## Thursday, February 24, 2011

### 73 - voltage taken at the drain

This is for Poynty who wanted to see the voltage at the drain. Hope it helps.

Kindest as ever,
Rosie

Channel 1 shunt
Channel 2 battery
Channel 3 Gate
Channel 4 Drain

### 72 - yet more on those elusive electromagnetic properties

The only thing that I predicted - in terms of the thesis - was that current from the supply would induce a counter electromagnetic effect in a resistor. This could, theoretically, be routed back to the supply to recharge that supply. To my way of thinking this would result in some level of charge conservation at the supply. I am afflicted, as mentioned, with a rather literal turn of mind. Therefore, as I saw it, if current flow is at 90 degrees to the voltage - and if current from the supply induces a corresponding but opposite voltage in the inductive/resistive components of the circuit - then current flow is the electric moment of the electromagnetic interaction and voltage the magnetic moment. As I understood it, as there is a measurable voltage induced in that inductive/conductive resistor then allow that resistor voltage to 'equalise' by interrupting the current from the supply. And it, in turn, will induce an electric moment at 90 degrees - but in counterphase to the energy supplied from the source or initiating supply. And then? Obviously in as much as current is then returned to the supply then the supply would be recharged to the extent that it was first discharged.

What I did not realise is that mainstream were very well aware of this. But the difference was this. They NEVER returned that energy to its source. For some reason this was seen to be of no value - no net gain to the system. I sort of saw it as a recycled current. They didn't. To this day I battle with mainstream concepts and I know that I am barely beginning to understand it. But there are huge differences - obviously. The main one being that I also saw current and voltage as having material properties. In other words, to me, current comprised the same magnetic dipolar particles that voltage comprised. They were the same fields - but separated from ech other by a critical spatial distance. Circuit conditions allowing, then current simply moved to establish a charge balance that first initiated that measurable voltage imbalance.

So. In my book current is the movement of imbalanced fields of magnetic dipoles that are first measured as voltage. But when that current induces other opposite voltages in sundry circuit material - then that material also needs to move to a 'balance' and it, in turn, will discharge current to resolve that imbalance. Therefore that circuit material - that circuit component - is as capable of being an energy supply source as is the energy from the initial supply both being evidently capable of inducing the electromagnetic interaction.

And I know that it's round about now that I've lost the most of my readers. The point is critical but subtle. Voltage is always a measure of potential difference. And current is the means whereby potential difference is discharged. Voltage is localised to sundry components. Current flow is not localised but requires a current path. Both fields are structured from one dimensional fields. These discrete and orbiting fields were previously binding sundry atomic material into solid or liquid three dimensional amalgams. If the valence condition of that amalgam is sufficiently imbalanced and extreme, such as is found in the electrolytic condition of batteries - then these fields split apart. They literally become spatially separate. This partially resolves that experienced imbalance. But it is at the expense of the bound condition of that amalgam. The other half - the remaining fields that have not structured themselves into magnetic fields - are no longer able to bind those atoms. This induces a cascading condition of disorder where those remaining magnetic dipoles - the other half of all those discrete binding fields, then come out of 'orbit' - out of their balanced condition. Their thermal properties are then locally evident and measurable.

However, if there are circuit paths to enable the discharging voltage/current to be returned to that localised voltage imbalance - then that imbalanced 'hot' condition can resolve itself back to it's cooler bound condition at the expense of voltage imbalance. The magnetic dipoles, moving as current, can then resolve themselves by losing that imbalanced 'field condition' to split back into discrete parcels of one dimensional strings that re-establish their orbital interaction with the atoms - specifically, with the atomic energy levels. In effect voltage is the measure of imbalance. As a field it can move as current flow. If it can do this it can then recombine a more balanced bound condition with the atoms. Magnetic fields always move to promote a condition of balance.

I keep saying all this. I just wish it could be understood. I keep hoping I'll stumble on the right way of explaining it.

Kindest regards,
Rosemary

Added. Perhaps this image will explain it better. Imagine that voltage is a continual line of magnetic dipoles that arrange themselves in a series of concentric rings around a specific component. Then imagine that this spring is released into a long line that moves through the circuit to effectively reach back to itself. That spring is the voltage. That dispersion through the circuit is current flow. But that spring is actually only the sum of one half of another field that is not able to 'orbit' or structure itself as a 'field'. The material in that spring and their other halves need to 'join up'. If they can do this then they can again split into discrete little orbits - join up with those separated isolated packets that are hot and bothered without their other half. When they join up they can then go about their work of binding atoms together. Then they again become balanced orbits and then they're again invisible and cold - both.