I should note that in this video I state that I get mabey 12v when connected to the cell.
As you allready stated in your video, you cann´t make this alone and I want to help with some thoughts. So maybe this can help you a little bit (some things are quite good known). :shy:
For me it only make sense to investigate the VIC. (Let us forget the 8XA and other circuits for a while). Because of replications and theoretical research we know that this circuits work with current (A range) and the VIC can work in mA Range.
What do we exactly know about the VIC?
Basically the two chokes should inhibit the current as much as possible I think. We know -because of some experiments- the WFC alone cann´t inhibit current. The tap water is an "electrolyte" which is conductive because of the pollution in it. Mainly iron (brown pulp).
To inhibit the current, the only possibility is to do this with the chokes:
1) resistive coil wire (Rs1,Rs2)
2) they are large enough (>1H) to block current with frequencys around 10kHz (L1,L2)
But there is also an effect which we should consider. Because of the multi layer of the coil, there is a large C in parallel to the L of the coil. This is called
http://en.wikipedia.org/wiki/Parasitic_capacitance
It seems to be purpose to gain a large C component of the coil to lower the resonant frequency. (Cd1, Cd2)
I also stated this in this post http://open-source-energy.org/?tid=170&pid=10219#pid10219
Each choke coil for it self is a resonant circuit (parallel). FL1 & FL2
We know that the impendance Z of a parallel resonant circuit when matching the right frequency is nearly "infinity". This can inhibit the current very good. In this diagramm it is only for demonstration of the chart of Z. (the values are examples)
There exist the VIC readings for example:
Choke 1: L=1218mH C=157pF---> fres would be 11.507Hz
Choke 2: L=1093mH C=180pF---> fres would be 11.347Hz
Nearly the same frequency. So therefore the secondary choke always shown as a variable L in the patents to match the data of the first coil.
Adding the resistive coil wire, one choke element´s Z can be very very high.
So the complete input voltage of the main secondary drops over the both coils because they work like a big impendance Z.
What will happen, if the core want to transfer the stored energy but it is limited in current. -->The voltage will rise automatically on the secondary main. Each ignition coil works like this. This grown voltage will be devided to the two chokes.
Ok, now we can inhibit the current and we can rise the voltage on the secondary.
The only way to get a potential difference measured over the WFC is to drive the two resonant circuits (C1 and C2) 180° out of phase. =bifilare wounding; when they are working in the same phase, this will not work I think.
So physically it is better to make the complete secondary side of the VIC electrically isolated to the primary side (floating ground). So the C2 can performe well and no current can flow back to the primary side when turning the phase.
But to establish the right frequency the capacity of the cell also has to be involved in the calculation -->PLL makes this automatically.
Because the two parallel resonant circuits are out of phase, they can create a potential difference which is changing ~10000x per seconds. But because of the diode, the C of the WFC can load only in one direction. The C of the cell cann´t discharge.
This voltage measured will always be 0V. Because no multimeter can measure such signals we should measure with an oscilloscope. But we need equipment for high voltage:exclamation:
Just some ideas. Maybe this can help you, when continueing testing the VIC and the cells.
I wish you all good luck! ;)
:)