A Practical Guide to 'Free-Energy' Devices

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chamber signals that the precise, proper quantity of helium has been allowed to enter. The entry of helium is then immediately halted by the closing of valve V3. The next step in preparing the fuel is to add neon to the mixture. The potential on the relevant ionisation heads, particularly head 241 (see Fig.17C), is raised by the addition of approximately 26% which results in a total of approximately 62% of the total calculated potential and valve V31 is opened, thereby allowing neon to slowly enter the mixer via port 245. This gas passes through branch B36, ionisation head 241, and branch B35 directly into the mixing chamber. Since the previously admitted helium is fully charged, the neon absorbs all of the increased ionisation potential. As soon as the neon acquires the additional charge, a spectroscopic flash of light occurs and the operator closes valve V31. In the same manner, the potential on the ionisation heads is increased by the addition of approximately 17% for a total of approximately 79% of the total calculated potential and then valve V30 is opened to admit argon into the mixer via port 243. This gas passes through branch B34, ionisation head 239, and branch B33 into mixing chamber 261. Again, when the proper amount of argon has been admitted, it emits a spectroscopic flash of light and the operator closes valve V30. Next, the potential on the ionisation heads is increased by the addition of approximately 13% to result in a total of approximately 92% of the total calculated potential and valve V58 (see Fig.17D) is opened to admit krypton into the system. The krypton gas passes through branch B51, ionisation head 271 and branch B48 into chamber 261. Upon the emission of a spectroscopic flash of light by the gas, the operator closes valve V58. Finally, the potential on the ionisation heads is increased by the addition of approximately 8% which brings the ionisation potential to the full 100% of the calculated ionisation voltage and valve V56 is opened to admit xenon into the mixer via port 279. This gas passes through branch B50, ionisation head 273 and branch B47 to the mixing chamber. When the proper amount of gas has been admitted, a spectroscopic flash of light occurs signalling the operator to close valve V56. Note that there are two filter/absorber units, labelled 253 and 291. Unit 253 is connected to the neon and argon inlet branches B33 and B35 while unit 291 is connected to the krypton and xenon inlet branches B47 and B48. These two units absorb hydrogen residue and immobilise the water vapour created when the pump circulates the gases and generates vacuum states. After all the gases are admitted in the desired proportions, all the valves are closed. (The mixture in the mixing chamber and in the adjacent tubing is at one atmosphere pressure at this time). Once this is done, the interval valves of the system are all opened (but the inlet and outlet valves remain closed) to allow the mixture to circulate throughout the tubing as follows: branch B44, magnetic coils 267 and 269, ionisation head 240, branch B29, ionisation head 231, branch B24, ionisation head 219, pump 217, branches B15 and B39A, ionisation gauge 255, branches B38 and B42, ionisation head 275, branch B28, ionisation head 229, non-directed cathode ray tube 227, quadruple magnetic coil 272, ionisation head 221, branch B23, twin parallel magnetic coil 266, branch B25 and mixing chamber 261. When this circuit is initially opened, the pressure of the mixture drops 40-50% because some of the tubing had previously been under vacuum. Pump 217 is then started to cause the gases to be slowly and evenly mixed. Because of dead space in the tubing and the reaction time of the operator, it may occur that the proportions of the gases are not exactly those set forth above. This is remedied during the circulation step. As the gas flows through ionisation gauge 255, excess gas is removed from the mixture so that the correct proportions are obtained. To do this the grid of gauge 255 is subjected to 100% ionisation energy and is heated to approximately 165 degrees F. This temperature of 165 degrees F is related to xenon's boiling point of -165 degrees F in magnitude but is opposite in sign. Xenon is the heaviest of the five inert gases in the mixture. As the gas mixture flows through ionisation gauge 255, the gas atoms that are in excess of their prescribed percentages are burned out of the mixture and their charge is acquired by the remaining gas atoms from the grid of the ionisation gauge. Because the gases are under a partial vacuum, the ionisation gauge is able to adjust the gas percentages very precisely. (Note: The steps described in the last two paragraphs are repeated if the finished gases are rejected in the final quality control step described below). The next step involves purifying the mixture so that only the five inert gases remain, absorbing any free electrons and regulating the electrical charge in the mixture. To do this, the circuit consisting of the following components is opened: Branch B44, magnetic coil 267, magnetic coil 269, ionisation head 240, branch B29, ionisation head 231, branch B24, ionisation head 219, pump 217, branches B15 and B39, magnetic coil 287 (see Fig.17D) polariser 289, branch B17, ionising and filtering unit 215, branches B16, B42, and B41, x-ray tube 263, branch B21, ionisation head 221, branch B23, magnetic coil 266, branch B25, and mixing chamber 261. The gases should complete this circuit at least three times. The last step required to prepare the mixture for bottling is polarisation of the argon. The circuit required to do this consists of the following components: mixing chamber 261, branch B44, magnetic coil 267, magnetic coil 269, ionisation head 240, cathode ray tube 265, branch B40, tubing coil 257, branches B49 and B30, ionisation head 231, branch B24, ionisation head 219, pump 217, branches B15 and B39, twin parallel magnetic coil 287 (see A - 1184
