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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force on the ro<strong>to</strong>r is 0 so that if the permanent magnets of the ro<strong>to</strong>r were aligned in any of these orientations there<br />

would be no resultant force <strong>to</strong> urge the ro<strong>to</strong>r either clockwise or anti clockwise.<br />

As shown in Fig.5 a plot of magnitude of resultant force applied <strong>to</strong> the ro<strong>to</strong>r against angular displacement of the<br />

ro<strong>to</strong>r shows a sinusoidal curve having a cycle of 30°. For a full 360° rotation of the ro<strong>to</strong>r the ro<strong>to</strong>r would<br />

experience 12 cycles of variation in resultant force.<br />

What Table 1 and Fig.5 show is that unless an additional force is applied <strong>to</strong> rotate the ro<strong>to</strong>r clockwise or counterclockwise,<br />

the ro<strong>to</strong>r will not be able <strong>to</strong> spin continuously in either direction. If it is desired <strong>to</strong> rotate the ro<strong>to</strong>r<br />

clockwise, then the force must overcome the counter-clockwise resultant force which occurs from 0 <strong>to</strong> 15°, 30° <strong>to</strong><br />

45°, 60° <strong>to</strong> 75° etc through the whole 360° rotation of the ro<strong>to</strong>r.<br />

Because each of the coils A <strong>to</strong> C has an iron core even when the coils are not energised the natural magnetic<br />

attraction occurring between each magnet and the iron cores results in each magnet M1 <strong>to</strong> M4 attempting <strong>to</strong><br />

move in a direction <strong>to</strong> the closest iron core. Whenever a magnet is opposite an iron core the magnetic attraction<br />

is greatest and there is no force applied by that magnet <strong>to</strong> move the ro<strong>to</strong>r either clockwise or counter-clockwise.<br />

Likewise when a magnet is positioned midway between adjacent iron cores, there is also a resultant force of 0<br />

which translates <strong>to</strong> no resultant force being applied <strong>to</strong> the ro<strong>to</strong>r <strong>to</strong> rotate it in either direction by that magnet.<br />

As shown in Fig.5 and Table 1, if magnet M1 is moved 5° clockwise, there is a natural attraction between the<br />

magnet M1 and iron core of coil A <strong>to</strong> pull the magnet M1 in a counter-clockwise direction. If the resultant forces<br />

applied by the other magnets were sufficient <strong>to</strong> overcome the attraction between permanent magnet M1 and the<br />

iron core of coil A the ro<strong>to</strong>r would still manage <strong>to</strong> move clockwise. However, as shown in Table 1 the angular<br />

position of the other magnets M2 <strong>to</strong> M4 results in an overall counter-clockwise resultant force. To overcome the<br />

resultant force, it is necessary <strong>to</strong> produce a pole X at coil A of like polarity <strong>to</strong> magnet M1 and thus push M1 away<br />

from coil A.<br />

As shown in Fig.5 the strength of the magnetic repelling action between coil A and magnet M1 must be sufficient<br />

<strong>to</strong> overcome the resultant force urging the ro<strong>to</strong>r <strong>to</strong> move counter-clockwise.<br />

A current could be applied <strong>to</strong> the coil A for an angular displacement of 15° of magnet M1, but it is preferred that<br />

coil A be energised only for 12° 51′ 50″ angular displacement of magnet M1. By applying current <strong>to</strong> coil A for this<br />

period of angular displacement a minimum amount of current is applied <strong>to</strong> coil A in order <strong>to</strong> overcome the counterclockwise<br />

resultant force which occurs for 0° <strong>to</strong> 15° of angular displacement of magnet M1.<br />

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