Page 273 - The Final Appeal to Mankind
P. 273

«The Final Appeal to Mankind» by Nicolai Levashov

            In  general,  conductors  have  unstable  electron  structures;  they  tend  to  keep
            combining and dissociating. Their entire system is in motion  – albeit this type of

            motion  is  chaotic.  Interestingly  enough,  however,  electrons  do  not  move  inside  a
            conductor.  The  external  (electromagnetic)  field  deforms  the  atom's  microspace
            curvature, increasing the electrons' instability and triggering their disintegration. This
            results  in  the  overflow  of  their  constituent  primary  matters  onto  the  etheric  level,
            where, still under the influence of the external field, they are forced to flow in a given
            direction.


            In  the  process  of  this  forced  overflow,  the  primary  matters  lose  a  portion  of  their
            energy, which leads to a new fusion of primary matters in still another area of the atom's
            microcosmic curvature – hence the synthesis of a new electron takes place.

            Thus, the movement of electrons along a conductor is really a periodic back-and-
            forth flow from physical to etheric and etheric to physical levels.

            This also accounts for the so-called tunnel effect, which occurs when crystal lattices
            of various types join together (as in the case of semiconductors), when correct external

            conditions are present; i.e., when the distance between the point of disintegration and
            the point of electron synthesis falls within the range of a fraction of a millimeter to
            several millimeters. When this occurs, that particular interval marks the “still zone” –
            where the flow of primary matters from physical to etheric levels does not occur.

            The above condition arises when there is a marked difference between the electron
            structures of the crystal lattices that make up a semiconductor (see F Fi ig g. .   1 14 48 8).












































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