Koen J. van Vlaenderen

arXiv2003

A generalisation of classical electrodynamics for the prediction of scalar field effects

Within the framework of Classical Electrodynamics (CED) it is common practice to choose freely an arbitrary gauge condition with respect to a gauge transformation of the electromagnetic potentials. The Lorenz gauge condition allows for the derivation of the inhomogeneous potential wave equations (IPWE), but this also means that scalar derivatives of the electromagnetic potentials are considered to be \emph{unphysical}. However, these scalar expressions might have the meaning of a new physical field, $\mathsf S$. If this is the case, then a generalised CED is required such that scalar field effects are predicted and such that experiments can be performed in order to verify or falsify this generalised CED. The IPWE are viewed as a generalised Gauss law and a generalised Ampere law, that also contain derivatives of $\mathsf S$, after reformulating the IPWE in terms of fields. Some recent experiment show positive results that are in qualitative agreement with the presented predictions of scalar field effects, but further quantitative tests are required in order to verify or falsify the presented theory. The importance of Nikola Tesla's pioneering research, with respect to the predicted effects, cannot be overstated.

physics.class-ph↗

arXiv1999

A charged space as the origin of sources, fields and potentials

The wave function $ψ$ is interpreted as charge density, or charge distribution, at each point in space. This is a physical interpretation of $ψ$. The notion of speed can be associated with $ψ$, which leads to the concept of conduction currents and (displacement) convection currents. The charge distribution is the origin of electrical and mechanical sources, potentials and fields. The notion of self potential is essential for defining electrical or mechanical sources. Maxwell's equations are derived from the condition of charge conservation and mass conservation. There are two methods of modelling the mass of a charge: The mass of a charge is its electrostatic energy. The mass of a charge is the energy of the Zero Point Field (ZPF) that interacts with the point charge. It is shown that the two models are related by a simple energy equation for a particle at rest.

physics.gen-ph↗