A Practical Guide to 'Free-Energy' Devices

cold-cathode tube 391, and an x-ray tube indicated generally at 393. Also shown on Fig.20B is an RLC network
395 which has an output on a line 397 which is at 35 V, this voltage being supplied to the x-ray tube.
High frequency discharge tube 255 (see Fig.20C) has a conductive electrode 399 at one end to which high
frequency current is applied to excite the gases in the mixer, and an electrode/heater arrangement 401 at the
other, a voltage of 45 V being applied to an input 402 of the tube. It is desirable that a small quantity of mercury,
indicated at 403, be included in tube 225 to promote discharge of the helium gas. Magnetic coils 237 have
disposed therein a pair of generally parallel conductors 405 to which a high frequency signal is applied. When
gas flows through coils 237 and between parallel conductors 405, therefore, it is subjected to the combination of a
DC magnetic field from the coil and high frequency waves from the conductors, which conductors act as
transmitting antennas. The resulting high frequency magnetic field causes the atoms to become unstable, which
allows the engine to change a given atom's quantum level with much less input power than would normally be
required. The volume of each gas atom will also be smaller. Also shown on Fig.20C is non-directed cathode ray
tube 227. The grids of tube 227 are at 145 V, the control electrode is at ground, while the anode is at 35 V to 80 V
(peak-to-peak). The purpose of non-directed cathode ray tube 227 is to add photons to the gas mixture. To
generate these photons, tube 227 has a two layer ZnS coating indicated generally at 407. Chamber 261,
described above, is also shown schematically on Fig.20C, along with an RLC network 409.
The power supply for the mixer (see the lower halves of Fig.20E and Fig.20F) also includes two pentodes 411
and 413, a transformer 415, and a diode tube 417. The control electrode of pentode 411 is at 5 V to 40 V (peakto-peak),
the grids are at 145 V, the anode is at 100 V, and the cathode is at 8 V to 30 V (peak-to-peak). The
control electrode of pentode 413 is at 115 V, while its grids and cathode are at -33 V. The anode of tube 413 is
connected to transformer 415. Also shown on Fig.20E are a relay 419 associated with ion gauge 255, and
focused x-ray tube 263 associated with ionisation head 240. The upper input to tube 263 is at 45 V to 80 V (peakto-peak).
Turning to Fig.20F, there is shown tubes 265 and 285. Directed cathode ray tube 265 is a pentode connected
like tube 227. High frequency discharge tube 285 includes a phosphor screen and is connected to a high
frequency source. Also shown on Fig.20F is a triode 421 with its anode at 30 V, its cathode at ground, and its
control grid at -60 V; a pentode 423 with its anode at 135 V to 1000 V peak to peak, its cathode at ground, its
control electrode at 143 V, its grids at 20 V; and a transformer 425. It should be understood that various
arrangements of electrical components other than those described above could be designed to perform the same
functions.
The operation of the mixer is best understood with reference to Fig.17A to Fig.17D and is as follows: Before and
during operation, the mixer, and particularly chamber 261 is kept hermetically sealed and evacuated. To begin the
mixing process, helium is admitted into the mixer via intake port 203. Then a vacuum is again drawn, by a
vacuum pump (not shown) connected to valve V38, to flush the chamber. This flushing is repeated several times
to completely cleanse the tubing branches of the mixer. The mixer is now ready. The ionisation heads next to
mixing chamber 261 are connected to a voltage corresponding to approximately 36% of the calculated total
ionising voltage, DC current is allowed to flow through magnetic coils 297 and 299 around chamber 261, and high
frequency current is allowed to pass through the mixing chamber. Helium is then slowly admitted, via port 203,
into the mixer. From port 203, the helium passes through ionisation head 219 into glass tubing coil 259. This
glass coil, being outside magnetic coils 297 and 299, is in the diverging portion of a magnetic field. The helium
slowly flowing through glass coil 259 is gently excited. From coil 259, the helium flows through branch B45 to
ionisation head 275 and from there, via branch B28, to ionisation head 229 (see Fig.17B). From head 229, the
gas flows through non-directed cathode ray tube 227 to high-frequency discharger 225. The high frequency
discharger 225, with heating element, discharges, separates or completely neutralises the charge of any
radioactive and/or cosmic particles that are in the helium atom in addition to the protons, neutrons and electrons.
The gas exits discharger 225 via branch B26 and passes to high-frequency discharger 285. The high frequency
discharger 285, without heating element, disturbs the frequency of oscillation which binds the gas atoms together.
This prepares the helium atoms so that the electrons can more easily be split from the nucleus during the
excitation and ignition process in the engine. Discharger 285 includes a phosphorus screen or deposit (similar to
the coating on a cathode ray tube) which makes discharges in the tube visible. From discharger 285, the helium
passes through directed cathode ray tube 265 and focused x-ray tube 263. Directed cathode ray tube 265
produces cathode rays which oscillate back and forth longitudinally underneath and along the gas carrying tube.
After that, the helium passes successively through branch B21, ionisation head 221, branch B23, twin parallel
magnetic coil 266, and branch B25 into mixing chamber 261. Helium flows slowly into and through apparatus 201.
The helium atoms become ionised as a result of excitation by magnetic force, high frequency vibrations and
charge acquired from the ionisation heads. When sufficient helium has entered the apparatus, the ionisation
energy (which is approximately 36% of the total) is totally absorbed. A spectroscopic flash of light in the mixing
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