Speaker A
Little tour for a demonstration on just how straightforward and just how nice the vacuum triode is working.
Demonstration of a vacuum triode device claimed to output 500 W of usable power from a sub-milliwatt grid signal, lighting lamps and running a fan. Claims are not scientifically validated.
Key Takeaways
- The video presents a claimed device producing 500 W output from under a third of a milliwatt input, a claim inconsistent with conservation of energy.
- The demonstrations rely on the inventor's own meter readings and narration without independent verification or peer review.
- Terms such as 'negative energy' and 'cold arc' are not established physics concepts and are used without rigorous definition.
- The video is a historical 1980s demonstration of an alternative energy invention and should be evaluated skeptically.
What the video covers
- Presenter demonstrates a vacuum triode powering five 100 W household lamps (500 W) and a 120 V AC fan at 60 Hz.
- Input grid signal is described as about 10 V with roughly 31 microamps, which the presenter calculates as under one-third of a milliwatt.
- Output plate voltage is reported around 112.5 V, with stated 500 W measured with a wattmeter at unity power factor.
- A second demonstration uses the device to drive a 24 V DC motor via rectification and lamps in series, claiming the output can be transformed and rectified like normal power.
- The presenter claims the energy is 'negative' and that circuits and wires stay cool while only the lamp filaments heat, a claim not supported by standard electrical theory.
- The video describes switching loads suddenly without arcing, attributing this to a 'cold arc' effect.
- Later segments show a magnet and coil apparatus tuned to resonant frequencies around 12-13 Hz, with the presenter discussing scaling to a 15 kW home unit.
- The demonstration is dated 1987 and presented in a home setting, with the inventor's claims framed as historically significant.
- Measurements were made with analog meters and the transcript shows fluctuating readings, limiting precision of the claimed values.
- The content presents extraordinary energy-gain claims that violate conservation of energy and lack independent verification in the transcript.
Chapters
- 00:00Introduction and vacuum triode overview
- 03:20Lamp and fan demonstration at 120 V
- 06:40Input grid measurements and power calculations
- 10:00Plate voltage and wattmeter readings
- 16:00Load switching and cold arc claims
- 22:00Scaling to home power unit discussion
- 28:20Resonant magnet and coil apparatus
- 38:20Second demonstration with 24 V DC motor
Full Transcript — Download SRT & Markdown
Speaker A
usable power now we'll turn around and here as just coming into view you see five 100 watt lamps ordinary Garden variety household lamps brilliantly lit so there's 500 watts of very real power here again coming right out of the
Speaker A
So we have a 120 volt fan. As you can see, it's turning at good power. It is providing quite a breeze, and it's real, usable power.
Speaker A
Steady it's a fairly deep decent sine wave very nice and steady and it's 60 htz it's right on the button just as conventional ordinary power it's 120 volts or very close there too and it's 60 Herz right on the
Speaker A
Now we'll turn around, and here, as just coming into view, you see five 100 watt lamps, ordinary garden variety household lamps, brilliantly lit. So there's 500 watts of very real power here, again coming right out of the vacuum. You see the assembly of very large meters, and I'll show you the kind of power amplification that is being achieved by the vacuum triode.
Speaker A
and real light being radiated away from the lamps however while the energy is still in the negative form and all the circuitry and wires going to the lamp all of those stay absolutely cool because there is no heating of those
Speaker A
Now we're going to come back in. There's the 500 watt bulbs, clearly illuminated. The power is rock steady. It's a fairly deep, decent sine wave, very nice and steady, and it's 60 hertz. It's right on the button, just as conventional, ordinary power. It's 120 volts, or very close, there too, and it's 60 hertz, right on the button.
Speaker A
in a resistive load travel back over to the fan and you see that we have a normal AC type load that's a normal AC fan runs very well on this power now we'll come back over to the load and we want to go up and show you
Speaker A
It is, however, negative energy that is being produced, as opposed to the normal garden variety of positive energy. In the lamps, in the resistive load, the negative energy is converted to ordinary positive energy, and that is real heat and real light being radiated away from the lamps. However, while the energy is still in the negative form, all the circuitry and wires going to the lamp, all of those, stay absolutely cool, because there is no heating of those circuits. Only in the filaments of the lamp is heat and light produced in the normal sense.
