Original subtitles

What is radiant energy?

If you're talking about radiant energy to me.

What do I consider radiant?

Okay. What I consider radiant is the capturing of a spike.

I consider that radiant.

You know, anything that, see

I generate the radiant energy.

I do that by my coils,

my switching circuits.

That's how I generate radiant energy.

In other words.

What I'm saying is that

I'm only concerned with a sharp transient in the spike.

As far as the radiant goes.

You know, as far as negative energy goes, the negative energy comes from the battery.

Once I generate this sharp transient and charge the battery

it's a negative effect of the battery because there's no heating of the battery,

with the radiant charger.

So basically, the thing is to

build circuits that generate these shock transients and then steal

that sharp transient and put that to the battery.

That way, I don't need much current at all to do it.

Next question.

-Could you talk a bit about the radiant spikes that we saw on the screen? The pendulumn's oscillation

The radiant spike.

The pendulum's a totally different machine, you know

And it's like one transient spike at a time.

You know, it's still have the same principle.

It's still each time that the pendulum goes up or the pendulum goes down,

but we just transfer that energy from one.

Right. It's a balancing act between, you know, the pendulum movement

And so one battery being lower than the other battery It balances between the two batteries.

it's still, it's still the same wave, except that the wave it's much longer in time.

-What happens if you try to swap the primary battery with a secondary battery that's being charged with the radiant?

Yeah, you cannot, you can't mix the two sources.

One, electricity is completely different than the next

one you're asking...

You're putting in a positive form of energy, right?

And you're asking for a negative form out, which is the radiant.

And so therefore, you can't just swap the batteries without a time period between them.

You just can't take the back battery and put it on the front battery because it's just going to kill itself if you do that.

However, you can put as many batteries as you want on the back.

Now you can move that to something else.

You take the battery that you charge and run an inverter, and then you could run the inverter and charge the front battery.

So you have to change the forms of energy because they're both different forms.

-So that would apply to every one of your devices?

Every one of my devices.

-In a normal circuit, when you increase the load, the current increases what goes on in your circuits?

You're talking about "Lorentz's law".

You're talking about the back EMF interfering with the work of the motor.

It's free in the monopole system.

We don't even go, we don't even have "Lorentz's law".

You know, we have no counterback EMF to slow down the motor under load.

So if we slow down the motor, we can't draw more current.

You never, you know, the current is just going to go down, motor is going to go slower, same pulse,

same spikes going to appear, same radiant.

But we're not faced with the "Lorentz's law" problem, you know, of counter electromagnetic force.

-Is the pendulum system a closed loop system?

No, they were two separate loops.

Two separate loops.

One being closed at the back and one being closed at the front.

But the two loops are not tied together,

and it's out of phase from each other.

So when the front's doing something, the back isn't receiving a signal at all.

It's not until the pendulum swings the other direction.

*So when the pendulum comes down, the trigger pulse comes in?

Well, no, it comes in after

You got to charge the iron in the pendulum.

And then that trigger pulse takes place later.

But 22 degrees after that.

-In that motor behind you, you were talking about an imaginary South Pole. Could you elaborate a little bit on that?

It's an imaginary pole between the two magnetic north.

Cause remember, these are sharp pinpoint beams.

And so they come up and they go round.

And then of course, the south appears and you can see that very

you know, you can see it with a magnetic indicator there between these poles

right in here.

The motor, isn't running until it's passable

between the two North Pole is an imaginary South.

And so being that this thing comes around and gets triggered,

you know, gets triggered here.

So when it passes the trigger circuit,

right, it's always passed the trigger circuit by about 22 degrees.

And so it's really in between these two magnets when the coil fires.

So.

It's just imaginary.

It's like.

It's a "scalar south"

you can see it with a magnetic indicator. It shows up, but there's no magnetic pole there.

That's where the fields all come together. Not a plastic wheel.

See actually, the shaft itself.

Well, if the magnet's way up here

and there's a loss.

How did this get to be south?

Cause this is a real South pole on the shaft.

And then, of course, coming here you have the North Pole going up comes around. Right?

But this actually becomes, and remember we talked about the magnetic beam,

being pinpoint on each one of these, so it's pinpoint.

