重力和电磁的单一复势

Riadh H. Al Rabeh
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引用次数: 1

摘要

据说,引力和静电之间的相似性止于支配两者的平方反比定律,甚至在引入广义相对论之后,这一点也受到了争议。一些人声称,定律本身的形式只是球体表面上的力变薄的结果,它随着远离源的半径的平方而增长。我们在这里表明,这种相似性实际上是更基本和更深刻的,因为这两种现象的单一起源,即电磁辐射,这一定是引力也以光速传播的原因。在[1]中,辐射被看作是蒸发的物质,而物质被看作是凝聚的辐射,因为辐射携带着电学和力学属性,当以拓扑EM孤子的形式凝聚时,它会导致质量、重力、电荷、本然自旋和偶极矩等其余物质属性的出现。引力和电的平方反比定律以缩合形式简单地作为动量守恒的直接结果[1]出现。这是一个基本的联系,但它留下了一个重要的区别。相似的质量相互吸引,而相似的电荷相互排斥。然而,如果我们把质量当作一个假想的电荷,那么类似的质量就会像电荷一样相互排斥,从而达到完全的相似。由于重力场具有这样的虚值,它们的平方和它们的作用力仍然是真实的。然后用它来为这两种现象中的每一种构建潜在的表示。用通常的迟滞势积分推导出类重力场的完整集合
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A single complex potential for gravity and electromagnetism
The similarity between gravity and static electricity is said to stop at the inverse square law that governs the two, and even that was disputed after the introduction of GR. Some claimed that the form of the law itself is only the result of the thinning of forces over a spherical surface that grows as the square of the radius away from the source. We show here that the similarity is in fact much more fundamental and deep because of the single origin of the two phenomenanamely EM radiation, which must be why gravity too travels at the speed of light. In [1] radiation was visualized as evaporated matter and matter as condensed radiation, since radiation carried electrical as well as mechanical attributes and when condensing in the form of a topological EM soliton, it causes the emergence of the rest of the matter attributes of mass, gravity, charge, intrinsic spin and dipole moment. The inverse square law for both gravity and electricity then appears simply as a direct consequence of momentum conservation in the condensed form [1]. This is a fundamental connection, but nonetheless it leaves one important difference. It is that similar masses attract whereas similar charges repel. However, if we took mass to be an imaginary electric charge, similar masses would repel as for electric charges and a complete similarity is achieved. With gravity fields having such imaginary values, their squares and their force effects remain real. This is then used to construct potential representations for each one of the two phenomena. The usual retarded potential integral is followed to derive a full set of fields for gravity like
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