Self-study doesn't always work, as
michaelsuede and
Michael Mozina have demonstrated in this thread.
Um, I'm the one that has read Alfven's books and papers, whereas you have not. That's essentially the primary difference between us, AKA "education".
Michael Mozina has been telling us that Alfvén's books and papers say absolutely nothing about magnetic reconnection. Here, however, he claims to have educated himself about magnetic reconnection by reading Alfvén's books and papers. That's a nonsensical argument.
I am not a physicist. Most of what little I know about physics is derived from self study.
I do, however, have enough formal education in math and physics to understand the most basic facts about magnetic reconnection. If that's what mike3 means by "this stuff", then freshman-level knowledge of vector calculus and electricity and magnetism would put you far ahead of Michael Mozina.
Nope. Been there, done that more than thirty years ago.
Why, then, is
Michael Mozina unable to compute the curl of a vector field?
Show me one (published) that satisfied Alfven's criteria. You've still never copped to the fact that Alfven wrote *ZERO* papers on the topic of magnetic reconnection theory, and HUNDREDS of papers on "circuits/DLs" in plasma.
As
I have stated elsewhere, magnetic reconnection can occur in the absence of plasmas.
Michael Mozina has said he would "
*LOVE* to see a "physical demonstration" of that, yet he refuses to look at a physical demonstration.
michaelsuede and
Michael Mozina are the ones who have been confusing themselves by dragging plasma into the picture before they understand even the basic facts about magnetic reconnection.
The knowledgeable people here generally attempt to explain magnetic reconnection without speaking of plasma. For example...
Let's skip the bluffing and go straight to the "tells".
Pick a unique point in space. Measure the B field direction. Take a differential step in that direction. Measure the B field direction, take another step. Etc. That traces out a line. This is the definition of a magnetic field line, it's perfectly clear, it ignores E fields by definition.
...snip...
The line "crossing" happens at saddle points, i.e. at places where B=0, where it is perfectly reasonable, indeed necessary, for lines to meet. It does not require a monopole or any Maxwell's Equation violation. Examples are trivial to construct: quadrupole fields like {Bx,By} = {y, x} have "crossing" lines.
From that field to magnetic reconnection is but a short step, yet
michaelsuede and
Michael Mozina refuse to see the connection:
Throwing out a list of random stuff that has nothing to do with the topic does nothing to diminish the points made in my article.
Ziggurat took that short step by giving this simple example of magnetic reconnection:
Indeed. In fact, we can produce reconnection with only a slight modification. If you use the field
{Bx,By} = {b*y, a*x}
then when you change the ratio a/b, you will reconnect points, as shown below:
[qimg]http://www.internationalskeptics.com/forums/imagehosting/1192499b6711ad5d6.gif[/qimg]
So the math clearly works. One may dislike the terminology all one wants to, but that's irrelevant. The term is well-defined, and actual magnetic fields which satisfy Maxwell's equations (you can check) fit the description.
michaelsuede couldn't follow
Ziggurat's explanation because he knew nothing about the vector fields he had been blathering about:
What is wrong with this B-field, Michael?
{Bx,By} = {b*y, a*x}
And why don't you illustrate for us that you understand freshman-level electrodynamics by computing its curl and divergence. If you cannot do that in your head or in a few seconds on paper, you have no business whatsoever discussing this topic.
Can you do that?
Then
Michael Mozina entered the fray. He can't compute a divergence or curl either, so he ignored all of the above.
Show me an experiment in a vacuum that is devoid of plasma entirely where "magnetic reconnection' happens. Then and only then can you tell me it's not the particles in the plasma and circuits doing the "reconnecting".
The
experiment I suggested can be set up around a vacuum chamber that's devoid of plasma. Although the vacuum chamber will make the measurements a lot less convenient, the magnetic reconnection happens just the same in the vacuum as in air. Since the vacuum is devoid of particles, plasmas, or circuits, the experiment I suggested refutes
Michael Mozina's claim. Decisively.
No wonder
Michael Mozina has ignored that experiment.
It fails to explain what is physically unique and different about magnetic reconnection that can be isolated and shown to be unique and different from ordinary particle collisions inside current carrying plasma, and "induction" which already has a proper scientific term. The fact the circuit topology changes over time is not evidence that "magnetic fields' did the actual reconnecting. It's the "current" that is simply being "redirected', it's not the magnetic lines that "reconnect". They just follow the current.
That's ignorant nonsense.
In the
experiment I suggested, there are no "ordinary particle collisions inside current carrying plasma", the "circuit topology" does not change over time, and the magnetic lines do not "just follow the current."
As I wrote on 28 March:

This thread is about denials of magnetic reconnection by people who (a) turn out not to understand the freshman-level math and physics they claim to be using as the basis for their arguments, and (b) refuse to read scientific papers that report experimental observations of magnetic reconnection.
You'll fit right in.
Several months ago, I described a simple experiment and suggested you conduct it in your own lab. That experiment can be conducted in a vacuum without changing its results in any way, although the vacuum will make the experiment somewhat more awkward. I suggest you perform the experiment in open air before duplicating it in vacuo.
Your refusal to do lab work does not make you an authority on the subject any more than your refusal to read the relevant literature or to learn the relevant math make you an authority on the subject.