0:00
NeuralStan
·
This is The Leaky Condenser, part 3 of The Textbook Behind the V, I, C, made by the archive at Stan's Legacy.
0:05
NeuralStan
·
I am NeuralStan, and I am a machine, not a man.
0:11
NeuralStan
·
Two other synthetic voices speak.
0:13
NeuralStan
·
Stan Meyer's is cloned from thirty seconds of him speaking in nineteen eighty-five.
0:17
NeuralStan
·
The other speaks for Charles Steinmetz, the electrical engineer; the archive knows of no recording of his voice, so it is a stock voice.
0:24
NeuralStan
·
Each reads only words they wrote or said, and every one is cited.
0:28
NeuralStan
·
Meyer is clear that the water cell is a capacitor.
0:30
NeuralStan
·
His patent calls the water a dielectric liquid between capacitor plates, and his raum und zeit article gives its dielectric constant, seventy-eight point five four at twenty-five degrees.
0:40
NeuralStan
·
And in a memo he says why a capacitor matters to the circuit at all:
0:46
Stan Meyer (synthetic voice)
·
This opposes any changes in circuit voltage.
0:49
Stan Meyer (synthetic voice)
·
A voltage change cannot occur until the stored charges can be altered through current flow, if allowed.
0:56
NeuralStan
·
A capacitor holds its voltage until charge flows in or out.
0:59
NeuralStan
·
That is the property the whole voltage intensifier leans on.
1:04
NeuralStan
·
But in the same article he says the water is also a resistance:
1:08
Stan Meyer (synthetic voice)
·
Water now becomes part of the V, I, C in the form of resistance between electrical ground and pulse-frequency positive-potential, helping to prevent electron flow within the pulsing circuit.
1:20
NeuralStan
·
It is easy to read those two statements as a contradiction.
1:22
NeuralStan
·
They are not.
1:24
NeuralStan
·
Every real capacitor with anything but vacuum in it leaks, and water leaks a great deal.
1:29
NeuralStan
·
Meyer is describing a capacitor with a resistance across it, and that is a case the textbooks solved.
1:36
NeuralStan
·
Fleming's condenser is the Leyden jar, and he describes its discharge with a picture worth keeping.
1:41
NeuralStan
·
When a condenser is discharged through a conductor, he writes, the potential energy runs down as a current, just as when a bent spring is released.
1:50
NeuralStan
·
More to the point, in section thirty-one of his third chapter he works through exactly Meyer's arrangement: a condenser with a resistance across its terminals, placed in series with a coil.
1:59
NeuralStan
·
He shows the pair behaves as though the coil's resistance had gone up and its inductance down, and that with the right values the leaky condenser cancels the coil's inductance altogether.
2:07
NeuralStan
·
We come back to that in the last film.
2:11
NeuralStan
·
Fleming gives the one number that tells you how long a leaky condenser holds a charge.
2:15
NeuralStan
·
Multiply the resistance by the capacity and you get a time, which he calls the time constant of the condenser.
2:20
NeuralStan
·
In one time constant the charge falls to about a third.
2:24
NeuralStan
·
And in a period of five or six time constants, he writes, the condenser is practically discharged.
2:32
NeuralStan
·
Steinmetz says what kind of change that is.
2:35
NeuralStan
·
With only one energy store in a circuit, he writes, the transient can only be a steady logarithmic term, a gradual approach.
2:41
NeuralStan
·
A leaky capacitor on its own never swings.
2:44
NeuralStan
·
It simply drains.
2:47
NeuralStan
·
Don Gabel measured the estate's tube cells in two thousand and nine, empty and with three waters.
2:52
NeuralStan
·
His meter reports a capacitance and a dissipation factor, which is what the part wastes divided by what it stores.
2:57
NeuralStan
·
A good capacitor reads well under a tenth.
3:02
NeuralStan
·
Empty, the cell is twenty-two picofarads.
3:06
NeuralStan
·
With rain water, the meter reads twenty-one nanofarads with a dissipation factor of twenty-nine.
3:13
NeuralStan
·
Read as a capacitor with a resistance across it, that is about two hundred and sixty ohms of water in parallel.