And then in between here is the subscale.

These are all north poles together.

So these are pushed together to make up of a magnetic pinpoint beam.

So it's very. It's not a good generator.

So it has trouble getting triggered.

You know, when you, when you spin this thing.

But I don't know if you could hear this or not.

We get the thing to.

Those are the triggers.

And seems it's always triggered after the fact, there's only one trigger.

So.

And it's more like a big radial magneto.

You know, because the H waves involved in this too.

And of course, the light you see in the background

is being generated from the trigger.

Just from the scale of North.

Because there's no South Pole involved. It's imaginary here.

And that's what's driving the engine.

Take away the magneto.

And it'll just.

No power at all.

That's not generating a thing.

Now there's no drag on it, even though it's connected to the battery.

there's no vaccum.

*So there was a piece of the footage that I saw about, i think you were demonstrating about using multipole motor to...

and I'm not sure two connected batteries and you talked about 4 poles...

I think you were saying that.

Yeah, trade them

*You can trade them too

*so, yeah, it was about just making clear that they're, none of your devices can be used to flip the batteries.

No, you wouldn't want to flip the batteries. It's two different types of energy.

One energy is driving the system, the other ones are radiant type energy being put into the secondary battery

Now you can drive normal stuff with, it can drive a light bulb, you drive an inverter, drive a DC motor,

you can drive an inverter to charge the front battery as long as you keep the two electricities isolated

S o the battery performs, giving you the same thing that for some strange reason,

if you trade batteries back and forth, you just run out of energy.

I really dig a little bit of the back battery and use an inverter.

You can charge the front battery.

You have to change the form of it.

-So if you took an inverter you could swap back and forth?

Yeah, you could.

-That motor behind you, what does that have in common with your other motors?

They all remain the same no matter what size they are.

They all function absolutely the same.

There's a smaller one over there.

And there's another one and there's one over here. There's one in this corner over here.

And you see just the sizes have changed Although they operate identically the same.

-So in terms of their ability to restore battery current batteries there's no difference?

Right, that's the radiant charger that, you know the motor.

Yeah, you can notice the same thing

Because since these are such high voltage unit,

They just can charge a battery that's been sulfated.

It actually breaks the sulfation away

-So the radiant energy can restore a scrappy battery that's completely sulfated?

Yes it does, it breaks it up.

-There's a number of poles on the different motors in motion makes any difference their effectiveness, "John"?

Doesn't make any difference

Could be two poles, could be one pole.

-And in the context of your radiant charging machine. How do you see the term COP applying?

Well, the COP is completely different from what you're measuring.

You know, one doesn't have anything to do with the other.

You know, I have to go along with "Tom Bearden" on that that most people can't measure COP.

You know, they have no idea what this machine's doing.

The COP is in the battery.

You know, does the battery run longer? Does it take the charge better? Does it charge faster?

You see, how long could we sustain this battery?

You're building up the COP in the system by charging the battery with this type device.

Because we're not seeing any COP develop in the machine whatsoever.

It's all in the chemical, in the battery.

You can charge with this system and immediately when you load the battery, you're going to find out that it's extended.

You know, now you start calculating your COP because you know what the battery can put out.

You do that and everybody likes the favorite thing "joules".

But you know that if you charge this battery and you put this in, but then you get extended out.

In a word, you know, that under normal conventional charger, you're losing time each time.

This system gains time, each time. And it gets to a certain point. That's it.

That's as efficient as the battery is going to get.

-"Tom" talks about negative energy and you talk about radiant energy. Could you expand on that a bit?

They're both the same. They're one and the same.

You know, if you're talking about radiant energy, you're also talking about negative energy.

That's basically the same thing. It's the negative end of it.

I mean, a sharp transient, produces this negative energy.

-How do you see radiant energy coming in, "John"?

Well, it comes in waves.

You know, radiant energy comes in a wave.

So of course, you're going to see this alteration

because all the devices are switching all at the same time.

They're all at the same level.

But yet you see this rolling wave.

It's low in frequency, you know, So you see this sort of like ocean wave.

