The thorny way of truth - Free Energy Community

- 117 -ting the charges of the first and second particles by q^, q^ and their velocities inabsolute space by ¥j, ^^ which, if measured on a clock which rests in absolute space,are called their universal velocities:(see, however, my comments to Pappas1. COULOMB-NEUMANN ELECTRIC AND MAGNETIC ENERGIES article published in this volume)U + W = (qjq2/c^r)(c^ + VJ.V2) = (qjq2/c^r)(CjC2 + ^y^^^.where v,, v^ are called also universal space velocities of the particles, c^ = c, C2 = care called their universal time velocities and are equal to the universal light velocity2 2 -1/2(however, the proper time velocities of the particles c , = c(l-v,/c ) ,2 2 -1/2c 2= c(l - vt/c ) are not equal one to another), and r is the distance between theparticles.AsVj = (Vj, ic), V2 = (V2, ic)are the 4-velocities of the particles (the univi?rsa1 4-velocities), we haveW - U = (qiq2/c^r)(Vj.V2 - c^) = (qjq2/c^r)Vj.V2.The here indicated notations are introduced by me and many of the notions are attributesof my absolute space-time theory (see my CLASSICAL PHYSICS).Thus the Coulomb- Neumann electric and magnetic potential energies are the basis ofthe 4-dimensional approach to electromagnetism which presents the electromagnetic formulasin a very elegant. and compact way unifying the space and time characteristics ofthe particles (see CLASSICAL PHYSICS, volumes 3-5).When proceeding from the Coulomb-Neumann potentials, the force with which two electriccharges (two current elements) act one on another is given by the Grassmann formula.2. COULOMB-WEBER ELECTRIC AND MAGNETIC ENERGIESU . W = (qiq2/c^r)Cc2 - {[y^-s^).T\^IZr^ ^ - HlSZ^^ - 1(^)2}.When proceeding from the Coulomb-Weber potentials, the force with which two electriccharges (two current elements) act one on another is given by Ampere formula.3. COULOMB- RIEMANN ELECTRIC AND MAGNETIC ENERGIESU + W = (qjq2/c^r){c^ - (V2 -v^)^}.It is not clear to me whether the term (V2-Vj) must be divided by the factor 2 (Irather think that it must be divided) and with which force two charges (two currentelements) act one on another when proceeding from the Coulomb- Riemann potentials.As far as I know, in his Course on Theoretical Physics, Prof. God of the Champs ElyseesUniversity works only with the Coulomb-Neumann potentials and with Grassmann 's formula.'