Sparky wrote:there are no birkeland currents without electrons moving through them, being supplied by a voltage source. If an arc mode birkeland current is conducting into an area that disperses the current into glow or even dark mode, the filament may appear to be disconnected, but if the arc can be seen there is current [electron] flow. And the arc will not loop back onto itself because it is basically of the same charge [voltage] throughout.
It was my mistake to be talking about Birkeland currents, and the more I come to understand them, the greater the difference between them and what I am imagining. So let's take a stroll through what I think I'm saying, and let's not think Birkeland currents, but rather let's call them New Type of Current X (or something).
For the sake of the visual image, we need a prime mover. This is where the construct is the weakest, but we need
something as a starting point, so that we can at least inspect the mechanistic properties of the rest of it. So let's use a nuclear explosion deep in the convective zone as the prime mover. For our purposes, we neither know nor care what caused this explosion -- we'll just use this as the stand-in prime mover. Anyway, as a consequence of the explosion, a bunch of neutrally-charged matter is accelerated to an extreme speed. In the ejecta, there will be atomic nuclei (some of them newly-fused into heavier atoms, and some of them just other atoms that got ejected from the explosion without being part of it) and there will be electrons. But at the temperatures in question, the atoms won't be able to hold onto the electrons, so it will all be pure plasma.
Now let's consider what will happen as the plasma expands outward from the explosion. Initially it will be traveling at thousands of km/sec. If the explosion occurs deep in the convective zone, the plasma will encounter friction from the surrounding plasma that will slow it down, but at least at first it will be traveling at an extremely high velocity. So what's going to happen?
We know that electric currents generate magnetic fields that then exert back-pressure on the currents, consolidating them in the effect known as z-pinch. Normally we think of this as an effect on moving electrons. But protons have electric charges too, so they should be capable of generating magnetic fields too, and thereby getting their own pinch going.
So this isn't really a "current" at all -- it's a plasma jet. And so far, the charges haven't been separated, so we really can't call it an electric current. It's just a bunch of matter moving at an extreme speed, that overall is neutrally charged, though it's all pure plasma.
But the magnetic fields generated by positive and negative charges spin in opposite directions, and therefore repel each other. So we won't expect just the electrons to get pinched, and for the atomic nuclei to get pinched as well -- all in the same jet. Rather, we would expect positive and negative charges to get split into parallel streams. So we'll end up with all of the electrons in one pinched stream, and all of the atomic nuclei in another pinched stream, and with some distance between them. Here's the image:
Figure 4. Opposite charges traveling in the same direction are attracted by the electric force, but repelled by the magnetic force.
If this is not correct, I need to know, because then probably the whole construct needs to be tossed. I'm not actually sure that I have ever read about this anywhere -- maybe this is just my imagination, based on what (little) I know about the theory of it all. But it stands to reason that if the speeds in question are capable of z-pinching charge streams, then opposite-polarity magnetic fields should be capable of separating charges. If opposite magnetic fields didn't repel, electric motors wouldn't work, so I think I'm correct here.
Anyway, now we have a charge-separated plasma jet. We started out with 360 degree radial expansion from a nuclear explosion. But because of the z-pinches, we end up with focused jets, and they're charge-separated streams.
So these aren't Birkeland currents at all -- they're charge-separated plasma jets. The only sense in which they are "currents" at all is that they are "moving electric charges" generating magnetic fields as they go. But they are not responding to an external voltage. (So are they still "currents"?) Anyway...
The interesting thing is that we now have parallel, oppositely-charged streams, so there is a voltage between them. Now, if all of the above is correct, and if all other factors were the same, we'd expect these parallel streams to speed out into space, attracted by the E field between them, but buffered from each other by the opposing magnetic fields.
But all other factors are not the same. What if these streams are pushing their way up through the convective zone, and being slowed down by friction? Then they will decelerate. And we know that the strength of a magnetic field is a function of the amount of charge, and the speed at which the charge is moving. So as friction slows down the charge streams, the force that is keeping them separate (i.e., the magnetic force) is getting weaker, while the force that is pulling them together (i.e., the electric force) is still there. Eventually, the magnetic force won't be able to keep the opposite charges apart, and the voltage between them will affect charge recombination.
Sparky wrote:You've been listening to the magnetic reconnection magicians..

OK, here's where the terminology that I'm using, and that the MHD theorists are using, becomes dangerously similar, drawing the accusation...

