09.02.2018 Views

Practical Guige to Free Energy Devices

eBook 3000 pages! author: Patrick J. Kelly "This eBook contains most of what I have learned about this subject after researching it for a number of years. I am not trying to sell you anything, nor am I trying to convince you of anything. When I started looking into this subject, there was very little useful information and any that was around was buried deep in incomprehensible patents and documents. My purpose here is to make it easier for you to locate and understand some of the relevant material now available. What you believe is up to yourself and is none of my business. Let me stress that almost all of the devices discussed in the following pages, are devices which I have not personally built and tested. It would take several lifetimes to do that and it would not be in any way a practical option. Consequently, although I believe everything said is fully accurate and correct, you should treat everything as being “hearsay” or opinion. Some time ago, it was commonly believed that the world was flat and rested on the backs of four elephants and that when earthquakes shook the ground, it was the elephants getting restless. If you want to believe that, you are fully at liberty to do so, however, you can count me out as I don’t believe that. " THE MATERIAL PRESENTED IS FOR INFORMATION PURPOSES ONLY. SHOULD YOU DECIDE TO PERFORM EXPERIMENTS OR CONSTRUCT ANY DEVICE, YOU DO SO WHOLLY ON YOUR OWN RESPONSIBILITY -- NEITHER THE COMPANY HOSTING THIS WEB SITE, NOR THE SITE DESIGNER ARE IN ANY WAY RESPONSIBLE FOR YOUR ACTIONS OR ANY RESULTING LOSS OR DAMAGE OF ANY DESCRIPTION, SHOULD ANY OCCUR AS A RESULT OF WHAT YOU DO. ​

eBook 3000 pages!
author: Patrick J. Kelly

"This eBook contains most of what I have learned about this subject after researching it for a number of years. I am not trying to sell you anything, nor am I trying to convince you of anything. When I started looking into this subject, there was very little useful information and any that was around was buried deep in incomprehensible patents and documents. My purpose here is to make it easier for you to locate and understand some of the relevant material now available. What you believe is up to yourself and is none of my business. Let me stress that almost all of the devices discussed in the following pages, are devices which I have not personally built and tested. It would take several lifetimes to do that and it would not be in any way a practical option. Consequently, although I believe everything said is fully accurate and correct, you should treat everything as being “hearsay” or opinion.

Some time ago, it was commonly believed that the world was flat and rested on the backs of four elephants and that when earthquakes shook the ground, it was the elephants getting restless. If you want to believe that, you are fully at liberty to do so, however, you can count me out as I don’t believe that. "

THE MATERIAL PRESENTED IS FOR INFORMATION PURPOSES ONLY. SHOULD YOU DECIDE TO PERFORM EXPERIMENTS OR CONSTRUCT ANY DEVICE, YOU DO SO WHOLLY ON YOUR OWN RESPONSIBILITY -- NEITHER THE COMPANY HOSTING THIS WEB SITE, NOR THE SITE DESIGNER ARE IN ANY WAY RESPONSIBLE FOR YOUR ACTIONS OR ANY RESULTING LOSS OR DAMAGE OF ANY DESCRIPTION, SHOULD ANY OCCUR AS A RESULT OF WHAT YOU DO.

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cold-cathode tube 391, and an x-ray tube indicated generally at 393. Also shown on Fig.20B is an RLC network<br />

395 which has an output on a line 397 which is at 35 V, this voltage being supplied <strong>to</strong> the x-ray tube.<br />

High frequency discharge tube 255 (see Fig.20C) has a conductive electrode 399 at one end <strong>to</strong> which high<br />

frequency current is applied <strong>to</strong> excite the gases in the mixer, and an electrode/heater arrangement 401 at the<br />

other, a voltage of 45 V being applied <strong>to</strong> an input 402 of the tube. It is desirable that a small quantity of mercury,<br />

indicated at 403, be included in tube 225 <strong>to</strong> promote discharge of the helium gas. Magnetic coils 237 have<br />

disposed therein a pair of generally parallel conduc<strong>to</strong>rs 405 <strong>to</strong> which a high frequency signal is applied. When<br />

gas flows through coils 237 and between parallel conduc<strong>to</strong>rs 405, therefore, it is subjected <strong>to</strong> the combination of a<br />

DC magnetic field from the coil and high frequency waves from the conduc<strong>to</strong>rs, which conduc<strong>to</strong>rs act as<br />

transmitting antennas. The resulting high frequency magnetic field causes the a<strong>to</strong>ms <strong>to</strong> become unstable, which<br />

allows the engine <strong>to</strong> change a given a<strong>to</strong>m's quantum level with much less input power than would normally be<br />

required. The volume of each gas a<strong>to</strong>m will also be smaller. Also shown on Fig.20C is non-directed cathode ray<br />

tube 227. The grids of tube 227 are at 145 V, the control electrode is at ground, while the anode is at 35 V <strong>to</strong> 80 V<br />

(peak-<strong>to</strong>-peak). The purpose of non-directed cathode ray tube 227 is <strong>to</strong> add pho<strong>to</strong>ns <strong>to</strong> the gas mixture. To<br />

generate these pho<strong>to</strong>ns, tube 227 has a two layer ZnS coating indicated generally at 407. Chamber 261,<br />

described above, is also shown schematically on Fig.20C, along with an RLC network 409.<br />