Sometimes it's higher, sometimes it's lower.

This is nothing more than what we were talking about it or any of these people, about the way they said that the energy comes in the waves.

Seems to me like an ocean wave or gravitational wave.

It seems to ride in on some form of gravity wave.

There it's up and down and up and down and up. Then sometimes it comes down stronger and sometimes it comes in a lot lighter.

It does change.

You know, this wave does change during, say, a full moon.

Some of these motors have been known, during a full moon, to speed up just a little bit.

You know, they actually go a little bit faster at night and a little bit slower during the day.

And of course, we've been able to see this on the Rpm gauges and things like that, that these things actually run a little bit faster at night.

So I wouldn't really say full moon.

*Who was the first person to pretty stumble into radiant energy was "Stubblefield" or "Tesla"?.

"Tesla"

"Tesla" is the one that.

Basically, you know, did everything radiant.

"(Nathan) Stubblefield" used it too, but a different form of it.

So.

It's just something that.

You know, people are trying to duplicate to this day.

We've found a way to do this. And we just charge batteries with it.

-According to "Tom", eventually there might be a possibility of running a huge charger output on secondary batteries that could power houses or whatever from just a .

Oh, yeah. If you look at a "Tesla" coil when a "Tesla" coil's operating

you think that the sparks that are being emitted from it are actually coming from,

but actually it's drawing this in,

it's more like a fluid and providing that you get this thing really into resonance and stuff like that.

This actually grows.

This, you know, envelops a whole field with this gaseous mixture of light.

You know, which is actually what you have to convert to get the energy, you know, from the vacuum.

You have to be able to convert this radiant and to be able to translate this,

to translate this in some form, and then turn it to something that's usable, like what we know is electricity.

But then once again, you know, you're going to end up charging a battery with it or you're going to end up running lights with it, or you're going to end up running a DC motor with it.

You know, no, just using this stuff right off you're not going to run an AC motor.

But you're gonna run an incandescent light.

-Could you talk about the nature of the radiant energy being a little bit more like a gas?

-Not like a conventional current, but like a nebulous gas.

Yeah. "Tom" talks about powering a battleship with a flashlight battery,

you know, which is entirely possible because we've seen some of these oscillators run down to 4/10 of a load.

You know, we've seen these things run in moonlight.

You know, so we've seen them go down. So we know of one volt they're putting out an amp or something like that.

So, yeah, it's entirely possible.

-So let me make sure I understand this. The system you're talking about would be the one that you currently have in development.

The system. It's our proprietary system. Yeah.

But I had to put that in there toy. Proprietary system.

You know, I'm not going to talk much about that.

*That's pretty much all of my questions.

So we're done. Now I can take this microphone off.

*We just keep going

*The book that you have now with "Tom Bearden". And what did you put in the book, "John"?

I have let loose all the inverted circuits "Tom" and I worked on to prove out what this stuff is.

You know, this is on a very minute scale, so people can actually make a working circuit.

So "Tom" and I were happy to let that go into the public domain.

Because we want people to work on this, you know, so they have no excuses anymore.

You just get the circuit, make the circuit, don't change anything and study what it's doing.

How it operates.

And that's my suggestion everybody, is just time to get to work.

You know, don't change anything.

Don't think that you know anything better right at this moment in time, because you don't, you know, it's you want the circuit to operate, just like I said, what's there

and then after that, after you get it working, you can make all the changes you want.

But up until that point, no.

If you make changes, don't expect it to work.

Do you really know what this pulse is and what's going on with this?

These inverted circuits and how the battery's being charged from the inverted circuit?

*And the first book, which is also being reprinted, the one from 1984, several people took that and

yeah, several people, the "Bedini's free energy generator"?.

Right, I think even "Mythbusters" tried to build that.

But yeah, anybody that follows that book, I would suggest that they follow it precisely

that they build it just like the diagram in the back and get it to go first.

You can solid state, build a solid state relay that does the switching like "Watson" did

But just expect that if you start running step with this, you'll probably disappear too, that's it.

I mean, "Watson's" machine was, like an 800 pound flywheel

and probably 15, 18 feet long, probably weighed something like almost 1500 pounds.

