4. Stationary Electromagnetic
Fields
//////Let us now admit that besides its
own spin the electron is able do develop a rotation movement on a parallel
plan to its spin, that is, a plan containing vector w,
as in picture 1. Being a uniform movement, we should expect that
after reaching this status the electron would keep this new inertial
movement, not depending on energy. What could we say about this new field A
to be observed?
//////Every instant the electron emits e.m.i.
towards all directions in space and informs the momentary orientation of
its vector w. If under these conditions w
spins clockwise on the paper, field A, at a given moment, will have
its pictorial representation given by picture 4. At every point
field A pictures a piece of information about a recent past, its
orientation being dephased in relationship to orientation of w
according to a function dependent on r (distance from the considered point
to the electron).
//////In picture 4 we show the A
vectors which are dephased from multiples of p/4
radians in relationship to a w, with
just the vector orientation being represented, but not its modular
dependence relative to r (this effect would be likely the one presented in
picture 1). As time advances vector A, at every point, spins
around itself as if it were emulating the movement of vector w
(picture 5).
Picture 5: Stationary
field A of a spinning electron.
Click in the image for amplification.
//////There is an intimate kinship
between the presented image and the one described in books and relative to
classical fields E and B of the so-called “electromagnetic
wave” circularly polarised in Maxwell’s theory. In contrast with it, I
would say that an observer in the spinning referent following this
secondary spin of the electron (own referent) will receive a similar image
for field A, but also stationary (for this observer, field A
does not spin around itself).
//////In order to understand some of the
possible limitations or restrictions imposed by the model in pictures 4
and 5, we should imagine for the electron a spin of 1,000 rotations
per second, which actually a relatively high value. Under these
conditions, the last point represented in picture 4 would be 300 km
from the electron (assuming c = 300,000 km/s); for smaller rotations, this
distance will be proportionally longer. Whatever this distance, depending
only on the intensity of the spin, another particle on this peripheric
point trying to keep in phase with the central electron, revolving around
it on the figure’s plan, should have a speed superior do six times the
speed of light (exactly equal to 2pc), which
would surely exclude this orbit of a possible relationship contemplating
the probable candidates to “allowed orbits”.
Picture 6: An unlikely orbit for an electron around other.
Click in the image for amplification.