Speaker A
actual reading of this meter okay and reading the meter it shows you that we're putting in right at 10 volts it's oscillating between 9 and 1/2 and 10 volts that one is really a 10 it's on the that's a 10
Speaker A
So in those resistive loads, we're translating normal negative energy into positive energy, and you can see that is real power: 500 watts, half of a kilowatt, in a resistive load.
Speaker A
approximately 10 volts for the input and so it's very easy to calculate the fact that there's less than one mwatt actually down around a third of a millatt or so of power actually going in to power the fan and
Speaker A
Travel back over to the fan, and you see that we have a normal AC type load. That's a normal AC fan, and it runs very well on this power.
Speaker A
looks like we won't get the glare but there we are that is a voltmeter and it shows that we're putting out about 112 1/2 volts coming out of the vacuum trial that's the plate voltage so to speak that's
Speaker A
Now we'll come back over to the load, and we want to go up and show you some instrumental measures. We want to show you how much we're actually putting into the grid signal of the triode. First, we're going to come right in on this meter here and try to give you a close shot of the actual reading of this meter. Okay, reading the meter, it shows you that we're putting in right at 10 volts. It's oscillating between 9 and a half and 10 volts. That one is really a 10. It's on the 10 volt.
Speaker A
divide that by two and so you see that we're putting out 500 watts of actual measured power okay coming on over power factor shows one as it will in the resistive load and of course single W single phase
Speaker A
Okay, we're going over now to show you the amperage that we're putting in, and hold your hats: that 31.2 is actually 31.2 microamps. We're dealing in the microamp scale, and we're putting in 31.2 microamps of current. We're putting in approximately 10 volts for the input, and so it's very easy to calculate the fact that there's less than one milliwatt, actually down around a third of a milliwatt or so, of power actually going in to power the fan and the 500 watts of lamps, brilliantly lit.
Speaker A
is the output current all of that the entire output is being taken from the energy of the vacuum output by the device and the grid signal to do that is less than 1/3 of a mwatt less than 1/3
Speaker A
Now we'll go over and show you some more meters, coming in on this set of instruments. Let's see if we can get a better focus and get the glare away from us. Looks like we won't get the glare, but there we are. That is a voltmeter, and it shows that we're putting out about 112 and a half volts coming out of the vacuum triode. That's the plate voltage, so to speak, output by the device.
Speaker A
stable it is not transient it is not noise is and it is not any other kind of spirous effect this is a real effect it's all coming from that little tiny box sitting behind the 500 wats of power behind the
Speaker A
Coming over to the next meter: this is a wattmeter, and you divide it by half, and you see it's reading one kilowatt. So on this one here, we get on the right meter, it's reading one full kilowatt, so divide that by two, and you see that we're putting out 500 watts of actual measured power.
Speaker A
m center of the very first vacuum Tri this is a most historical occasion I show them some more okay now for this second demonstration here we have our 120 volt fan again rotating finally stirring up a breeze right behind that you see a 24v DC
Speaker A
Coming on over, power factor shows one, as it will in the resistive load, and of course, single phase circuit. You can see now the amps on this meter being put out by the machine. Very clearly, let's give a read on that: we're putting out 4.6 amps of current, 4.7 to be a little more precise, 4.7 amps of current. That is the output current. All of that, the entire output, is being taken from the energy of the vacuum, output by the device, and the grid signal to do that is less than a third of a milliwatt, less than a third of a milliwatt signal on the vacuum triode grid. Yet the plate is putting out well over 500 watts of power, 500 watts of the resistive load.
