Practical Guige to Free Energy Devices

When an EMF is applied to a conductor, something akin to the domino effect is set up in the ethers. This
effect travels at the speed of light since it is produced in a similar manner.
That the source of electricity flowing in power lines as well as that produced by generators, comes from soft
particles which permeate and surround the area, has been proven during auroral displays. When aurora
activity is unusually high, transformers in Canada have been known to burn out and even explode. At the
same time, increase of current flow in power lines has been great enough to trip circuit breakers as far south
as Texas. As explained earlier, the concentration of soft electrons in the atmosphere is greatly increased
during auroral phenomena. Some areas receive higher concentrations than others at the same latitude.
A loop of wire or a coil offers impedance to alternating current. This property is known as “inductance”.
Since a single loop of wire has inductance, it follows that the effect can be explained in terms of one loop.
Electrons tend to travel along the surface of a conductor as that is the path of least resistance. The major
source of this electricity is the high concentration of soft electrons which gather around a conductor and
permeate the material. This is due to the relatively high positive charge of the conductor. The greatest
concentration is found at the surface and a short distance below the surface. When an EMF is applied to the
conductor, free electrons are set in motion. During this process, soft electrons concentrated at and just
below the surface tend to disintegrate and release more hard electrons. This is enhanced by the
concentration of the soft electrons, which is turn causes an agitation of the soft particles, causing them to
become highly unstable.
In a straight wire, most of this disintegration and nearly all of the electron flow takes place below the surface.
This condition greatly shortens the mean free path of the electrons and the flow stops immediately after the
applied EMF is shut off. Consequently, an alternating current will encounter the same ohmic resistance in a
straight wire as will a direct current. However, the situation is different when the conductor is looped.
When an EMF is applied to a loop, the free or released hard electrons below the surface are forced to the
outside by centrifugal force, whence a still greater disintegration of soft electrons occurs because the
greatest concentration is at the surface. The mean free path of the electrons is greatly increased and the
flow continues for a brief period after the EMF travelling in the direction of the current flow ceases. When the
EMF continues in the opposite direction as in the case of an alternating current, the force must oppose the
momentum of the electron flow still continuing in the opposite direction to that of the new EMF direction. It
follows that this impedance will be directly proportional to the number of turns and to the frequency of the
AC. It is logical to assume that the deceleration rate of the electron flow is a constant when the EMF is zero.
This means that the more quickly that the EMF is applied in the opposite direction, the higher the velocity of
flow that will be encountered. It will be a linear function.
It would now seem evident that when the AC is rectified of has been changed to a pulsed DC, the coil will
produce an increase in amperage where a straight wire will not. Experiments have confirmed this. It was
found that the input amperage of a current was greatly increased after it passed through a coil. The increase
was greatest during the initial stage of the applied EMF and soon dropped to a lower value as the
concentration of soft electrons around the wire was reduced. It follows that a coil will offer impedance only to
an AC current. It follows that pulsed DC has numerous advantages over AC. It can be used to operate
transformers as well as AC without suffering impedance.
A steady direct current experiences the same resistance in a coil as it does in a straight wire of the same
length. The fluctuating EMF produces extreme agitation of the soft electrons around and inside the wire,
resulting in the disintegration of a large percentage of them, and the release of a high concentration of hard
electrons. This does not occur during the steady flow of direct current. During the initial application of DC
there is a surge of additional current during the build-up of the EMF. When the current is shut off, there will
be a momentary surge of current in the opposite direction. The excess of electrons on the surface of the
conductor and in the coil will naturally flow towards the void outside the coil and in the opposite direction to
which the current was flowing. The concepts just outlined can be applied when building a self-sustaining
electric generator.
When an alternating current is applied to a coil, the EMF must overcome the impedance each time the EMF
changes direction. The greatest amount of resistance occurs at the beginning of each change and then
steadily decreases as the current builds up. The resistance will be at a minimum when the current reaches
it’s maximum. With AC, the EMF changes direction very frequently and so the maximum resistance is
encountered for a high percentage of the time.
The flow of electrons in a wire results in a circular magnetic flow around that wire. As mentioned previously,
the magnetic effects between electrons moving together tend to cancel each other out. They are drawn
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