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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no motional e.m.f. Thus, dφ/dt in equation (11) is zero, even though the flux is changing with time. Note<br />

that dφ/dt was defined as representing the right hand part of the expression in equation (10) and dφ/dt<br />

must not be interpreted more broadly than that.<br />

In the application of the present equations, it is required that all flux densities and movements are<br />

referred <strong>to</strong> a single, specified co-ordinate system. In particular, the velocities will all be with respect <strong>to</strong><br />

this system alone and not interpreted as relative velocities between conduc<strong>to</strong>rs or moving lines of flux.<br />

The co-ordinate system is selected arbitrarily and the magnitudes of variational and motional fields<br />

depend upon the selection.<br />

Example 1:<br />

A fundamental electric genera<strong>to</strong>r is shown in Figure 2:<br />

The parallel, stationary conduc<strong>to</strong>rs, separated by distance "l", have a stationary voltmeter connected<br />

across them. The circuit is completed by a moving conduc<strong>to</strong>r connected <strong>to</strong> the parallel conduc<strong>to</strong>rs by<br />

means of two sliding contacts. This conduc<strong>to</strong>r is connected at y = 0 at time t = 0, and it moves <strong>to</strong> the right<br />

at a constant velocity V = Vay. The applied flux B is represented by dots on Fig.2 and has a magnitude of<br />

B = B O CosBy Coswt ax. The unit vec<strong>to</strong>rs in the direction of the co-ordinate axes are ax, ay and az<br />

respectively.<br />

Solution: Let S denote the plane rectangular surface bounded by the closed electric circuit, with a<br />

positive side selected as the side facing you. The counter-clockwise e.m.f. around the circuit is dφ/dt<br />

with φ signifying the magnetic flux out of the positive side of S (As ds = 1 dy ax). The scalar product B x<br />

ds is B O l CosBy, Coswt dy; integrating from y = 0 <strong>to</strong> y = y gives:<br />

With y 1 denoting the instantaneous y position of the moving wire. The counter-clockwise e.m.f. is found<br />

by replacing y with vt and evaluating dφ/dt. The result is:<br />

The variational (transformer) component is determined with the aid of equation (12) and is wB O l/BsinBy<br />

sinwt where y = vt. This is the first component on the right hand side of equation (13).<br />

Note: y 1 was treated as a constant when evaluating the partial time derivative of φ.<br />

The motional E-field is the line integral of V x B along the path of the moving conduc<strong>to</strong>r. As V x B is -B O<br />

vcosBy 1 coswt ax and As dl is dz ax, evaluation of the integral -B O vcosBy 1 coswt dz from Z = 0 <strong>to</strong> Z = 1<br />

results in a motional E-field of -B O lvcosBv 1 coswt. This component results from modulation of the lines<br />

of flux by the moving conduc<strong>to</strong>r. If the voltmeter draws no current, there can be no electromagnetic force<br />

on the free electrons of the wire. Therefore, the e.m.f. along the path of the metal conduc<strong>to</strong>rs including<br />

the moving conduc<strong>to</strong>r, is zero.<br />

A - 1208

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