Yes, I understand that.

It's a question of HOW MUCH current flow, and how HIGHLY ionized the plasma then becomes due to that current flow. The whole definition of an electrical discharge BEGINS in a plasma.
No apparently you do not understand as we can see of the next comment of yours.
Then please give the
full definition of discharge that you are going to use from now on. Because in my view the plasma is a product of a discharge not the start.
Ya, but we are not discussing discharges through a GAS, now are we? Some "greater" concentration of "current flow' is going to be required in order to explain multi-million degree plasmas anywhere near an "opaque" 6K surface.
No, we are talking about a current through a plasma, where there is no (Peratt's comment) break down of the medium. Just more ionization does not make a break down of the medium, that happens when it goes from non-conducting neutral to conducting ionized.
The heating part is discussed by me.
Great. We are in total agreement on that point. It's all a function of the pinch and current flowing through the pinched filament.
There is no need to go and discuss pinches here. Also without pinches (look at those loops do they look pinched? I think not) will an increased current heat the plasma more.
No, I'm looking for *ANY* definition of an "electrical discharge" in a "plasma" (already ionized gasses) so we can discuss Dungey's paper, and get on with it. If you insist on deviating from a relatively 'standard" definition from the realm of plasma physics, well, I guess I'll have to live with it, so long as we can *MOVE ON* in the conversation.
No, I am on solid ground, no one at this time will define a discharge as Dungey did it approximately 40 years ago. And actually it is just a word, that has absolutely no influence on what Dungey presented. He says discharge and then also says what he means: a strong current in a plasma. That is
enough to discuss the Dungey paper. You have to use the definition
in context, I can read the paper with the stingent definition of discharge, and that will get me nowhere. So, start discussing Dungey's paper, but then please start with paper 1 on which the comment was written to which Dungey replied again. Otherwise the discussion is useless, because we don't know the starting point of the discussion.
I think it's utterly ridiculous you're arguing with a plasma physicist too, but then you reject Alfven's work too I suppose, or at least some of it. Even still, this is simply a "definition" of a discharge in a plasma. Unless one believe it's impossible to release EM energy into a plasma, it's must occur.
Well, I also disagreed with Duncan Bryant on the definition of a double layer and particle acceleration, so what. I do not reject Alfven, I do reject some of the things he claims because they have been shown to be incorrect (but that is not the point here). I think the definition is ridiculous, but for reading the Dungey paper I will have to accept that he calls a strong current through a plasma a discharge, otherwise I will not be able to understand what he is writing about. So from your comments I see you want to use the idea that a discharge is "a current in a plasma." I could live with that, if you would just have the balls to make a stand and say, I think it is this, which you will not do.
tusenfem said:
The Fe will be ionized in the Sun proper (otherwise it cannot rise with the magnetic field, because it would not stick, basic plasma physics thank you very much). It will have something like 5+ or so (humble estimate, not necessarily correct) and then through the heating of the plasma by the current be ionized further quite possibly to 20+.
But then fundamentally we are talking about the "intersection" of two "discharges" at the point of "reconnection". It's not simply a "magnetic" process, it's an *ELECTRO*magnetic reconnection process.
No we are not talking about an intersection of anything. I am talking about one loop, through which a current is driven and where further ionization takes place of the species that are present. There is nothing about reconnection going on here. I am just driving a current through a loop, point, nothing more, and have the plasma heated.
You need to chill out a bit. FYI, I'm typically responding to these posts between tech calls at work, I'm responding to LOTS of individuals and sometimes I do in fact misread things from time to time because (drum roll please) "I'm human".
So, you think I have nothing else to do? You don't think that I am working hard every day? Maybe you should discuss less topics at the same time. Maybe you should ignore most of the post and spend more time thinking about stuff and trying to find out if it has merit and actually do a real discussion of a paper. You want to be the amateur plasma astrophysicist, and thus you have to put some effort in it.
Ya, but we already know that "discharges" produce them. We know "discharges" occur around every large body in the solar system with an atmosphere and a magnetic field and the sun has both. Why do we need to go looking for anything particularly exotic when we already KNOW a "natural' source of such photons in our *OWN* atmosphere?
No doubt at the "base' of the loops where the "discharge" process heats plasma to millions of degrees.
Most of the X and gamma radiation is emitted by the footpoints, yes, where e.g. the electrons enter the Sun again and bremsstrahlung is emitted.
We don't know that discharges produce them, because we apparently don't know what a discharge is in this case. What I see there is a plasma filled magnetic tube that exits the Sun, and which through intial conditions and through footpoint shear, carries a current that gets increased in strength through an electromotive force. If the current gets too strong, i.e. if the drift velocity of the particles get greater than the thermal velocity an instability will start in the plasma (Buneman instability) and possible double layers can be created and we can get highly accelerated electrons and ions. So, that is all we need to know, we don't need to call this a discharge, it has no purpou
Peratt's definition of an electrical discharge in a plasma is clear, it's concise, and it's perfectly congruent with Dungey's use of the term. Why do we need to deny a perfectly good definition of a discharge in a plasma again? Oh ya, to protect *IGNORANCE* spewed by a couple of clueless individuals.
You and I seem to be able to communicate. Let's just focus on moving forward and I'll just ignore the ignorant for awhile, ok?
Alfven referred to these "pinched" filaments as "circuits", so what would be an appropriate term for two 'circuits" reconnecting and some change in topology between those two circuits?
Okay, then Peratt's
complete definition of a discharge
including the general break down of the medium. But then we will get into the discussoin of what break down is. (yet another ten pages or so)
Alfven called
everything a circuit, there need not be a pinch, forget about that because that is just making things more complicated.
Well, for one thing you cannot describe reconnection in such a way, because the currents do not follow the cables that Alfven is defining, i.e. they no longer flow along the magnetic field. Near the region where it gets interesting, i.e. near the X line in the ion diffusion region, the Hall currents flow perpendicular to the magnetic field. But be my guest, build up your circuit model and then show how it works and show how it explains the data that
Runov et al. (2003) measured with the 4 spacecraft Cluster mission. Now that's a starting point for discussions.