The power supply for the mixer (see the lower halves of Fig.20E and Fig.20F) also includes two pen<strong>to</strong>des 411<br />

and 413, a transformer 415, and a diode tube 417. The control electrode of pen<strong>to</strong>de 411 is at 5 V <strong>to</strong> 40 V (peak<strong>to</strong>-peak),<br />

the grids are at 145 V, the anode is at 100 V, and the cathode is at 8 V <strong>to</strong> 30 V (peak-<strong>to</strong>-peak). The<br />

control electrode of pen<strong>to</strong>de 413 is at 115 V, while its grids and cathode are at -33 V. The anode of tube 413 is<br />

connected <strong>to</strong> transformer 415. Also shown on Fig.20E are a relay 419 associated with ion gauge 255, and<br />

focused x-ray tube 263 associated with ionisation head 240. The upper input <strong>to</strong> tube 263 is at 45 V <strong>to</strong> 80 V (peak<strong>to</strong>-peak).<br />

Turning <strong>to</strong> Fig.20F, there is shown tubes 265 and 285. Directed cathode ray tube 265 is a pen<strong>to</strong>de connected<br />

like tube 227. High frequency discharge tube 285 includes a phosphor screen and is connected <strong>to</strong> a high<br />

frequency source. Also shown on Fig.20F is a triode 421 with its anode at 30 V, its cathode at ground, and its<br />

control grid at -60 V; a pen<strong>to</strong>de 423 with its anode at 135 V <strong>to</strong> 1000 V peak <strong>to</strong> peak, its cathode at ground, its<br />

control electrode at 143 V, its grids at 20 V; and a transformer 425. It should be unders<strong>to</strong>od that various<br />

arrangements of electrical components other than those described above could be designed <strong>to</strong> perform the same<br />

functions.<br />

The operation of the mixer is best unders<strong>to</strong>od with reference <strong>to</strong> Fig.17A <strong>to</strong> Fig.17D and is as follows: Before and<br />

during operation, the mixer, and particularly chamber 261 is kept hermetically sealed and evacuated. To begin the<br />

mixing process, helium is admitted in<strong>to</strong> the mixer via intake port 203. Then a vacuum is again drawn, by a<br />

vacuum pump (not shown) connected <strong>to</strong> valve V38, <strong>to</strong> flush the chamber. This flushing is repeated several times<br />

<strong>to</strong> completely cleanse the tubing branches of the mixer. The mixer is now ready. The ionisation heads next <strong>to</strong><br />

mixing chamber 261 are connected <strong>to</strong> a voltage corresponding <strong>to</strong> approximately 36% of the calculated <strong>to</strong>tal<br />

ionising voltage, DC current is allowed <strong>to</strong> flow through magnetic coils 297 and 299 around chamber 261, and high<br />

frequency current is allowed <strong>to</strong> pass through the mixing chamber. Helium is then slowly admitted, via port 203,<br />

in<strong>to</strong> the mixer. From port 203, the helium passes through ionisation head 219 in<strong>to</strong> glass tubing coil 259. This<br />

glass coil, being outside magnetic coils 297 and 299, is in the diverging portion of a magnetic field. The helium<br />

slowly flowing through glass coil 259 is gently excited. From coil 259, the helium flows through branch B45 <strong>to</strong><br />

ionisation head 275 and from there, via branch B28, <strong>to</strong> ionisation head 229 (see Fig.17B). From head 229, the<br />

gas flows through non-directed cathode ray tube 227 <strong>to</strong> high-frequency discharger 225. The high frequency<br />

discharger 225, with heating element, discharges, separates or completely neutralises the charge of any<br />

radioactive and/or cosmic particles that are in the helium a<strong>to</strong>m in addition <strong>to</strong> the pro<strong>to</strong>ns, neutrons and electrons.<br />

The gas exits discharger 225 via branch B26 and passes <strong>to</strong> high-frequency discharger 285. The high frequency<br />

discharger 285, without heating element, disturbs the frequency of oscillation which binds the gas a<strong>to</strong>ms <strong>to</strong>gether.<br />

This prepares the helium a<strong>to</strong>ms so that the electrons can more easily be split from the nucleus during the<br />

excitation and ignition process in the engine. Discharger 285 includes a phosphorus screen or deposit (similar <strong>to</strong><br />

the coating on a cathode ray tube) which makes discharges in the tube visible. From discharger 285, the helium<br />

passes through directed cathode ray tube 265 and focused x-ray tube 263. Directed cathode ray tube 265<br />

produces cathode rays which oscillate back and forth longitudinally underneath and along the gas carrying tube.<br />

After that, the helium passes successively through branch B21, ionisation head 221, branch B23, twin parallel<br />

magnetic coil 266, and branch B25 in<strong>to</strong> mixing chamber 261. Helium flows slowly in<strong>to</strong> and through apparatus 201.<br />

The helium a<strong>to</strong>ms become ionised as a result of excitation by magnetic force, high frequency vibrations and<br />

charge acquired from the ionisation heads. When sufficient helium has entered the apparatus, the ionisation<br />

energy (which is approximately 36% of the <strong>to</strong>tal) is <strong>to</strong>tally absorbed. A spectroscopic flash of light in the mixing<br />

A - 1183

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