Speaker A
are two uh 12vt lamps in series brightly lit uh showing you that yes indeed we have the full 24 volts we're showing that the this power can be transformed and can be rectified just exactly like normal positive power
Speaker A
At the same time, you see the fan stirring up a nice breeze. This is real, usable power. It's stable. It is not transient, it is not noise, and it is not any other kind of spurious effect. This is a real effect. It's all coming from that little tiny box sitting behind the 500 watts of power, behind the lamps. That little box is putting out all of that power, well over 500 watts, and yet it is receiving less than a third of a milliwatt of input power.
Speaker A
or stepped up it can be rectified and we can handle the power Just indeed as we do normal Power and you see again at the same time we have four of those lamps now lit and so we have another 400 wat resistive
Speaker A
This is April the 30th, 1987, at about 10:30 p.m., in the home of... [name not clear in transcript] ...center of the very first vacuum triode. This is a most historical occasion. I'll show them some more.
Speaker A
drawing about 10 Vol oscillating between 9 1/2 and 10 volt to the input of the grid of the vacuum triode which is that little box right there behind the brightly lit 100 wat bugs now in the lower left of your
Speaker A
Okay, now for this second demonstration, here we have our 120 volt fan again, rotating, finally stirring up a breeze. Right behind that, you see a 24 volt DC motor. In front of that, there is a little rectifier. Here, see if I can get my finger here. This is a rectifier, and this is a transformer dropping the AC power down to 24 volts. You can see there are two 12 volt lamps in series, brightly lit, showing you that yes indeed, we have the full 24 volts. We're showing that this power can be transformed and can be rectified, just exactly like normal positive power, except, again, the power is very cool in the actual lines and the feeder circuits. Only in the actual resistive load do you have translation into normal power. But it can be run through a transformer and stepped down or stepped up. It can be rectified, and we can handle the power just as we do normal power.
Speaker A
volt uh the resistance for 24 volts applied across them and in front of that then uh we are rectifying this power to furnish DC power to the DC motor and so what this demonstration does is that with very little change to the input to
Speaker A
And you see again, at the same time, we have four of those lamps now lit, so we have another 400 watt resistive load going here at the same time. If we close up on our little meter here, we'll see that now we're drawing only 29.2... we get the glare out of there... 29.2 microamps. 29.2 microamps. We're still drawing about 10 volts, oscillating between 9 and a half and 10 volts, to the input of the grid of the vacuum triode, which is that little box right there behind the brightly lit 100 watt bulbs.
Speaker A
or step it down it's a very practical very uh straightforward type of power to use even though we're using negative energy in the lines and the characteristic when you switch suddenly power loads of negative energy you do not have the big flashing and arcing
Speaker A
Now, in the lower left of your screen, again, four brilliantly lit ordinary 100 watt lamps, household lamps. You can see here the 24 volt DC motor. You can see the transformer stepping down the voltage, the two 12 volt lamps in series, so that we have effectively a 24 volt resistance, for 24 volts applied across them. In front of that, we are rectifying this power to furnish DC power to the DC motor.
Speaker A
all that you can switch the load suddenly uh very easily with normal switches and so this is a very practical power you can see again the 120 volt fan you can see here a normal flat pancake type of 24volt DC motor you can see two
Speaker A
So what this demonstration does is show that with very little change to the input to the vacuum triode, we can provide a power which is practical. There's plenty of it. It's a very great power gain. It can be transmitted along lines without any heating. It can be rectified. We can use a transformer to step it up or step it down. It's a very practical, very straightforward type of power to use, even though we're using negative energy in the lines.
Speaker A
we're still providing 400 wats of power in the lamps and of course there wouldn't be any problem with turning the other lamp on and you have seen of course that we're still drawing less than 1/3 of a millatt we're drawing now
Speaker A
And the characteristic, when you switch suddenly, power loads of negative energy: you do not have the big flashing and arcing, because that's a positive energy effect. The arcing effect on these is reversed. In other words, it's a cold arc, an arc of cold, so you don't see all of that stuff, and you don't burn out the circuits and all that. You can switch the load suddenly, very easily, with normal switches.
