In electrodynamics we find that \u201cA quantum-mechanical description of photons necessitates quantization of only the vector potential\u201d ([1], pg. 242), as in the summation of all the manifolds of gravitational fields at a given location. In a more densely packed summation of manifolds, the action of an electric charge will have a lesser rotational effect on the electric fields of the gamma rays than on a less dense field. The power of the rotation is the same in either field however, as long as we are referring to a gravitational field that is not too sparse for electric fields to propagate.<\/p>\n\n\n\n
\u201cThe definition of B<\/strong> = \u2207 x A<\/strong> specifies the curl of A<\/strong>, but it doesn\u2019t say anything about the divergence \u2013 we are at liberty to pick that as we see fit, and zero is ordinarily the simplest choice.\u201d ([2], pg. 235) The reason we may pick the divergence as zero is that the manifolds \u201care frozen in time for phonon transmission\u201d:<\/p>\n\n\n\n https:\/\/www.fruechtetheory.com\/blog\/2022\/03\/29\/transmission-of-the-coulomb-field\/<\/a><\/p>\n\n\n\n As far as group action, Mackenzie [3] calls these \u201cgroupoids\u201d, such as an ellipsoid, a spheroid, or another 3-dimensional shape. The definition of a spheroid I find is that it is like a sphere, but not a perfect sphere, and in the present case we have \u201coscillations and accordion motion in multiple axes\u201d:<\/p>\n\n\n\n