3:17
NeuralStan
·
Distilled water came out almost the same.
3:21
NeuralStan
·
Tap water was seventeen ohms.
3:23
NeuralStan
·
On a meter, at one kilohertz, every one of those cells is more resistor than capacitor.
3:30
NeuralStan
·
There is a second thing in Gabel's table.
3:32
NeuralStan
·
An empty cell of twenty-two picofarads, filled with water whose dielectric constant is seventy-eight and a half, should read about one point seven nanofarads.
3:41
NeuralStan
·
It reads twenty-one, more than ten times as much.
3:45
NeuralStan
·
And tap water reads twenty-five microfarads at a hundred hertz and less than six at a kilohertz.
3:51
NeuralStan
·
Capacitance that is far too large, and falls steeply as the frequency rises, is the usual signature of the double layer: the thin sheet of charge that forms where metal meets water.
4:02
NeuralStan
·
It is the same effect a University of Latvia laboratory measured in two thousand and twelve, pulsing a cell through a bifilar transformer and a diode.
4:08
NeuralStan
·
For a builder the lesson is simple.
4:09
NeuralStan
·
A meter's capacitance reading of a wet cell at low frequency is mostly the double layer, not the water.
4:15
NeuralStan
·
Measure at the frequency you will pulse at.
4:21
NeuralStan
·
Now put Fleming's time constant to work.
4:23
NeuralStan
·
Gabel's rain-water cell holds its charge for about five microseconds.
4:27
NeuralStan
·
The archive's film Resonant Action did the same arithmetic for Meyer's own cavity, a sixteenth of an inch of water between two tubes, across four grades of water.
4:37
NeuralStan
·
Tap water drains it instantly.
4:39
NeuralStan
·
Ordinary distilled water holds for a microsecond and a half.
4:42
NeuralStan
·
Very good distilled water, seven.
4:44
NeuralStan
·
Deionised water holds for a hundred and twenty-nine microseconds.
4:49
NeuralStan
·
At five kilohertz the gap between pulses is two hundred microseconds.
4:54
NeuralStan
·
So by Fleming's rule, only the deionised cell keeps any meaningful part of each charge until the next pulse arrives.
5:01
NeuralStan
·
Every other water has let it go.
5:04
NeuralStan
·
Meyer knew this.
5:06
NeuralStan
·
In his patent for the gas generator voltage control circuit of nineteen eighty-nine, he wrote that distilled water, like air, having no conductive medium, will inherently inhibit electron leakage, and that sea water or water with a mineral content would tend to draw current and curtail the operation of the generator.
5:24
NeuralStan
·
The textbooks say why.
5:26
NeuralStan
·
Everything the voltage intensifier does, the overshoot, the stepping, the ringing, needs the capacitor to hold its charge between pulses.
5:35
NeuralStan
·
The leak across the water decides whether it can.
5:38
NeuralStan
·
Water quality is not a detail of Meyer's specification.
5:40
NeuralStan
·
It is the condition the whole circuit depends on.
5:45
NeuralStan
·
So, what to measure.
5:47
NeuralStan
·
Your cell's capacitance empty, and then with your water, at the frequency you will pulse at, and always with the dissipation factor.
5:52
NeuralStan
·
The water's conductivity, with a meter, at the same time.
5:56
NeuralStan
·
From those, the resistance across the cell and Fleming's time constant.
5:59
NeuralStan
·
Then compare it with the gap between your pulses.
6:04
NeuralStan
·
And write the conductivity down beside every other number you take.
6:07
NeuralStan
·
A result without it cannot be compared with anyone else's, and that is the main reason so many replications cannot be compared with each other.
6:15
NeuralStan
·
The next film is the heart of the series: the resonant charging choke, and the doubling Steinmetz and Fleming both describe.
6:21
NeuralStan
·
The written tutorial, Gabel's readings and the Latvian paper are on the site.
6:26
NeuralStan
·
The archive is at stanslegacy dot com.
6:27
NeuralStan
·
Thank you for watching.
6:31
NeuralStan
·
Every source in this film is in the archive.
6:34
NeuralStan
·
The addresses are on the screen.