Speaker A
operated a pancake motor being operated and 120 volt fan being operated all from less than 1/3 of a mwatt of power the rest of that power is coming out of the surging energy of the vacuum and this little box that you see right
Speaker A
So this is a very practical power. You can see again the 120 volt fan. You can see here a normal flat pancake type of 24 volt DC motor. You can see two 12 volt lamps brilliantly lit. You see the rectifier that rectifies the current for the 24 volt DC motor. You can see we're coming through a step-down transformer from the 120 volt negative power line, and you can see we're still providing 400 watts of power in the lamps. Of course, there wouldn't be any problem with turning the other lamp on. And you have seen, of course, that we're still drawing less than a third of a milliwatt. We're drawing now 29.3 microamps of current, and we are still sitting at about 10 volts on the grid, 10 volts, 29.3 microamps.
Speaker A
Model 2011 CR the maximum power this oscillator can put out is only three Watts when it's at full Peak power into 600 ohms and it has it's going out into 600 ohms and that would be 45 volts if you
Speaker A
want to use 45 how using 10 volt the maximum uh voltage that this little oscillator can put out is 45 volts uh however as you can see we're only using 10 volts as you can see right here on the
Speaker A
scale so we're using 10 volts of uh power to the grid uh voltage to the grid right now we have 29.3 stable very stable micro ERS on the grid so we still have less than 1/3 of a millatt of power on the grid and from
Speaker A
that we're pulling out of the vacuum from cathode to Plate we are gating and controlling uh well over 400 watts of power you can see the four 100 watt bulbs brilliantly lit and when I get off to the side you'll
Speaker A
see just how brilliant they are when the CD uh readjusts you see that we're stepping it down through the Transformer uh lighting the two 12vt bulbs going through a rectifier driving a DC motor which runs fine off negative power likes it real well and
Speaker A
then the 120 volt uh negative power is going to the 120 volt fan which again likes it very well indeed and so negative power negative energy taken from the vacuum is very useful and very practical power this power can be put into
Speaker A
production can be developed into for example a reasonable home power unit say a 15 KW and you can see that this box which we showed you a while ago with 500 watts on it it uh doesn't represent too much of a
Speaker A
step up uh problem uh we're not dealing with very much a magnitude Step Up problem and so our scale up problem should not be uh bad at all I will mention that the little box in the back the solid state vacuum triode see if I
Speaker A
can get my hand on this you can see my hand on it it is not hot it's solid solid state no moving Parts no vibrations absolutely rock steady and imminently practical it is not expensive uh ordinary Machining ordinary Parts
Speaker A
ordinary type construction can easily build uh this kind of a power device as we said the closest anomen clature for this device is a solid State vacuum triode nature itself is providing the river of current that's flowing from a
Speaker A
special cathode to a special plate and we are only putting in a very small control or gating signal to the grid to gate all the other power that you see being consumed right here this power can be transmitted it can be be transformed
Speaker A
it can be rectified it runs Motors it runs resistive loads and it's a very eminently practical type of electrical power very safe power and a very clean power that's waiting right now for development and marketing uh the incredible and
Speaker A
historic vacuum trial okay here we go again with the equipment shut down we'll give you a short tour through what is connected and the major types of meters that we have connected Ed so that measurements can be ongoing
Speaker A
dynamically first of all behind this card the little box that you see there is the vacuum triode invented by Mr Sparky sweet the incredible vacuum triode now we've placed over the triode some small strips of metal so that
Speaker A
you'll be able to see uh parts of the pattern of the magnetic fields surrounding the vacuum triode and as we come back away from the triode you see we have a load which is a bank of five 100 watt
Speaker A
lamps can be connected to the 120 volt uh AC output load 60 HZ these are ordinary common household lamps resistive load we have various meters you see the frequency meter measuring the output of the vacuum triode and you'll find that
Speaker A
that's a very Rock stable 60 htz here are some lines uh this is the input line right here uh to the vacuum triode grid uh nominally 10 volts RMS coming into the grid 60 Herz and as you will later see