Fig.17D), polariser 289, branch B17, ionising and filtering unit 215, branches B16, B42 and B20, ionisation head 229, cathode ray tube 227, magnetic coil 237, ionisation head 221, branch B23 and magnetic coil 266. This too is repeated at least three times. The key to the polarisation of argon is polariser 289 and twin parallel magnetic coil 287 that encircles it. Polariser 289 is a glass bottle which is filled with finely powdered soft iron which can be easily magnetised. The filled bottle is, in effect, the iron core of the coils. The iron particles align themselves with the magnetic lines of force, which lines radiate from the centre toward the north and south poles. The ionised gas mixture is forced through the magnetised iron powder by means of pump pressure and vacuum, thereby polarising the argon gas. Filters 293 and 295 are disposed as shown in order to filter metallic particles out of the gas. The mixture is now double-checked by means of spark chamber 251 at atmospheric pressure since the fusion reaction in the engine is started at one atmosphere. Because the gases in mixing apparatus 201 are at a partial vacuum, sufficient gases must be pumped into spark chamber 251 to attain atmospheric pressure. To do this valves V33, V36 and V40A are closed and circulating pump 217 pumps the gases in the mixing apparatus via branches B15 and B39A, through check valve V39A into spark chamber 251 until the vacuum and pressure gauge 242 indicates that the gases within spark chamber 251 are at atmospheric pressure. Valve V34 is then closed. The spark chamber is similar to a cloud chamber. Six or more high capacity brass capacitor plates are spaced 1/8" to 1/4" apart in the chamber. A small plastic container holds the thorium 232. One side of the chamber is equipped with a thick glass window through which sparks in the chamber may be observed. A potential is placed on the brass plates in the chamber and the current flowing between the plates is measured. If this current exactly corresponds to the ionisation current, the mixture is acceptable. A difference of greater than 5% is not acceptable. A lesser difference can be corrected by recirculating the gas in the mixer and particularly through ionisation gauge 255 as previously described in the circulation step. A second test is then given the gases that pass the first test. A calculated high frequency current is gradually imposed on the spark chamber capacitor plates. This excitation causes neutrons to be emitted from the thorium 232 which, if the mixture is satisfactory, can be easily seen as a thin thread of light in the chamber. If the mixture is not satisfactory, light discharges cannot be seen and the high frequency circuit will short out and turn off before the desired frequency is reached. To bottle the mixture, valve V33 is opened and valves V36 and V40 are closed. During bottling polariser 289, twin parallel magnetic coil 287, ionisation unit 215 and ion gauge 255 are electrically energised (all electrical circuits are previously de-energised) to improve the stability of the mixture. The prepared gases are withdrawn from the mixing apparatus via branches B24 and B16, ionisation unit 215, branch B17, filters 293 and 295, polariser 289, twin parallel magnetic coil 287, branch B39, ion gauge 255, check valve V39A, branch B38 and spark chamber 251. If desired, after bottling the mixer may be exhausted by opening valves V12, V13, V14, V23, V24, V29, V32, V57 and V59. Of course, one can also automate the fuel preparation process to be continuous so that it would never be necessary to exhaust the gas. In operation of mixing apparatus 201, certain operational factors must be considered. For one, no electrical devices can be on without the pump being in operation because an electrical device that is on can damage adjacent gas that is not circulating. For another, it should be noted that directed cathode ray tube 265, nondirected cathode ray tube 227 and focused x-ray tube 263 serve different functions at different points in the mixing process. In one mode, they provide hot cathode radiation, which can occur only in a vacuum. When gases are flowing through these devices, they provide a cold cathode discharge. For example, during argon polarisation and the circulation step, focused x-ray tube 263 is under vacuum and affects the gases flowing through ionisation head 240 by way of hot cathode radiation. During the introduction of the different gases into mixing apparatus 201 and during the recirculation step, the gases are flowing through focused x-ray tube 263, which affects the gases by way of a cold cathode discharge. It is preferred that each switchable electrical component in mixing apparatus 201 be wired into a separate circuit despite the fact that one of the poles of each could be commonly wired. In a common ground circuit if one device is turned on, all of the other units may also turn on because the gases in the device are conductive. In addition, if one unit on a common circuit were energised with high frequency current, the others would also be affected. In the same vein, the high frequency current cannot be used when the cathode ray tubes, the x-ray tubes or the dischargers are heated and under vacuum because the heater filaments will burn out. Finally, the current source, the variable rectifiers and the electrical measuring instruments must be located more than ten feet from mixing apparatus 201 because the high frequency current is harmful to the rectifiers, causing them to burn out or short out. It is hoped that a brief summary of the concepts used by the inventor in developing the above invention will be helpful to the reader, it being understood that this summary is in no way intended to limit the claims which follow or to affect their validity. The first concept is that of using an inert gas mixture at approximately one atmosphere at TDC (at ignition) as a fuel in a thermonuclear energy production process. The second concept is the layering of A - 1185
