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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The output of the 555 chip is then used <strong>to</strong> drive the remainder of the circuit which operates at 27V. A BC109C<br />

transis<strong>to</strong>r costs only a few pence, can handle the voltage and has a minimum gain of 200 although the gain can<br />

be anything up <strong>to</strong> 800 and a BC109 can handle the current quite easily. If you need <strong>to</strong> find out any of these<br />

things, then download a datasheet for the transis<strong>to</strong>r from the internet.<br />

The output of the 555 timer is on pin 3 and it can easily supply 200 mA which is far, far more current than we<br />

would ever need for this circuit. We can feed the 555 square-wave output <strong>to</strong> the 27V electrodes using a<br />

transis<strong>to</strong>r:<br />

As the transis<strong>to</strong>r is made of silicon, the switch-on voltage is when the base voltage is about 0.7 volts above the<br />

emitter voltage. That means that when the transis<strong>to</strong>r is switched on, the <strong>to</strong>p of resis<strong>to</strong>r “R1” will be at around 10<br />

volts and the bot<strong>to</strong>m of “R1” will be at about 0.7 volts, which means that the voltage across “R1” will be (10 – 0.7)<br />

= 9.3 Volts. When that voltage is present across “R1” we want it <strong>to</strong> feed sufficient current <strong>to</strong> the transis<strong>to</strong>r <strong>to</strong><br />

switch it on fully. The transis<strong>to</strong>r supplies a 100K resis<strong>to</strong>r (which will carry 0.27 mA when 27 volts is across it) and<br />

the electrodes which will have a minimum resistance of 820 ohms across them (causing a current of 33 mA<br />

through them). So, the transis<strong>to</strong>r might have <strong>to</strong> supply about 33 mA maximum. The BC109C transis<strong>to</strong>r has a<br />

minimum gain of 200 so the current flowing in<strong>to</strong> the base needs <strong>to</strong> be 33 / 200 = 0.165 mA and the resis<strong>to</strong>r which<br />

will carry that current when it has 9.3 volts across it is 56.3K. A somewhat smaller resis<strong>to</strong>r will suit.<br />

A commonsense check that the resis<strong>to</strong>r calculation is correct is:<br />

A 1K resis<strong>to</strong>r carries 1 mA per volt and so will carry 9.3 mA with 9.3 volts across it.<br />

A 10K resis<strong>to</strong>r will carry one tenth of that amount, or 0.93 mA with 9.3 volts across it.<br />

A 100K resis<strong>to</strong>r will carry one tenth of that again, or 0.093 mA with 9.3 volts across it.<br />

This indicates that for a current of 0.165 mA which is about twice the 100K current, a resis<strong>to</strong>r of about half of 100K<br />

should be about the right value, so 56.3K looks correct.<br />

Considering that the gain of 200 is the minimum and three or four times that is typical, we could perhaps choose<br />

<strong>to</strong> use a 47K resis<strong>to</strong>r for “R1”<br />

As the electrode current is likely <strong>to</strong> be considerably less than 33 mA and as the BC109C gain is likely <strong>to</strong> be very<br />

high, it could be quite difficult <strong>to</strong> get the transis<strong>to</strong>r <strong>to</strong> switch off as it can operate on very tiny amounts of input<br />

current. To get it <strong>to</strong> switch on and off cleanly when the 555 output voltage is say, about 5 volts, (at which point the<br />

NE555 voltage will be changing very rapidly), “R2” is included. With it in place, the output voltage of the NE555 is<br />

divided between “R1” and “R2” in the ratio of their resistances. The situation we want is:<br />

When The transis<strong>to</strong>r is not switched on, it draws almost no current and so looks like a very high value resis<strong>to</strong>r <strong>to</strong><br />

the circuit. This allows the “R1” and “R2” resis<strong>to</strong>rs <strong>to</strong> act as a voltage-divider pair. This causes the voltage at<br />

point “A” <strong>to</strong> be determined by the ratio of “R1” <strong>to</strong> “R2” and the transis<strong>to</strong>r can be ignored provided that the voltage<br />

at point “A” is below 0.7 volts. If the voltage at that point rises <strong>to</strong> 0.7 volts then the situation changes dramatically<br />

and Ohm’s Law no longer holds as the transis<strong>to</strong>r is not a passive resis<strong>to</strong>r but instead, is an active semi-conduc<strong>to</strong>r<br />

device. If the voltage at point “A” tries <strong>to</strong> rise further it can’t because the transis<strong>to</strong>r base clamps it solidly there by<br />

appearing <strong>to</strong> be an ever lower resis<strong>to</strong>r between the base and the emitter of the transis<strong>to</strong>r. So for higher input<br />

voltages, resis<strong>to</strong>r “R2” might as well not be there for all the difference it makes.<br />

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