Bo Lehnert's A Revised Electromagnetic Theory with Fundamental PDF

By Bo Lehnert

ISBN-10: 9185917001

ISBN-13: 9789185917006

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40) when applying Eqs. 29). 40), and its counterpart of Eq. 2. 11) according to which the local relation IMθ Imθ = Iqθ Isθ is obtained. However, as has become obvious from the present analysis and Eqs. 23), the detailed deductions of the electron model do not become quite as simple. 50). Combination of Eqs. 41) where fΓq is the flux factor being required by the corresponding quantum condition. This factor should not be confused with the factor fΓf of Eq. 38) which results from the magnetic field geometry.

With this set of equations the iteration procedure can be performed according to the following scheme: • One first assumes some plausible initial values of q ∗ and h0 which both are of the order of unity; • With these values Eq. 58) becomes a linear relation between x and y; • Solving for x by means of Eq. 58) and substituting the result into Eq. 53). 51) are determined as well. This also applies to the two values of the flux factor which are obtained from the second and third members of Eq. 59).

20). The following analysis will show this to become possible, by shrinking the characteristic radius r0 to the very small values of a “point-charge-like” state. It does on the other hand not imply that r0 has to become strictly equal to zero, which would end up into the unphysical situation of a structureless point. 1) n T =1+ {a2 ν−1 sin[(2 ν − 1) θ] + a2ν cos(2ν θ)} = ν=1 = 1 + a1 sin θ + a2 cos 2 θ + a3 sin 3 θ + . . 1), it may at a first glance appear to be somewhat special and artificial.

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A Revised Electromagnetic Theory with Fundamental Applications by Bo Lehnert

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