Where do you propose that one might build a 1000 km long plasma tube to contain the experiment?
I'm going to have to assume that I will never personally have access to that kind of funding or equipment, and I would think that is probably unnecessary for purposes of this particular point. The "best" laboratory tests I could find seem to be related to the optical test done at Los Alamos. Figuring out how to work their input screens looks to be rather "challenging" at first glance.
http://www.t4.lanl.gov/cgi-bin/opacity/tops.pl
How do you propose to conduct the experiment, if and when it is built?
It seems to me that enough physical tests have probably already been done to answer our question, but we'll have to make some "assumptions". I guarantee you that some light from my arc welder with penetrate at least a couple of feet of a thin hydrogen plasma. How much optical depth I might hope to achieve will be at least as dependent upon the amount of current I use in the arc welder, and therefore the amount of light I generate at the point of origin as the amount of plasma between me and the arc.
You constantly revert to an insistence on controlled laboratory experiments.
Why wouldn't you do that too? Aren't you busting me right here and now on that same issue, and isn't it a valid criticism?
But you yourself will reject even the most controlled of laboratory experiments, when they contradict your pre-conceptions, as you do with magnetic reconnection.
I don't actually "reject" them as you seem to think. At space.com I was handed a paper by someone named Birn, et all that I found to be 'acceptable' in terms of the math and physical explanations, but the term itself "magnetic reconnection" seemed to be it's single flaw. There was no "magnetic reconnection" going on, just particle reconnection at the point of intersection. It would have been equally valid to call this process "particle reconnection" or "circuit reconnection", both of which are significantly more accurate and significantly more universal than the term "magnetic reconnection". No self respecting electrical engineer would use that term when describing electrical events in solids.
More importantly however I don't see how you determined "magnetic reconnection" occurred rather than a combination of particle interactions (as in any ordinary current sheet) and circuit rewiring, and/or a wee bit of induction. There seems to be no way to isolate "MR" from any of the other aforementioned items.
So why should anyone be impressed by your insistence that other people adhere to criteria that you will not adhere to yourself?
You should require of me what I will require of you and everyone else. In other words, there's no point in me playing the role of hypocrite Tim. We should all want to do this the "right way", from beginning to end. I would certainly agree that there is work to be done in this area.
And you fail to notice that some things cannot be demonstrated to your satisfaction in any conceivable controlled laboratory experiment.
What problem did Birkeland have in confirming most (ok, not all) aspects of his electrical discharge model? The moment he turned the sphere into a cathode, he was able to replicate the aurora with it, to generate discharges in the atmosphere, jets, solar wind, etc. Ok, sure, he didn't build a breeder reactor in his lab, but that's been done now too.
This is one example. Even a "thick" plasma, let alone a "thin" plasma, can be transparent or translucent under laboratory conditions,
Fine, but let's start with some basic logic and common sense. When we are talking about "optical depth", we mean "how far" will that light penetrate a plasma (not completely ionized by the way) before we can no longer see it. In other words, if the discharges originate below the surface of the photosphere, we will definitely see those loops before they reach the surface, if only a few kilometers. At this point we're arguing about "how far below" the surface of the photosphere that we might be able to see an electrical discharge of epic proportions. We might start by comparing the event to what we see here on Earth during an electrical storm. In other words, this light source is *POWERFUL* and as long as that current is flowing through the loop, we will certainly see it to some depth below the surface of the photosphere, assuming that the discharge occurs below the photosphere.
I hear you about the need to do some additional work Tim. I do. You also need you to recognize that there will be penetration of these high energy wavelengths to some optical depth. If these loops originate under the photosphere they will be visible below the surface of the photosphere to some specific depth determined by the density and absorption pattern of the plasma, the specific wavelength in question and the light intensity at it's point of origin.
while being opaque in nature because nature exists on spatial scales that cannot be duplicated in any laboratory.
Ya, and I can't get my arc welder to crank up to that current level either, so we'll have to do some scaling sooner or later. First we would need to agree on what material exists in a photosphere and how deep is the "photosphere". I tend to use the standard depth measurement personally, so the depth part seems to be a given, but the composition of that layer is going to result in an immediate argument.

How will you and I even agree on that much?
You must pay attention to the relevant physics, just as you demand of others to do the same, or you just wind up in a thread dominated by a sea of insults and minor conversations on unimportant points, as you are now.
Sure, I agree, but that works both ways. You and I both know that we can fire up an arc welder and demonstrate that we can see light to some depth through just about any type of plasma of the density you're assigning to the surface of the photosphere. Yes, I agree that after some specific depth (could be tens or hundreds or thousands of kilometers), we may not still be able to see a powerful discharge in some wavelengths. You will also have to accept that I am talking about extremely large discharge events, many times more powerful than the ones we observe here in our own atmosphere.
It's also much harder to calculate optical depth in a separated model than you make it sound by the way. The gas model and a plasma separated models are very different, starting with the whole concept of a separation of elements. Whereas you would attempt to calculate the optical depth of the photosphere based upon a "mixture" of various elements, I would have to calculate the opacity of various layers of the atmosphere separately, by the element, based upon the distance from the surface of the photosphere composed of NEON, another plasma layer below made of silicon, and layer of calcium plasma to boot. I have to know all the depths of these things of course and then I have to take into account the fact that that electrons and protons are flying out of the sun at a millions miles an hour, etc, etc, etc. It is a lot more complicated than you make it sound. It's a whole lot easier in a standard gas model because it begins (of course) with a gross oversimplification, namely the concept that all elements will stay mixed together due to convection in the outer layers. Unfortunately that "stratification subsurface" is sitting in the middle of what is suppose to be an open convection zone.
It seems to me Tim that we are arguing about a specific depth, not *IF* we might see through *SOME* amount of the photosphere. It still comes back to where the base of the loops begin.