On Sun, 3 Jun 2007, Michel Jullian wrote:

> Only they are not filamentary in the monopolar drift area (most of their
> path),

Says who?

I hope you're not suggesting that, since theory predicts that they spread
around, therefore they DO spread around, and no experimental verification
is needed?

> they spread around more or less evenly because they repell each other.

Again: who as OBSERVED that they spread around as you say?

My personal observations of actual ion flows shows that filament-shaped
flows are common when potentials are below a certain high threshold.

  Threadlike streams of Electric Wind
  http://amasci.com/weird/unusual/airthred.html

I initially found this very confusing, since self-repelling particles
should fly outwards in all directions.  How are these filament-shaped
flows even possible?

I know of two effects which could lead to narrow flows.  First, when
material is
forced to flow through a fluid environment, sometimes the flow pattern of
individual particles is not stable, and narrow jets spontaneously arise.
Example: a descending cloud of volcanic particles sometimes forms a narrow
ground-hugging sheet which flows at immense velocity.  This is the origin
of pyroclastic surges.  Or more common: a descending group of rain drops
moves together and flows faster than individual drops otherwise would
fall, forming a "rain shaft."  And rising hot air from a cigarette will
become a very narrow vertical jet.  In these cases the group of moving
particles is dragging the air along with them, so the individual particles
experience reduced air friction, and a self-organized flow structure with
a particular diameter is created.

Of course where charged particles are concerned, these "jet forming"
forces would have to dominate over the particles' self-repulsion.
If ion density was too high, the narrow jets would not appear.




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