Speaker A
very very low amperage will be measured on the micro ameter that measures the amperage going into the grid input so it'll be 10 volts plus whatever this instrument measures the next instrument here is the voltmeter itself that measures the GD
Speaker A
input and on this one we'll see the 10vt input the input signal itself is coming from an audio oscillator which is a sine wave oscillator it has a maximum output of 3 wats that's all you can possibly get out of it 45 volts into a 600 ohm
Speaker A
load that is what we're using for the input and as you will see there'll be far from far less than that 3 wats going into the vacuum triod then here are the triod output cables going to the instrumentation and then around behind
Speaker A
the back to the load to the lamps we will be feeding a 1 kilovolt 120 uh 1 kilovolt ampere 120 volt kba 120 volt transformer has dual 24 volt secondary the loads will be two 12vt lamps in series plus a rectifier plus a
Speaker A
24volt DC motor here is the rectifier right here coming from the output Transformer with the two lamps in series across the 24 volt output of the rectifier and with a 24v DC pancake motor motor 1/8 horsepower 2000 RPM which will be
Speaker A
energized here you see a voltmeter which reads the voltage on the rectifier output and then we will have a standard 120 volt AC fan load also connected to the output of the vacuum triod coming on back around now to
Speaker A
finish the inst struments we see a bank of instruments here we have first of all a voltmeter that reads the voltage of the output of the triod then we have a kilowatt meter that measures the actual power output of the
Speaker A
vacuum triode we take a look at the phase you'll see that that's really uh single phase crunt and everything's in Phase then the Amper being put out or the current being put out into the load by the vacuum triode and finally coming
Speaker A
around here we have an illos oscilloscope which will be set up across the output of the vacuum triode so that you can look at the 60 HZ output waveform we will show you the waveform on the scope that completes the primary
Speaker A
instrumentation with the exception of the frequency counter here where we actually show that it really is a 60 HZ uh frequency output and so Mr s will now turn on and energize the equipment and we'll take you through another
Speaker A
tour now turn got okay we're now turning on the oscillator and we just just heard the 24v DC motor start up the two 24v lamps are illuminated showing you that we're Furnishing power to that Transformer stepping it down the 24 volts going
Speaker A
through the rectifier lighting lamps and running the DC motor the same time before we step it down the 120 volt power is being furnished to the 12 volt AC fan and as you can see the fan is blowing up a nice pleasant fre here on
Speaker A
this very warm evening uh by the way this is May the 16th 1987 at the home of the inventor Mr Sparky sweet and from the lamps we want to call attention to a direct Ray which is invisible to the eye
Speaker A
but is visible to the uh tube the CCD uh solid state part of this camera you see a very straight beam of some kind associated with each of the lamps we're still investigating that beam okay the equipment is now
Speaker A
energized and ready to be connected let's take a look at the uh output wave form let get down at the right level and as you can see we have a very good sign wave in the 120 volt AC output from the plate
Speaker A
of the vacuum trial a very nice sine wave indeed and as you can see when we turn to the frequency meter we'll take a look here and you'll see that the we keep counting the frequency and it's right on 60 htz right
Speaker A
dead on 60 HZ you can see now that the power we are actually Furnishing to the grid this is the voltage it's about 10 volts it's oscillating between about 9 and 1/2 and 10 and on the microammeter these are microamps right now we only
Speaker A
Furnishing uh 7.9 microamp and yet we're running two Motors and lighting two lamps you want to energize the the other lamps okay we'll look first now at the bank of [Music] meters and we will see that for the
Speaker A
output voltage we've made a very careful adjustment and it's right on 120 volt right on the button 120 volts in the output AC uh this is the watt meter uh I can't get a good focus on that so
Speaker A
I'll read it for you dividing it by two we're putting out right now about 140 145 watts of power the power factor of course is one ampir we're actually putting out is about um about 1 five let me back up 1 Point
Speaker A
25 amp of power being output so we're actually putting out uh 240 Watts right at it now about 240 watts and yet we're only putting in 10 volts and 7.9 microamp 10 Vol 7.9 microamp so the total input is a tiny bit less than