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JUAN AGUERO Patent Application EP04
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the exhaust manifold. This heats so
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combustion chambers. The hydrogen i
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21. The system of claim 20, charact
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electrolysis of water at such a rat
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Fig.4 is an elevation view of the h
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Fig.10 is a cross-section on the li
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Fig.16 is a cross-section on the li
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Fig.23 is an enlargement of part of
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Fig.33 is a perspective view of a v
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A - 843
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through a resistor R4 to provide tr
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The installation of the above circu
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cathode in the upper region of the
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transformer and, assuming an input
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valve apparatus to control engine s
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. a first hollow cylindrical electr
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CHRISTOPHER ECCLES UK Patent App. 2
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Fig.1 is a circuit diagram of fract
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If a large electric field is applie
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The pulses R1 and S1 are of the sam
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DISCLOSURE OF THE INVENTION The inv
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A - 867
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Fig.5B shows a stylised representat
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Fig.6 shows a gas collection system
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Fig.8A and Fig.8B are views of a se
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A - 875
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Figs.16-30 are graphs supporting th
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A - 879
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A - 881
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A - 883
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A - 885
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A - 887
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If it is the case that the hydrogen
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plate shown in Fig.1A and Fig.1B an
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is in equilibrium where the 10 watt
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The previously mentioned prior art
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The stores of high pressure gases c
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unit to retain operational gas pres
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HENRY PAINE This is a very interest
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Henry Paine’s apparatus would the
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some form of distortion of space. I
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superconductive disk is made part o
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Fig.2A and Fig.2B are diagrams, pre
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Fig.4A and Fig.4B are diagrams, pre
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#1 hollow superconductive shield #2
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Fig.2B shows the counter-clockwise
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In this example, the difference bet
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CHARLES POGUE US Patent 642,434 12t
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Fig.3 is a horizontal sectional vie
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Fig.9 and Fig.10 are detail section
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having a valve 52 in it. Chamber 50
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CHARLES POGUE US Patent 1,997,497 9
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Fig.4 is a detail sectional view of
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A low-speed or idling jet 25 has it
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DESCRIPTION OF THE DRAWINGS Fig.1 i
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Fig.5 is a detail sectional view on
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Vapour formed by air bubbling throu
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From the foregoing description it w
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Fig.2 is an enlarged view of the de
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Fig.6 is a section taken along line
