By Bo Lehnert
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Extra info for A Revised Electromagnetic Theory with Fundamental Applications
20) 0 where ρk are small radii of circles centered around the origin ρ = 0 when G is divergent there, and ρk = 0 when G is convergent at ρ = 0. The case ρk = 0 will later be treated in detail. 20) have been obtained from integration of the local contributions dq0 , dM0 , dm0 , and ds0 to the total charge, magnetic moment, mass, and angular momentum. With the volume element dV = 2πρ2 (sin θ)dρ dθ these contributions become dq0 = ρ¯ dV , dM0 = 21 (sin θ) C ρ dq0 , dm0 = cw2 dV , and ds0 = Cρ (sin θ)dm0 .
1: Crude outline of a magnetic field configuration in the case of one magnetic island situated above and one below the equatorial plane θ = π2 . Only the upper half-plane is shown, and the figure is axially (rotationally) symmetric around the vertical axis θ = 0. In the interval θ1 θ θ2 there is a magnetic flux into the spherical surface ρ = (dashed circular line) being equal to the inward magnetic island flux only. The outward flux parts in the intervals 0 θ θ1 and θ2 θ π2 consist of the outward main flux, plus an outward island flux.
29) Chapter 6 A Model of the Electron 51 ˜ These relations can be considered to include an undeterfor small δ. ˜ mined but finite equivalent amplitude G0 ε−δ/3 . Since we are free to choose the magnitude of G0 , this holds whether or not δ approaches zero more strongly than ε. 29), and due to the fact that the ratio AAm s is close to unity, it is readily seen that the radial constant c0 becomes nearly equal to the Compton wavelength mh c divided by 6π. 3 Magnetic flux According to Eq. 30) which vanishes at θ = (0, π).