Right. And did some like 5 kva

it was running on two small little car batteries. and we're talking about a big math, talking about, you know, aircraft starter that he had to order special. Right?

But but once he wound up this flywheel to, I guess it was around maybe 400 or 500 RPMs

then he never... He only had a supply pulse every once in a while.

Click, clack, click, clack.

Capacitor charges up, dumps to the battery, capacitor charges up, dumps to the battery.

Same thing is the monopole motor now.

What we see. We tried to reduce the size of it so you could understand the effect of it.

The next day John Bedini demonstrates to U.K. mathematical physicist David Clements Ph. D how the radiant energy is captured and put to use on the bench.

This is reengaging itself. So the zero is in the center

*When you say reengaging it is basically changing.

Right. Let's do this episode, because everybody's always said to me, "I can't find the south pole".

Did you get that on film?

"I can't find the south pole"

Not balanced.

*He's just proving that the wheel's not balanced.

And that there's a rock inside of it

Okay, the professor must have his glasses.

Okay.

So see, there's a north

Are you getting this?

Here is the north.

And then you move out here and see here's the imaginary south

at about 23 degrees right here.

And this is since the motor is attracted, it's going to push away on this south. When it fires.

So then you come down here and there's the north.

See in there's, in between the south and the north is a zero.

And then there's the South again.

There's a zero between the north and the south. See, there's imaginary south there, and then there's the north.

All right, so there's an imaginary south here and a null out or a zero and a zero again.

And then a north. And then an imaginary south. A zero and a zero.

So there's there's like four.

What it's doing is coming around here like this.

Going like this.

Back to this one over here.

So now what we want to do is these are all north poles. You can see by the indicator that they're just all north.

There's no south poles out here,

and what we're going to do is.

Show you by, just the little trigger signal, and when these blink, that's the spike that you want to capture.

So let it pick up speed and it'll pick up speed automatically

is pulling a lot of weight right now. So.

Okay. But we're going to map these fields right now.

Okay. So what we have is a North Pole here and a North here.

So.

We have a south.

And that's there.

And then what we have is a zero here and a zero here.

So we have this all the way around the wheel like this.

So now we want to collect, the motor's pushing away at 23 degrees. This is actually 23 degrees.

The 23 degrees that John refers to here is actually the top of the range that one will normally encounter with an 8 pole monopole motor. The angle for this particular 16 pole motor is about 11.25 degrees.

Okay, so now we're going to run on the south. We're going to charge the iron with the north and we're going to run on the south.

So once again.

This is the radiant energy we're going to collect.

And you can see these things are burnt black.

From trying to contain that voltage.

So here. Now the radiant goes away and gets into the capacitor.

And now what we're going to do is store this charge and then discharge it across the battery.

So this is what we're going to end up with.

Each time

We're going to take another flash of that.

So once again, we're storing the radiant charge in this capacitor it gets to a certain level and we want to discharge it to the battery,

And each time the battery gets that discharge, this is what I get

*So the potential you're getting across that capacitor is a lot, about 400 Volts?

Yeah, but this capacitors probably about 75 or 80 volts here. With this capacitance.

If you were to use this point, it be like a 400 volts or 500 volt, much more than what this capacitor could take.

So basically what you're going to do is you're going to store the charge and you're going to repeat this operation over and over like this.

it can go up here.

See. And then you just, you time it.

So that you just give it that little bug right there.

Tell me about it, 2 or 3 seconds each pulse.

So you just need to be over the battery with this pulse like this.

So we didn't work with the capacitor.

Because of the way this arrangement is. And we just go right to the next battery and it absorbs the radiant energy.

See, this battery didn't have very much in it because it rose up at the beginning and lowered the impedance, and now it's putting the charge to the battery.

As the battery falls downward the impedance gets lower and lower and lower.

So the energy is actually getting absorbed into the chemical, right now

you want to repeat that again "Tony"?

+That's well.

So we'll watch the capacitor build this time and you decide which one you want.

We're starting now with a capacitor that really doesn't have that, a little bit

see, they charge themselves after they've been sitting

Once they're charged into this method.

And so, we've got this capacitor at zero.