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ROBERT SHELTON US Patent 2,982,528
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Fig.4 is a transverse sectional vie
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HAROLD SCHWARTZ US Patent 3,294,381
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182,420 now abandoned. The present
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DESCRIPTION OF THE INVENTION The ca
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THOMAS OGLE US Patent 4,177,779 11t
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In accordance with other aspects of
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Fig.3 is a sectional view of the va
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Fig.7 is a partial side, partial se
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The cooling system of the vehicle c
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Upon initial starting of the engine
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(f) A filter positioned in the vapo
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with the magnitude of the current a
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Fig.1B is a perspective view of the
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Fig.3 is a top view of the motor of
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Fig.7 is an isometric view showing
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Fig.10 is a top view showing the ro
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Fig.13 is a top view of a pair of r
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Extending in opposite diametric dir
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Fig.5 shows the state of the switch
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otor magnets 42 - 49 when in the ho
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Fig.9 and Fig.10 show a second arra
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constructed otherwise than as speci
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12. The motor of claim 11 wherein t
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timer or a control mechanism mounte
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Fig.4 is a view similar to Fig.3 bu
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Fig.10 is a view similar to Fig.3 f
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Fig.13 is a schematic circuit diagr
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Fig.16 is a simplified embodiment o
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Fig.22 to Fig.25 are similar to Fig
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Referring to Fig.2, the permanent m
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Fig.7 shows a modified embodiment w
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them, will depend upon the order in
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Fig.14, shows another embodiment 14
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Fig.18 shows the air coil 210 posit
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Figs. 22-25 show four different pos
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movement with the first permanent m
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a shaft and means journaling the sh
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CLAUDE MEAD and WILLIAM HOLMES US P
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Fig.2 is a front elevation of the w
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impactors and drills. The turbine d
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(a) fourth rotating means responsiv
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path to the other side of the perma
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Fig.3 is an oscilloscope waveform t
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DETAILED DESCRIPTION OF THE PREFERR
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although it is by no means obvious
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second diode connected at its posit
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In the present invention, a permane
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Fig.4 is a circuit diagram, illustr
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and Fig.3. In practice, this coil m
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y a simultaneous magnetic accelerat
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Mr. P.G. Mallory started out in 191
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All models have a 30 Watt power rat
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In the auto racing circles it has a
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BATTERY + _ SIMPLIFIED MULTIVIBRATO
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Schematic Wiring Diagrams for two P
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motor. What is not generally known,
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Mark McKay's investigation of Edwin
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Investor Photo #012D Popping a coil
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capacitors connected in series, wit
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PULSE WIDTH TIME IN mS went to the
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TOP DEAD CENTER 0° REFERENCE Accor
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The recovery and simple analysis of
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FILTER CAPACITOR + 2 OHM 200 WATT R
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Subject: CSET design Date: Sun Feb
