Hopefully everyone has seen the John Shive "Wave Similarities" video. In that video he demonstrates his mechanical wave machine where it is clearly visible how waves propogate, reflect and are dampened. This is pretty neat to watch happen with a slow mechanical system, but how can we do the same with an electrical system where the waves move much faster? We can use an oscilliscope to look at the superposition (final result) wave, but we have no means to clearly see an audio frequency wave propogate through and reflect from various electronic components, especially custom wound inductors (such as bucking coils). What I think we need at the bare minimum is the equivalent of an audio frequency SWR meter. With this, we could at least get some idea of what nodes exist and what the minimum and maximum node values are, then we could attempt to tune these systems--impedance match them.
For instance if I connect an 8 ohm load resistor to my 300 watt PA amp on the 8 ohm output terminals, nearly all the power gets dumped into the load resistor because it is impedance matched. But if I add a couple of chokes to each side of the transmission line, it's nearly impossible to guess which output terminals I now need to connect to for proper impedance matching. My scope only shows that I'm not matched, but it doesn't give me any hint as to what direction to go in. So this is one problem we need to tackle.
Now for amp restriction, what do we needed to do? I'm thinking here we need to create a standing wave. This is basically setting up a reactive power scenario where the voltage and amperage are 90 degrees out of phase from each other. The amperage is actually there, but since it is out of phase with the voltage, it simply gets all reflected back to the source and ends up costing us nothing. So how do we do this? Well, again like in the John Shive video, we can either have an open-ended transmission line or closed-ended. One way will reflect a mirror and the other way an inverse mirror. For our purpose a closed-ended setup would seem more appropriate since we are not trying to propogate the energy wirelessly. All we want are the oscillations. This is the source and termination of the first transmission line. The second transmission line is between the end of the first and the cell. The end of the first transmission line leaves us with simply oscillations. Now we need to superposition these oscillations so that they continue to build upon themselves in amplitude and as they do this, they need to swing more and more positive each time so the DC component becomes stronger and stronger. And finally we dump these positive oscillations into the cell with the impedance matched so the full energy of the wave is absorbed by the cell. This is where I think the gating plays a role. When the oscillations from the first transmission line stop, the built-up DC potential in the second transmission line bursts into the cell. And when that energy is completely abosrbed by cell, we restart the whole cycle again.
I wish I was sharp enough to build a demonstration of this whole system using water waves, because I'm sure if everyone could see how it worked, visually and in real-time, it would become obvious what we need to do electrically. The main thing we need to keep in mind is that each end of a transmission line has an impedance, which means we can have a fixed impendance on the terminating side and a variable impedance at the source. This will alter how the reflected waves reflect again at the source side even though we may not alter the source signal at all. Here's an example:
Suppose we have a 50 ohm transmission line, 50 ohms at the source side and 50 ohms at the terminating side. We send an impulse. The impulse travels down the line and gets completely absorbed on the terminating side. Now we change the source side to 10k ohms. This time the impulse travels down the line and because the terminating side is still 50 ohms (different than the 10k source side), it reflects. And when the impulse gets back to the source side, it reflects again and so on, because of the impedance mismatch. So we have the ability electronically to change the impedance at each end of the line on the fly, making it possible to do all sorts of things with the wave(s) bouncing back-n-forth on that line. My theory about adding chokes on the transmission line is that they artifically extend the length of the transmission line, same way a loading coil on an antenna artifically extends the length of the antenna. This now artificially extended transmission line gives us time to manipulate the waves on this line in real-time. And one way I see straight off is by making one leg of the transmission line slightly larger or smaller than the other--think adjustable choke. Now you have a curved/biased transmission line.