Gill's electronic theory of magnetism (1964) was put forward by the author to explain a change in configuration of the atoms which then start to behave like magnets. The author does not agree with the pre-existing dipole theory of Maxwell (1873). By applying Gill's electronic theory of magnetism (1964) to Faraday's (1831) iron ring experiment, the unexpected result obtained by Michael Faraday in 1831will be explained. Using Coulomb's law, dot-product calculations and equations have been

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... d by the author versus the cross-product Lorentz equations ( 1893 ). Magnetism and the Tesla unit will be addressed and it will be shown with the help of Coulomb's law that if we have 𝒏 = 𝟏 𝒌.𝒆 =( 𝒌. 𝒆)⁻¹ non-moving inner electrons at the north magnetic pole and have at a distance of one meter the same number of exposed protons as the south magnetic pole, then we will experience a magnetic force of one Tesla between the two magnetic poles. The issue of asymmetry between magnetic force and electrical force pointed out by A. Einstein in 1905 and Richard Feynman in 1943 is resolved by applying Gill's electronic theory of magnetism (1964) instead of Maxwell's dipole theory of magnetism (1873). Introduction: This article has been written to explain the results obtained by Michael Faraday in his 1831 iron ring experiment with the application of Gill's electronic theory of magnetism (1964). The ability to do the same also lends support to Gill's electronic theory of magnetism. It will be shown with line diagrams and a simple experiment that the magnetic force is a combination of positive and negative forces from the protons and electrons of a re-configured magnetized atom. The author will go on to derive dot product calculations and equations after having failed to reconcile with the cross-product Lorentz formula of 1893. The derived equations are applied to define and calculate a Tesla unit. Maxwell's dipole theory of magnetism (1873) causes the asymmetry issue and it will be shown that Gill's electronic theory of magnetism resolves the asymmetry issue. Conclusion: Application of Gill's electronic theory of magnetism (1964) shows how a centrifugal force is created and manifests and travels on the surface from the northpole to the south pole of a magnet during magnetization and in the opposite direction during demagnetization and manifests only at the ends of a magnet otherwise. It will be shown that both during magnetism and electricity, the interaction is between positive and negative forces of an atom. During electrical current we have the free valence electrons flowing in the conducting coil. During magnetism, the atom undergoes a change in configuration between its electrons and protons. Dot product equations suffice. Method: Gill's electronic theory of magnetism (1964) will be summarized followed by a simple experiment to show that the fundamental magnetic force is a combination of proton based positive and electron based negative forces. Next, a simple thought experiment involving Faraday's iron ring experiment (1831) to show how opposite induction works. Next will be the actual Faraday's iron ring experiment (1831) and how the application of Gill's electronic theory of magnetism (1964) helps in explaining the magnetic induction followed by the electrical induction. This will be followed by dot product calculations developed by the author instead of the cross-product equations of Lorentz (1893). Finally, the asymmetry issue will be addressed and resolved if you apply Gill's electronic theory of magnetism instead of Maxwell's dipole dependant theory. GILL'S ELECTRONIC THEORY OF MAGNETISM (1964) This is based on the structure of the atom and explains how the positively charged protons and the negatively charged electrons are responsible for both magnetism and electrical forces. Faraday's iron ring experiment (1831) explained with Gill's electronic theory of magnetism (1964)