I'm actually not sure that we're not talking about the same thing, but when they talk about magnetic reconnection, especially as an explosive force, they're talking pure gibberish. But both of us might be looking at the same thing...
Now, we have two parallel charge streams, that are generating opposite-polarity magnetic fields that have been keeping the charges separate, but which are now weakening. So the opposite charges begin to curve inward toward each other. Interestingly, if all of the above is correct, the magnetic fields will actually help the charges curve inward. If the charges can curve inward such that they meet head-on, the opposite-polarity magnetic fields will no longer repel. Opposite charges traveling in
opposite directions generate the SAME magnetic field.
Figure 5. Fast-moving electric charges can recombine if they form a loop.
So these opposite-polarity magnetic fields get book-matched back together as the charge streams curve inward and meet head-on. So perhaps this is what MHD calls magnetic reconnection, but that's fiction. I'm saying that it's electric reconnection, and that the magnetic fields simply figure out a way to stop fighting each other, and with explosive results --
due to the electric force.
Sparky wrote:you can not violate the laws governing electricity and invent scenarios which just can't happen...not in this dimension. We may have to move this thread to another, more tolerant one.

Please let me know if I have goofed somewhere in here. The whole construct is purely hypothetical, but I don't
think that I'm violating any laws.

(But officer, I didn't see the freaking sign -- now what do you want from me...football tickets?)
So the whole point of this exercise is that now I have a construct (legally or otherwise

) that establishes a vigorous charge separation and recombination mechanism, and that will create loops in the photosphere and chromosphere that look exactly like what actually happens. I'm still working on a variant of this construct that explains photospheric "tufting".
Lloyd wrote:Charles, you seem to make some good points, so I'm trying to elicit some comprehensive answers from our experts. But I don't know if they'll have time soon to provide them.
No worries -- if they took the time to smack down epiphanists like me, they'd never get anything done.

But I'd love to hear what they might have to say. Perhaps if this line of reasoning matures a bit, it would be worthy of a critical response. Right now, it's just some new ideas.
Lloyd wrote:I'm not greatly familiar with electric or plasma phenomena, so I don't understand a number of things being discussed in this thread. Can you explain the difference between an "imploding discharge channel" and active current z-pinches?
Let's consider what happens in a lightning bolt here on Earth. There is an electrostatic potential between the cloud and the ground. Electrons start moving in response to that potential. Due to the magnetic pinch effect, the flow of electrons gets consolidated into discrete channels. The consolidated electron avalanche heats the air. Interestingly, hotter air is a better conductor, so it allows the passage of more current. Soon, the air is excited to a glow discharge, and ultimately, to a full-scale arc discharge, where the increased charge density and greatly increased particle speeds generate a z-pinch that tightens the current into a channel less the 5 cm wide, with a temperature of roughly 2500 degrees Celsius. But this is nothing compared to the heat that will be created next. As soon as the electrostatic potential is released, the current stops. Now there's this 5 cm wide column of superheated air that no longer has a reason to be superheated. In the presence of the surrounding atmospheric pressure, the near-perfect vacuum inside the obsolete discharge channel collapses. The air actually fills the vacuum moving at the speed of sound, so it's actually an imploding shock wave. When that shock wave meets at the centerline of the channel, the temperature shoots up to roughly 25,000 degrees Celsius. This is what actually creates thunder, and is the source of the X-ray emissions from lightning.
So, if a 5 cm wide imploding shock wave can generate 25,000 degrees Celsius, then a 500 cm wide channel (too big for a lightning strike on Earth, but still theoretically possible) will generate temperatures in the range of 2,500,000 degrees Celsius. And that's hot enough for nuclear fusion. Now what would a discharge channel on the surface of the Sun, 500
km wide, do? Better put in your ear plugs!
Lloyd wrote:CharlesChandler wrote:But I disagree that galactic currents offer an accurate description of the Sun. The form of the energy release doesn't make sense if it's an exchange between the Sun and its external environment. That's why I'm looking at forces within the Sun.
I don't know if you've already explained that, but what "form of the energy release" from the Sun's environment to the Sun would you expect to observe?
I'd expect tightly-pinched currents, like lightning bolts, perhaps radiating outward into glow discharges as the voltage drops off away from the Sun. In other words, I'd expect sorta like a frayed cotton-ball effect. The corona IS filamented, but the filaments are going in the wrong direction, as if the matter is being ejected from the Sun, and is getting pinched into filaments as it heads off. Yet the EU model has the Sun positively-charged, so we would expect electrons to be streaming in, and to pinch down into arc discharges on connection with the Sun. The might be an extremely naive set of assumptions, but I haven't heard the specific reasons why a current capable of lighting up the Sun wouldn't behave like that. And don't just tell me that plasma is good like that.