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Date: Fri Feb 28, 2003 8:25 pm (Tim
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(Tad Johnson) I'm being as careful
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SANGAMO ENERGY DISCHARGE CAPACITOR
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(Alan Francoeur) But I also measure
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Subject: Progress Date: Sun Mar 30,
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● all electrical connections were
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Mark Gray claims that the heart and
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Mark Gray claims that some potentia
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Radio Frequency (RF) Generator Gene
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Some time during 1987 - 1988, Gray
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The two-channel trace from the osci
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What “maximum squareness” means
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Zo = 112 Ohms Td of 293 nS. 50 KV 8
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MIKE BRADY’S “PERENDEV” MAGNE
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Fig.3 is a perspective view showing
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Fig.7 is a perspective view showing
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In the rotor assembly 30 of Fig.2,
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Fig.7 shows a typical magnetic sour
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DONALD A. KELLY ABSTRACT Patent US
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This series of magnetic oscillating
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Because there is no natural, lock-i
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Fig.3 is an enlarged top view of on
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An arm 9, is fastened to a flat fac
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Fig.2 is a vertical transverse cros
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Fig.6 is a vertical, longitudinal,
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Working inside the cylinders 12 are
Page 311 and 312: Leroy K. Rogers Patent US 4,292,804
Page 313 and 314: Preferred embodiments of a method a
Page 315 and 316: Fig.6 is a cross-sectional view of
Page 319 and 320: tapped hole in the cylinder 20 typi
Page 321 and 322: A second embodiment of a valve actu
Page 323 and 324: otates faster, the other end 98 of
Page 325 and 326: In normal operation (as seen in Fig
Page 327 and 328: Eber Van Valkinburg Patent US 3,744
Page 329 and 330: Referring to the drawings in detail
Page 331 and 332: Since the pump depends for its supp
Page 333 and 334: Briefly, in one aspect the engine o
Page 337 and 338: Fig.12 is a cross-sectional view si
Page 339 and 340: Fig.14 is a schematic diagram of an
Page 341 and 342: A - 1163
Page 343 and 344: A - 1165
Page 345 and 346: Figs.20A-20F are schematic diagrams
Page 347 and 348: Note: Corresponding reference chara
Page 349 and 350: Integral with the piston bodies are
Page 351 and 352: The piston has a generally semi-tor
Page 353 and 354: Referring back to Fig.13A, for engi
Page 355 and 356: As piston 39A reaches BDC, distribu
Page 357 and 358: mixture and do not combine because
Page 359 and 360: These wires are about twelve gauge,
Page 361: cold-cathode tube 391, and an x-ray
Page 365 and 366: Robert Britt US Patent 3,977,191 31
Page 367 and 368: Fig.3 is an elevational view of the
Page 369 and 370: Fig.7 is an electrical schematic of
Page 371 and 372: Referring now to Fig.3 of the drawi
Page 373 and 374: and drives Q1 into conduction. The
Page 375 and 376: Floyd Sweet Recently, some addition
Page 377 and 378: The day when we witnessed the VTA d
Page 379 and 380: up to see Floyd. Floyd was with the
Page 381 and 382: Energy cannot enter a space of zero
Page 383 and 384: electromagnetic and gravitational f
Page 385 and 386: or in another form: So, the e.m.f.
Page 387 and 388: Example 2: Suppose the conductor wi
Page 389 and 390: Meguer Kalfaian There is a patent a
Page 391 and 392: Fig.2 illustrates a controlled top
Page 393 and 394: Fig.9 is a modification of Fig.6; a
Page 395 and 396: the outer periphery of the magnet,
Page 397 and 398: wobbling top is sufficient, as proo
Page 399 and 400: Theodore Annis & Patrick Eberly US
Page 401 and 402: BRIEF DESCRIPTION OF THE DRAWINGS F
Page 403 and 404: Fig.6 is a schematic diagram of a s
Page 405 and 406: DETAILED DESCRIPTION OF THE PREFERR
Page 407 and 408: Fig.5 is a detail drawing of an alt
Page 409 and 410: In the preferred implementation of
Page 411 and 412: William McDavid junior US Patent 6,
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This sloping floor causes the drive
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FIG.3 is a side elevational view of
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FIG.9 is a horizontal cross-section
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otational downstream annular chambe
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In Fig.5 is shown a perspective vie
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small hydro-electric version of the
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Fig.10 is a perspective view of a s
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longitudinally mounted in the upstr
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shaft in the central aperture, said
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Scientific Papers The following lin
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