Let's see it here. And watch is just going to build its charge up.

*That's just having one top connected?

Yeah.

Okay, so now we're going to connect it up and. And take this radiant energy.

Radiant Energy here and now we're going to just switch the currents

Okay, so here we go.

So this is what we've collected.

The radiant flash precedes the current flow.

So now let's not use a capacitor. Let's just tell the machine to charge our battery.

We're saying, this demonstration that the battery is actually the radiant collector.

So you can see the radiant energy is on their full.

So now we're going to connect this out.

The radiance's absorbed by the battery.

And we're just going to go ahead and push that battery up.

So now we've traded batteries, the battery that we've charged we now have driving the input

and the battery that's discharged we're now charging.

You can see it changing here. With that pulse.

*In effect, your sense is a say about 2% of the source battery and you can.

Yeah ,That's what I'm doing right now, right

So to show you that it's not generating anything with this movement, we disconnect the source battery.

And so it's not a generator.

Now we trigger the radiant out with this pulse, and we're doing the mechanical work and charging the battery.

We're doing this mechanical work here.

And so you have to take into account the electrical energy in the, electrical energy out, and the amount of work that the wheel's doing to keep that fan going.

*And always it seems to me like it's, that mechanical motion is needed, is almost as a byproduct to get an action to check out.

Yes, exactly.

To get the triggering each time in the coil.

You can see it speeding up. As its pins changes in the battery, it's starting to speed up more and more and more.

Kind of interesting a little bit.

So this battery now is coming up. See, it's almost at 13.50. So yeah, it's bouncing between four and five there, see?

Nine.

Each one of those pulses a little bit different.

*And you only had that on the capacitor for a few seconds.

Yeah, about less than that, we want to, we want to discharge this capacitor.

And then the other thing is don't leave the capacitors open because they sometimes build another charge.

*They build the charge when they're near to where the machine is?

Oh, no, no.

Just after we use them, sometimes they build up another charge and we think that's the residual left over in the plates as they expand back.

*So what you collected there and discharge was purely radiant?

Purely radiant, we transformed that high voltage into the capacitor.

And then, of course, we get regular electricity when we short this out.

We get real current flow.

So when the battery sees real current flow it just jumps.

All right. So.

The idea is to not have this capacitor because this causes then heat in the battery.

And what we want to do is take advantage of these high voltage spikes you see here.

So you can see here that the meter can't even measure.

It doesn't want to measure it.

It's got it locked, see?

*That changed the noise that you're hearing when you took off. Is just that or it's just the lights?

You're hearing the high voltage being triggered now, listen.

That's these pulses. That's the magneto effect.

So remember that this machine works.

Let me get this little bit in the camera.

Then what happens is this magnet comes down here and the iron charges, it becomes the same as a magnet.

Now, the magnet pulls away in the court that the magnetic field discharges

That then is at the correct sign to trigger the devices. You can see it here in one pulse.

There.

See.

I'm not quite quick enough, but see there.

It's after the magnet leaves.

*So that's when it reaches the zero.

Yeah, that's when it reaches a zero.

If we take these LEDs.

They're in two different phases here.

And we just go across the coil.

Okay.

In other words, put the LED across the coil.

And suppose we had a timing mark in the center here.

So let's say that we can do something like that.

Where we can get close.

You can see right away that the red one and the green one's flashing, but they're out of phase from each other.

So if you get it on there and

you hit the mark, it's a black mark and actually we need a white piece of tape.

But you'll find out that this will show you the timing if you look in here,

you see the two bars in here?

That's the timing.

See, it's after the fact.

It's after the magnet already leaves.

So it's got to be run another scale or so.

The imaginary pole.

So you would put a white dot

let's just get a white piece of

Let's just say we had this white piece of paper right

and actually it has to be much thinner that.

So if we put this in the center of the magnet. Right.

So it looks like.

There it is there. So it's right there on the green.

It's after the pole leaves.

Then, so you can make a simple set of timing lights by using two LEDs back to back and a couple of resistors.

So that you can see the firing across the coil.

And you can see it here.

You can see one is the charge and one is the discharge.

