Practical Guige to Free Energy Devices

understand clearly that the current flowing through any coil connected across a high voltage source such as 110V
or 220V and using any of the following configurations, is limited by the impedance of the coil itself. ‘Impedance’ is
effectively ‘AC resistance’ at the frequency of the AC voltage supply. If the coil impedance is low, then the current
flowing through the coil will be high and since the power dissipated by the current flow is Voltage x Current, the
power dissipation with increased current goes up very quickly when the voltage level is as high as 220 volts. The
power dissipation is in the form of heat which means that with excessive power dissipation, the wire in the coil is
liable to melt or ‘burn out’ in an impressive flash of flame, smoke and blackened wire. Consequently, the coil
winding needs to have many turns and the wire diameter needs to be sufficient to carry the current flow – the wire
table on page 1 of the Appendix shows the current which can be carried by each size of wire when wound into a
coil. If there is no back-EMF effect with the following configurations, then the current in the primary winding
connected across the mains will not be affected by the other coils, so remember that when preparing the primary
coil.
The first arrangement uses three toroids to give four separate outputs. The amount of current which can be
drawn from any secondary depends on the amount of magnetic flux which can be carried by the magnetic core or
cores between the primary coil and that particular secondary coil. Obviously, the output current draw will also be
limited by the current-carrying capacity of the wire used in the secondary coil. If that level of current is exceeded
for any length of time, then the insulation of the wire will fail, turns will short-circuit together, the coil impedance
will drop, the current increase further and the coil will burn out – so, common sense is called for.
Here, the primary coil “1” is wound on a toroid which is horizontal in the picture above, and the secondary coils “2”
are wound on toroids which are shown as vertical in the drawing. The important point here is that the toroids with
the secondary coils, touch the primary coil toroid at right angles, that is, at 90-degrees. For convenience of
winding the coils, any toroid can be assembled from two half toroids which allows the coil to be wound separately
and when completed, slid on to one of the C-shaped half toroids before the two halves are placed together to form
the complete toroid.
The second arrangement three toroids:
The third arrangement uses four toroids, in a more powerful arrangement where the magnetic flux carrying
capacity of the transformer is doubled as the cross sectional area of the toroids inside each coil is doubled. This
is a more difficult arrangement to construct and if the coils are to be wound on a separate coil winder, then the
toroids each need to be made from one half-toroid plus two quarter toroids so that the coils can be slipped on to
two separate quarter-toroid sections which are curving in opposite directions, unless of course, the inside
diameter of the coils is a good deal larger than the toroid cross section (which reduces the number of turns for any
given length of coil wire):
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