Note 388(2): Complete Theory for Circuit Vacuum Interaction

The complete set of equations are Eqs. (19) and (20). Any measured quantity in electrodynamics always has a contribution from the vacuum. This is well known through the radiative corrections, observed to be very small. So the approximation (22) is used as a starting point, that the experimentally measured charge current density in a circuit is approximately the intrinsic quantity. Using this approximation the theory can be worked out entirely as shown, and any quantity of interest graphed. It becomes clear that the nineteenth century Maxwell Heaviside (MH) theory is incomplete because it obviously did not account for the radiative corrections (vacuum effects) of the mid nineteen forties. This was first shown in UFT131 ff, and the failure of MH is summarized in Eqs. (8) to (11). A theory can never be free of the spin connection. I will repeat this development for gravitation and proceed to write up UFT388, Sections 1 and 2. The interaction equation column (20) produces everything in electrodynamics and optics that the intrinsic MH equations can (column (19)). This includes various types of very well known resonances, radiation theory, everything in any textbook. So column (20) is a new subject area, the field equations of circuit vacuum interaction. Equation columns (19) and (20) reduce to electrostatics and magnetostatics in the usual way, when the Maxwell displacement current vanishes. Conservation of antisymmetry (CA) produces the spin connection and an entirely new subject area. CA refutes all aspects of the MH theory and standard model U(1) electrodynamics. It therefore refutes U(1) x SU(2) electroweak theory and U(1) x SU(2) x SU(3) standard unified field theory and Higgs boson theory. This entire development can be repeated with the Proca equation and photon mass theory, leading to an understanding of B(3) in terms of matter to vacuum interaction.

a388thpapernotes2.pdf

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