So that's one way you can do it to find the exact timing.

So what it looks like is.

Then when this white piece comes around. That's the center of the pole.

That it comes in it charges the iron, it discharges and fires right about there.

So that puts, basically

If we look at this.

These zeroes is basically where it's firing.

You follow me? Then it repulse, it's in repulsion because its already passed it.

So it's actually fired at 23 degrees, charging, discharging, firing,

Follow me?

Charge, time and charge, time and discharge of the iron.

And then the pole is in repulsion and then the motor spins.

That's exactly what's, how this is operating.

*So if you could talk about the conventional uses of potential and, for example, either conventionals will tell you how you can use a battery,

*how you can't use a battery or how you have to have them together and how you can't and how it will work in those ways.

Okay. So let's just look at it with these three batteries off the start.

So here's what we have.

We have this battery.

Which if we put these two together, we will get three volt

And of course, the positives at the top.

Negatives at the bottom.

And we only have one battery on this side and this is what we have.

So we have one like this, one like this, one like this.

So we have.

Another battery.

Negative terminals at the bottom.

This is the way I see differentials.

all right.

And these are both positive terminals.

Okay. So if you.

If I said to you okay, hook up the batteries this way.

what would you basically say was there? You would say there was nothing there, right?.

Because there can't be anything.

But there is.

We look at it, there's a potential.

That's flowing of 1.5 volts, positive.

*So in essence, what you're saying, is that

So if we look at it this way.

I look at the wave of 3.

And we keep it in the same phase.

And we look at a wave of 1.5.

Well, that equals 1.5.

Okay now if we have a wave.

That's 3.

And a wave that's 3 plus and minus.

They're in the same relationship.

So we've altered the frame.

We've taken this wave,

and we've moved

This frame underneath this frame.

Right. So basically what we're looking at is this.

Okay?

And this equals zero.

*So you can have hidden information on the zero

Yes, You can have hidden information because.

I could take this wave.

And expand that wave.

And expand that wave.

And I can then put information in here.

And then see this zero, when it's zero is out it's gonna equal.

This zero is going to contain.

All this information and all the substructure.

So that's the way I see differential equations and what I do in my circuits.

So if I say to you,

okay, I have a transistor here.

All right.

And I put this wave in it.

And I take this portion, right. And I take this portion.

And say that these are equal.

I am putting this information in the device.

But what's coming out of this end is just the scalar function.

Which is this, which is going to look like this.

*Great. So what you're saying is that's all of the substructure that you send in this wave,

*you pick off the substructure, which is in the zero, which is carried along with that wave.

*And that's where you picking up.

So suppose we did a sophisticated circuit and there was a device here and there was a device here, there's a device here.

And I pick off.

All these structures

A, B and C

Okay. And they all, they both have similar structures. Right.

And they're all

I decide that I don't want to form a zero.

I just want the potential.

So what I do is I take this A. And I go A plus B plus C equals some number.

All right.

And then I suppose i don't like this number, suppose this number's three.

And I say, okay, now what I'll do is I'll take this last potential

and I'll take this phase and beat it against this phase and get 2.5.

Because the way that's going to work is if I have this potential that's 3.

And this potential that's 2.

What I have out here is 1, along with the zero

Because it's trying to cancel out, but there's this difference in potential.

It's the same thing as if you took this battery.

So when we talk about inverted circuits in the book and stuff that's coming out.

if I have this potential generated with a spike.

And this is 300 volts, we just call it a spike.

I put this 300 volts to the plus,

and I take an invert, the transistor to the ground.

Right.

And I come up with some form of switch here.

When I closed that switch. The difference in potential is across this battery.

So if this is 12 volts, this is subtract this 300 volts.

And that's the difference in potential with charge in the battery.

So we want just potential and no current

*So in essence what you're saying here is two things.

*First of all, you're trying to get rid of the mathematics involved in current because you're not interested

I'm not interested in it.

*And the second thing you're trying to do, you're talking about a sort of hidden

variable

*Just to do with the potential difference in the hidden substructure within potential zero.

Right. The the whole idea is to hide all the information in the zero.

So this becomes a sharp transient. It becomes a very sharp, just transient.

