真空中电荷密度和光速的运动

N. Yener
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引用次数: 2

摘要

作为作者过去关于无限光速可行性的肯定工作的延伸,这篇笔记着重于无限光速对在时间上突然开始的运动中的电荷密度的影响。在以前的工作中,证明了标量势和矢量势必须是非延迟的,或者对于这样的电荷密度,光速必须是无限的,这样标量势和矢量势才能满足麦克斯韦方程。这里发现,对于这种突然开始的电荷密度函数运动,麦克斯韦方程组将失效,即使电势没有迟滞。因为即使无限的c足以满足势的洛伦兹条件,当t=0时,它并不满足。然后就出现了面对不满足的麦克斯韦方程组的问题,因此必须在这些方程中引入额外的源项以使它们满足。可见,如果包含电荷和电流密度项,则无法达到这一目标,而需要磁荷和电流密度项作为唯一的手段。给出了确定所需磁源的步骤。这个问题被看作是解泊松方程的逆源问题。所引入的磁源所得到的电场和磁场是无延迟的。所得结果不仅适用于点电荷分布,也适用于连续电荷分布的情况。
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Motion of a Charge Density and the Speed of Light in Vacuum Revisited
As an extension of affirmative past work by the author on the feasibility of an infinite speed of light, this note focuses on the consequences of an infinite speed of light $c$ for a charge density in a motion that starts abruptly in time. In previous work it was proved that the scalar and vector potentials need to be non-retarded or speed of light must be infinite for such a charge density in order that Maxwell's equations be satisfied by the scalar and vector potentials. Here it is found that for this abruptly starting motion of a charge density function Maxwell's equations will fail even if the potentials are not retarded. For even though an infinite $c$ is sufficient for the Lorenz condition on the potentials to be satisfied when $t > 0$, it is not at $t=0$. Then there arises the problem of facing unsatisfied Maxwell's equations and hence the necessity of having to introduce additional source terms into these equations to render them satisfied. It is seen that with inclusion of electric charge and current density terms this objective cannot be attained, and magnetic charge and current density terms are needed as the only means. The steps for the determination of the required magnetic sources are given. The problem is seen to be reduced to that of solving an inverse source problem for Poisson's equation. The obtained electric and magnetic fields with the introduced magnetic sources are non-retarded. The obtained results apply to the case of a continuous charge distribution as well as a point charge.
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