Determining the measure of a wave length between wave guides

[Hidden]

Im going to be starting a few topics of current interest... these topics will not be for solving the total problem but more or less going into a further depth of understanding in specific subjects of importance.. We must decipher the whole system incrementally in order to understand the mechanism as a whole..


I am not sure of the proper approach for determining the wavelength between a gap (waveguide)

Any info or opinion on this topic please share.

[Hidden]

Here is a perspective of the wavelengths involved in a unipolar dc voltage

[Hidden]

Column 11 Row 44
"Since resonance is a matter of matching a physical distance with frequency of the back and forth motion over that distance, matching the particular wavelength, can be either d.c. voltage pulses or the duty cycle pulses."

[Hidden]

Maybe the chokes were made to match the water and source impedances to become a transmission line.would be a super conductive conduction under ambient temperature...


In Fig. 17, you can see that the output current is clearly dominated by the resistance until the cable behaves like a transmission line. The current from the generator (AC) should be equal to V/R ... V is 1 Volt, and R (for the 100 metre line at 1 ohm/ metre) is 200 ohms (including the two external resistors). This works out to 5mA, and indeed, that's exactly what is measured - until the "magic" frequency of 100kHz, where the current increases.Above 1MHz, the current is 10mA (1V /100?), meaning that the cable resistance has disappeared! In the space of one decade in frequency, the cable has transformed itself into a true transmission line, where the signal is not conducted as such, but transferred by a waveguide (waveguides are usually just tubes for UHF signals [e.g. microwave], however a wired transmission line is also a waveguide). Naturally, the resistance never really disappears, but its influence is greatly reduced.It is worth noting that a cable will never act as a true transmission line with a defined (and maintained) Zo unless its source and load impedances are equal to the line impedance. This means that no audio cable will ever be a transmission line, (almost) regardless of length, unless the amplifier output impedance, cable impedance and load impedance are all equal at all frequencies within the desired range. No known amplifier or loudspeaker system can meet these criteria. Alternatively, the cable may be infinitely long, however this is usually impractical in a domestic environment.


i know is not very related but if you think longitudinally maybe the frequency of the tube were a harmonic of the used resonant frequency...



http://www.sound.westhost.com/cable-z.htm

[Hidden]

First things first stan is transmitting only a positive  force into the cell the negative potential being inverted and having only a "Unipolar" pulse entering the cell..

my philosophical perspective is
The negative side is being "restricted"  Stan is only influencing a positive polarity into the cell (a vacuum to the electron)..  To find the proper wave length you simply have to vary the duty cycle while being in a amplitude range that complies with the gap .. all the duty cycle is gonna do is gate the unipolar dc voltage in a proportional manner of on/off..  its a circuit to adjust how many unipolar pulses per on and off..

A system that is generating a doubled frequency of 400 hz unipolar voltage can only gate a minimum duty cycle of 200hz.. The scr only shuts off as the amplitude of pulse falls again to a certain gradient. Since stan is applying a vacuum  while restricting amp flow on the negative side, voltage is gonna wanna collapse in the cell naturally it will influence the scr to shut off