Speaker A
8 80 uh micro wats we'll now energize the main lamps simply by connecting them into load screwing them in there's the first 100 wat bulb which goes in here's another one and here's another one and here's another one so we've kept the AC motor going we
Speaker A
kept the DC motor and the DC lamps lit we have 4 100 wat bulbs now being powered and when I come off of this you can see they are brilliantly powered when the camera is on the buls the CCD steps the lens down so that we
Speaker A
can actually get a picture so we're producing now well over 400 watts in fact if we come in on the watt meter right here let's take a reading we're producing uh 400 and some 80 watts and as you can see from The Meters
Speaker A
here at 10 volts and now 25.1 microamp we're putting in only 251 microwatts 251 microwatts and about 480 wats out so as you can see we have quite a power factor gain as a matter of fact the gain right now is approaching
Speaker A
1,500,000 for each nominal watt of power input one would get a nominal one point 5 megaw output in a bank of such devices this is May the 16th 1987 at the home of the inventor Mr Floyd Sparky suite and this is the
Speaker A
incredible vacuum troud which organizes and Gates Energy directly from the vacuum itself producing usable practical power so they really never changed anything did they that's well let's see now you want light on there you want the thing working yeah I need more light if
Speaker A
I can get it but the hell am I going to get no that's all right I I'll take it like that what I need you to do is explain what I'm what we're looking at here and turn yeah and I'll
Speaker A
uh we're at the home of Mr Sparky site this is 15 May 1987 and we're showing here the conditioning setup to actually make the vacuum triode uh to make the pump waves and establish them in the permanent magnet itself to make a
Speaker A
permanent magnet vacuum triod and so you can see here the large coil which we'll focus in on here a little bit it and the large upright coil here inside this large coil if we can go in there and see the
Speaker A
bottom there's another one there is another coil which we're not going to be able to see with that light but it looks about like a spool of wire like this I get on it here like this it's an entire spool of
Speaker A
wire number 15 wire Sparky number 15 wire with a GC okay about a 4 ohm impedance number 15 wire a whole spool of it is sitting inside the large conditioning coil down on the bottom right here we see the s CR is
Speaker A
part of the circuitry there's a light bub that gives him an indication of the voltage across the capacitor here you see he's reduced this conditioning circuit to using only one capacitor uh what's the capacitance of that uh this is uh 1600 1600 microf it's
Speaker A
A600 microfarad microfarad capacitor 250 250 volts ac working voltage AC working voltage DC DC working voltage and he has a varc trigger set Arrangement set up and a potentiometer to adjust the circuitry which we're doing now which he's now doing as you'll see by the
Speaker A
Light BB and there is the capacitor large tuning coil or conditioning coil with a coil in the bottom coil coil in the bottom is driven by uh wave wave Tech oscillator he has a wave Tech oscillator driving the coil inside
Speaker A
at the bottom through a 100 wat amplifier through a 100 watt amplifier and this this determines the uh natural frequency of the molecular structure that's the one that you impress in there right that's that when we open the gate in the molecular
Speaker A
structure of the domains Whatever frequency we impress with that inside bottom coil is the frequency that's put into the magnet as a memory in another words that determines the actual uh frequency of the pump wave you might say a cathode to
Speaker A
Plate uh oscillating current is established inside the magnet and by analogy that's what's established to make a vacuum triode the gate the gate here is opened by pulsating frequency of the uh capacitor discharge system which there's a capacitive discharge
Speaker A
system attached to the large coil it's being triggered by the Vic and as spark is pointing out that is going this determines across the time this set the time constant right this sets the time constant of that and that's going to determine the
Speaker A
uh gate opening in the uh Tri which is R time C which is R time C the RC time constant which is of course the resistance of the coil and passes master and fair and of course the time will be in second
Speaker A
Exel of the large coil is in ohms and the capacitance is in farads and of course the time is in seconds for the RC time constant which which in this experimental setup this particular magnet to be approximately 10 or 11
Speaker A
