According to the Quantum Physics Model, the subatomic particles have
electrodynamic double toroidal spin (rmfd). In simpler terms, this is a
bi-rotational magnetic field. This same dynamic structure also applies to
the Aether. The conductance of the
Aether is actually equal to the speed
of light divided by rmfd:
Cd = c / rmfd
My theory is that if subatomic particles and the Aether have a natural
bi-rotational magnetic field, then there must be a practical way to harness this
heretofore unknown quality of both subatomic particles and the Aether.
As an experiment, I propose using two flat spiral coil parallel to each other
to generate the conditions that closely resemble the subatomic structure (as
described in the Quantum Physics Model.) But first I'll examine the
magnetic field of a single flat spiral coil. Figure 1 is the flat spiral
wound coil with no voltage applied:

Figure 1
Magnetic north is the earth magnetic north. In figures 2
and 3 a DC power supply of 12V, 1.2A is applied between the outer lead and
center post of the coil. Magnetic north now points toward the center of
the coil.
Figure 2
|
Figure 3
|
I also tried a 12v, 3A AC power supply. The AC power
supply would point either the south pole or the north pole of the compass toward
the center of the coil, depending on which way it was oriented before entering
the coil's magnetic field. This indicates that an AC current has the same
effect as a DC current except that it alternates, which is what would be
expected. But since the AC current is ambiguous, I'll do the rest of the
testing with the 12v, 1.2A DC power supply. This will clearly depict the
magnetic field of the single wound flat spiral coil.
In figures 4 and 5 the magnetic field of the underside of the
coil is depicted. Oddly, the south pole points to the center of the coil
on the underside. This indicates that the center of the coil is not a
magnetic pole at all. If it were, then both the bottom and the top would
point north to the center.
Figure 4
|
Figure 5
|
So the magnetic field in a flat spiral coil is not polar, but is
continuous. To get a better idea of what this magnetic field looks like, I
turned the compass up on edge and measured the direction of the magnetic field
for several points from the outer edge toward the center of the coil.
Figures 6 through 12 show the results.
Figure 6
|
Figure 7
|

Figure 8

Figure 9

Figure 10

Figure 11

Figure 12

Figure 13
The north magnetic "pole" of the flat spiral coil
points slightly upward and toward the center of the coil when it is outside the
winding area. At a circle marking the line where the surface area of the
inner windings is 3/4 of the total surface area, the north magnetic
"pole" on the top side is perfectly horizontal to the coil and
pointing toward the center. From there it gradually angles downward until
at the center of the flat spiral the north "pole" is pointing
downward. These readings were also done on the bottom side of the coil
with the same exact magnetic field characteristics except that north was away
from the center of the coil.
With this type of magnetic field around a flat spiral coil it
occurred to me that this coil geometry is conducive to producing the rmfd.
My theory is that winding the same type of coil under this coil, with the
thickness of 1/4" Plexiglas between the windings, would produce two
opposing magnetic fields. In the top coil magnetic north will point down
through the center of the top coil and in the bottom coil magnetic north with
point up through the center of the bottom coil. The two fields will meet
and repel each other. In between the two coils will be two different
magnetically north aligned magnetic fields trying to get out toward the outer
edge of the spirals. These two fields will be of the same polarity and in
an effort to repel each other, the top magnetic field will develop a clockwise
orientation and the bottom magnetic field will develop an counter-clockwise
orientation. These two magnetic fields will be pointing in opposite
directions and thus attract each other to hold this bi-rotational magnetic field
orientation.
The question in my mind is whether this combination of forces
will cause a static rotating magnetic field or a dynamic rotating magnetic
field. At this point have just wound another spiral coil on the underside
of the above pictured coil. As soon as the coatings have dried, I will
test for rotating magnetic fields and other characteristics and post them as a
follow up to this page.
The Results
04/22/03
The finished coil is 13" in diameter with a 1/4" brass
post in the center. Both sides of the coil are identical and wound in
complete parallel. When measuring the inductance with an LCR meter, the
inductance is 1.111mH. The resistance of the coil is 9.31 Ohm. The
total wire length as calculated by the geometrical formula is about 976
feet. Calculated by the DC resistance of 21 gauge wire, the wire length is
about 925 feet.
When a DC current of 12 volt, 1.2A is applied to the two
terminal wires, no current passes through the coil. Also, when an AC
current of 15KV, 30mA was applied to the two terminal ends, no current flowed
through the coil.
Applying a 24 volt, 30A current through the coil produced a weak
magnetic field. The magnetic field pattern of the coil produced the
opposing magnetic fields the experiment was intended to produce.
It is apparent that this coil will require a specific voltage
and current in order to produce the rotating magnetic field. Further
research is needed to derive the exact electromagnetic power source
needed. Since I don't have a variable high voltage DC power supply for
trial and error experimentation, I'll first attempt to derive the equation using
the Quantum Physics Model.