Practical Guige to Free Energy Devices

inductance, in a receiver, between the aerial and the ground, and a tuned collector coil resonates to increase the
sensitivity and the amplitude of the signal.
4. The full-length electromagnetic transformer unit of claim 3, where the tuned transmitter coil resonates with an
oscillator and an aerial to act as a transmitter for radios, televisions, cell phones, radars and computers.
5. The full-length electromagnetic transformer unit of claim 1, where the lengths of the sheaths are some multiple
of the wave length of a particular electromagnetic frequency.
6. The full-length electromagnetic transformer unit of claim 5, where a number of the units are connected in
parallel to increase the current.
7. The full-length electromagnetic transformer unit of claim 5, where a number of the units are connected in series
to increase the voltage.
8. The full-length electromagnetic transformer unit of claim 5, where the parts are reduced to a size small enough
to fit in, and supply power to, a cell phone, a lap-top computer, or other electrical appliance.
9. The full-length electromagnetic transformer unit of claim 1 further comprising three or more, metallic, parallel,
side by side, pipe like sheaths, where the sheaths are not electrically connected, and have two or more coils
wound inside the sheaths.
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Up to the present time (June 2013), I have not heard of anyone attempting to replicate the design shown in this
patent, and so it is just being put forward here in case somebody wants to try it. It appears to be a clever
technique. The power gain is maximised by tuning the transmitting and receiving coils to the frequency of the
oscillator, although in practice, it is highly likely that the oscillator frequency would be adjusted to the transmitter
coil as it is so easy to adjust the frequency of an oscillator.
Boyd does not go into great detail about attaining resonance, and that is generally a major difficulty in any design
which does not have automatic tuning. It needs to be borne in mind that the length of wire in each coil (and
possibly its weight) is a key factor. Boyd talks about the coils possibly having the same number of turns, and that
is fine provided that the coils are identical in size, that is, having the same shape when viewed from the top and
the same depth of turns when viewed from the side, and exactly the same number of turns with each coil having
exactly the same wire length. Resonance in a length of wire, whether it is laid out straight or wound into a coil,
tends to confuse many people. Richard Quick’s very clear explanation of resonance in any length of wire, in his
US patent 7,973,296 of 5th July 2011 is very helpful. He says:
“Quarter-Wave” Resonance; Standing Electromagnetic Waves”
One of the two main types is electrical resonance is referred to here as quarter-wave resonance. This type of
resonance depends almost entirely on the length of a wire element For reasons described below, if a segment or
length of wire is one quarter as long as the “voltage waves” which are travelling through the wire, then a set of
“reflected” waves will be added to the emitted waves, in a synchronised alignment which creates stronger
“superimposed waves”.
Accordingly, an understanding of the “quarter-wave” phenomenon will help a reader understand how a
straightforward and easily-controlled factor (i.e., the length of a wire ribbon which will be used to form a spiral coil)
can help create a “quarter-wave” resonant response, which will create the types of electromagnetic pulses and
fields referred to as “standing waves”.
The speed at which a voltage impulse is transmitted through a metal wire is extremely fast. It is essentially the
same as the speed of light, which travels 300 million meters (186,000 miles) in a single second (that distance
would circle the earth more than 7 times).
If wavelength (in meters) is multiplied by frequency (cycles per second), the result will be the speed of light, 300
million meters/second. Therefore, the wavelength of an “alternating current” (AC) voltage, at some particular
frequency, will be the speed of light, divided by which frequency.
Therefore, using simple division, if an alternating voltage operates at a frequency of 1 megahertz (MHz), which is
a million cycles per second, then the “wavelength” at that frequency will be 300 meters. If the frequency halves
become 500 kilohertz, the wavelength becomes twice as long (600 meters); and, if the frequency were to increase
to 2 megahertz, the wavelength drops to 150 meters.
It should be noted which the term “cycles” is what scientists call “a dimensionless unit”, which drops out and
becomes silent when other physical terms are multiplied or divided.
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