right in this magnet uh the resonant frequency of that magnet can be shown to be in the vicinity of 11 Hertz now each magnet will vary a little bit and uh you must find the actual frequency for each
Speaker A
individual magnet but it's around 11 Hertz for the size of magnets we're using right now in the demonstration device and that's that's determined by see shut that off for a second yes okay here we have placed one of the
Speaker A
magnets on top of the large coil maybe maybe I get that to and we're tuning the driver frequency down towards the 11 Hertz uh this is on the inside call we're driving now and when we get down to the resonant
Speaker A
frequency of the magnet you will see the lamination that's been placed on top of the magnet uh start to vibrate you'll see its shape and oscillate a little bit just at the frequency that is the resonant frequency of the
Speaker A
magnet do a little adjustment now makeing adjustment make it this is the amplifier is's tuning the amplifier voltage oh I plug this we have to plug it in there's a plug missing here hold I put the lamp in
Speaker A
I took that up see something and with me here this evening is Mr John bini oh wait a minute took took the oscillator off yeah okay now it's going see if we can get that going there see if we can get it adjusted right on
Speaker A
the resonant frequency let see a little lamination we I'm hit it just right can see this guy what you want oh I wonder we're getting it set up now for the right resin frange and that's a sine wave frequency
Speaker A
going to this inside call now you can the magnet should also be aligned with the Earth huh what is it you the long part of the magnet should also be generally aligned with Earth's magnetic field for best results things that I
Speaker A
can't see I can't see see where at 11 somewhere around 11z before right 11 yeah right there yeah to go too high there it is it's very lightly magnet is now beginning to resonate we'll see it just when we cross
Speaker A
it right on there it's a very small fairly precise spot frequency I can tell right away that's here see this one that may be a good indicator for you you know just hold it here hold it yeah but then you can set this you
Speaker A
feel it yeah there it is it is right yeah you want a resonance right right there there it is yes that thing's really moving now the magnet is in resonance and so we have the proper frequency 12 to resonate
Speaker A
the maget 12 and this particular magnet is resonating at about 12 each one's different each magnet is a little bit different even though going a little better no that's good no it's really going there okay that's in good
Speaker A
resonance now okay now you want it absolutely in perfect resonance right there you go there's the best resonance we can get and that's fine right there right see it's a 12 1/2 Hertz right there you go now you got both of them
Speaker A
locked oh this this one is at this one is at 60z and now we're putting the okay now you go go up with this one right yeah uh the 60 htz I'm sorry that's good right there if you go off just a little
Speaker A
bit to the edge there the 60 HZ was hold it we got to bring this one up okay with the magnet in resonance at its 12 and 1 12 Herz resonance there you go got to bring this up to the then we bring up
Speaker A
the trigger circuit at 60 HZ right which is being applied to the large coil and now it's stopped and there we are you can see yes just just should be okay you want to bring it down a little more till it
Speaker A
stops there you go now now now explain how the 60 HZ is the is in that magnet with the magnet at its natural resonance which for this magnet is 12 1/2 Hertz see see this circuit is putting in spiked signals of
Speaker A
60 HZ through the large coil uh triggered into spikes with certain RC time constant discharge determined by the capacitance and the resistance and that impresses the 60 HZ there you go into the magnet itself as a permanent memory and so the magnet will have a
Speaker A
locked in 60 HZ resonance and pressed in when it is in when it is in its natural resonance it has a natural window that's opening so the 60 HZ can be put into the actual nuclei of the atoms in the magnetic
Speaker A
domains themselves and once that's done that magnet 60z can't see is uh conditioned for the 60 HZ condition that's the cathode to Plate current is now conditioned for a 60 hzz current everything this thing was rocking yeah look now just sit
Speaker A
there so you just put it to the edge see see that mhm oh that thing's moving you want to get it going faster that's real good right there that's maximum okay that's 12 13 Herz at 13 Hertz we now have a maximum in this
Speaker A
magnet as you can see right here so it's a little we've shown the first part of the conditioning process to condition each magnet individually and now the I you say you have to condition this the entire magnetic assembly must be conditioned
