independent’ versions of electromagnetic equations, with additional parameters that take different values in the different systems, which have been proposed in various forms over many decades.
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