Practical Guige to Free Energy Devices

4. Anyway, following through on just one L1 coil, there is likely to be at least one further step-down transformer
needed and eventually, we need conversion to hot electricity:
Probably the easiest conversion is by feeding the energy into a capacitor and making it standard DC. The
frequency is still very high, so high-speed diodes (such as the 75-nanosecond UF54008) are needed here
although the voltage level is now low enough to be no problem. The DC output can be used to power an inverter
so that standard mains equipment can be used. It is not necessary to use just one (expensive) large-capacity
inverter to power all possible loads as it is cheaper to have several smaller inverters, each powering it’s own set of
equipment. Most equipment will run satisfactorily on square-wave inverters and that includes a mains unit for
powering the input oscillator circuit.
PVC pipe is not a great material when using high-frequency high-voltage signals, and grey PVC pipe is a
particularly poor coil former material. The much more expensive acrylic pipe is excellent, but if using PVC, then
performance will be better if the PVC pipe is coated with an insulating lacquer (or table tennis balls dissolved in
acetone as show on YouTube).
However, there are some other factors which have not been mentioned. For example, if the L1 coil is wound
directly on top of the L2 coil, it will have roughly the same diameter and so, the wire being four times longer, will
have roughly four times as many turns, giving a step-up or step-down ratio of around 4:1. If, on the other hand,
the coil diameters were different, the ratio would be different as the wire lengths are fixed relative to each other. If
the L2 coil were half the diameter of the L1 coil, then the turns ratio would be about 8:1 and at one third diameter,
12:1 and at a quarter diameter 16:1 which means that a much greater effect could be had from the same wire
length by reducing the L2 coil diameter. However, the magnetic effect produced by a coil is linked to the crosssectional
area of the coil and so a small diameter is not necessarily at great advantage. Also, the length of the L1
coil wire and number of turns in it, affect the DC resistance, and more importantly, the AC impedance which
affects the amount of power needed to pulse the coil.
It is also thought that having the same weight of copper in each winding gives an improved performance, but what
is not often mentioned is the opinion that the greater the weight of copper, the greater the effect. You will recall
that Joseph Newman (chapter 11) uses large amounts of copper wire to produce remarkable effects. So, while 9
inches and 36 inches of wire will work for L1 and L2, there may well be improved performance from longer lengths
of wire and/or thicker wires.
We should also not forget that Don Smith pointed out that voltage and current act (out of phase and) in opposite
directions along the L2 coil, moving away from the L1 coil:
It has been suggested that a greater and more effective power output can be obtained by splitting the L2 coil
underneath the L1 coil position, winding the second part of L2 in the opposite direction and grounding the junction
of the two L2 windings. Don doesn’t consider it necessary to reverse the direction of winding. The result is an L2
winding which is twice as long as before and arranged like this:
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