Speaker A
and then you put the whole thing in and so as you can see otherwise you want to where you're at wa no now as you can see Sparky has assembled the two magnets over with the aluminum box that is the
Speaker A
holder and this is in the positive mode and the ends must be kept in the same direction they were in when they were conditioned before mode we put this in and they're in the attractive mode uh they're then placed in the
Speaker A
Box onto the into inside the large coil sitting down on the other coil so they're about in the center of the large coil they approximately centered in the large coil with a box in that position then the final conditioning process is
Speaker A
ready uh at this point you can hear the chattering as the beat frequencies go pump waves are going and all it remains to be done is to turn on the 10 HZ uh 10 volt 60 HZ driver signal
Speaker A
nothing's moving and at that point I see your driver signal is in the small coil this time right yeah that's the small Co 10 volts well in the case of the one we have inside is power to drive it is 3/4 of a m right
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13 of a m right and we don't change that no more right you don't change any frequency you don't change this thing here right everything stays the same after we get a good wiggle on the magnets yeah and you
Speaker A
put the magnets down in there just leave it on put put this sem in there put this whole sem in there and then you hit it with the frequency 60 HZ 60 HZ boom that's it the mem in there yeah stay there you
Speaker A
don't touch anything no no to to activate it you need a signal of 10 volt into the uh into the particular wire once it's which is not shown here right 10 Vols at 27 to 30 uh micro right will drive 500 W of power
Speaker A
out right so that's the conditioner you have to take the door with the two mag you know MH find first what that uh hole is no no no we find out first what the frequency is the natural frequency magnetic res
Speaker A
with the iron bar yeah know what that is now I found on the other one but I just took the two magets like that of course now I got together shirt slide slide I took them like this and I put
Speaker A
them like that okay so you mark the ends now I Mark the ends so you don't go back the same way mhm but I found what the what the frequency was now what it'll do what it'll do it'll average out the godamn godamn
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natural Resonance of this one and that one right you'll average it out right so what you read on here right it's a basic you know resonance magnetic resonance of magnetic domains right that know that's there so you know
Speaker A
what that is right mhm don't do nothing but take you know what it is MHM so you take them off of there and you put them on this box and you put the whole assembly down in there right right now
Speaker A
no no don't don't change nothing leave it right at that frequency mhm right mhm leave it at that frequency while it down in there okay then hit it with the with the uh 60 HZ the 60 HZ go in there and
Speaker A
stays in there right then you can shut the 60 HZ off take it out forg it now you put them keep the maget the same as they are remember though that you did it with this air kind of air gap you put you put
Speaker A
one on one stuck them down in there right but don't change this right because this has to this has to open it up while it's down in there not when it's up on here this tell where that frequency is has to open up the
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nucleus when it's down in there in the middle has to be in the middle right it's the maximum uh strength in the you put them like that you just stick them in there kind of I had a compass I was I
Speaker A
was oriented in the north south position right with the North Pole towards the north towards the South Pole of the Earth or them with magnetic field of the earth that's what I did okay I put it down in there like that
Speaker A
what all right now this is on right so it's rocking that's on mhm Co is on now you hit it with the frequency and that's it that's it that's it you can load the coils and go cool just hit the big coil
Speaker A
with the frequency right that's it yeah the pulse yeah and that's it you know that's it at that point the conditioning is finished and you now have a permanent magnet vacuum Tri incredible invention of Mr Sparky sweep this is May the
Speaker A
15th 1987 in the home of Mr Sparky site in Sherman Oaks California
Topics:vacuum triodefree energyover-unityalternative energy1987 demonstrationFloyd Sweetnegative energypower amplificationresonant magnetpseudoscience
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