And so we really expand that transient out.

What we have is all this hidden stuff inside the 0

*And that's an expansion of that.

Yeah, that's an expansion of this.

And that's how I see the electronics working.

That's how I see the motor working

I say that.

You know, this wheel has a North Pole and these are all North.

And we know.

And so, between these two north is a zero, two zeros, and a south.

So what I want the motor to do is I want it to give it the correct phase to fire.

So that's the north. So what happens is the magnet comes by.

And this field actually couples like this.

And this becomes energized.

*And this is this is the core of the coil.

Yeah. This is the core of the coil,

And so upcharge this iron, and it's at this potential.

It's charged.

Now, the magnet leaves, right?

And the iron wants to discharge. So it flips.

And that's the correct phase for this transistor to fire.

Right.

And then since it's an attractive motor, since it's the attraction instead of repulsion, what kicks the wheel away is this south.

It's imaginary.

It's really there because you can see it with the magnetic indicator.

And it's just enough, there's no power involved in the machine whatsoever.

In other words, you're not any torque being developed.

It's just a triggering mechanism to catch this energy.

*So in essence, what you're talking about is this south is the trigger to get the motion.

*But what you're really getting at is coming back to what you're talking about, the hidden information in there.

*it's when you pass the zero that you get this hidden information which is dropping.

I want to combine it into the spike and send that signal to the battery to tell it "Recharge!"

*So in conventional circuit, that all gets chopped off.

Yeah. In a conventional circuit.

If they see. If they see that.

They're going to short that out.

To protect this device.

But since I'm taking it off.

I'm just catching the spike and sending it to the battery.

I don't have to protect anything.

If I want to protect this device, I'm just going to put a neon light here.

I'm going to limit it to 90 volts

And that's exactly the way I see it.

*So the mathematics and the workings behind this is simply done to understand a difference of potentials and that's all you do

That's all I care about, is the difference of potential.

I move one potential to either a higher level or a lower level,

*So essence when, you can kind of get confused by plus or minuses.

That's why I can use, right, that's why I can use two identical batteries

because I'm building up the potential to take one.

There is no free launch, you have to do the work to get it

*But once you

Once you understand that fundamental, you can take all your electrical circuits

And look at them as a differential and say, gee, I can take a little bit from here.

I can take a little bit from here and think about it.

It's all in the same phase, it's all additive.

Now I've got this high potential.

And if my potential is too high.

I can direct another phase and subtract from the potential.

Because it's out of phase by a lesser degree.

So, in essence, I'm looking at a wave.

It may look like that

Or I'm looking at a wave that may look like that.

Now, what's the motorwave look like?

*So this is your...

See this is the actual battery level.

And this little piece, where do you see it on the scope that comes down is in the negative range.

The device is going negative.

It actually wants to become a negative resistor or a "Negastor"

A transistor that's a "Negastor".

So that cools it off.

*Okay. Okay.

And that's just the way I see it.

The formal session is now over but, after removing the mike, John continues the lecture.

So, the motorwave... this is the battery level.

And then the spike.

Is here.

*Ok, But what I mean is when you, when you look at all the spikes together.

Oh, yeah, yeah, yeah.

You're seeing, you're seeing that.

*That's right. That's right.

So actually what you're looking at it's digital signal.

For somebody to build the receiver to pick up the background.

That's a real faster one, that's like in the terahertz and beyond.

*So would you kind of say that it seems to me that a second attributed wave.

Yeah.

*So what you're really loking at it's the kind of motion of wheel ?

Yes.

Yeah. But this one's longitudinal

*That's right

This is the EM.

And this is the longitudinal

*Cause what I was thinking about this must show you is you have that T field part and you've got the normal magnets and that's the pressure, right?

That's the pressure

*So in kind of thinking that's natural. These are kind of pressure.

Is a pressure way.

So what you want to do is build a receiver.

That tunes into the pressure wave.

See, it's way beyond light because you have to capture individual particles.

Then you have to convert them into something.

To turn into electrons, because everything is electrons.

*So in essence, everything that's like explanation blows to the transverse and this is the access is the pressure part.

Yeah.