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Re: IONS/metal pedagogy



This is a re-post; the original seems to have died somewhere!
*******************************
Hi Brian,
I apologize - my statement was hurried and vague - but of serious import.
I was referring to a line of reasoning which I earlier outlined: the
standard classical line of reasoning (hinging largely on Gauss' law) says
that a conductor (charged or neutral - in an external field or not) is
under a force of tension wherever there is a surface charge. The net
electrostatic force per unit area (DUE TO THE REST OF THE CONDUCTOR AND
THE REST OF THE UNIVERSE) = (1/2) sigma^2 /epsilon - always an outward
force. This (says the classical model) is the net electrostatic force
due to the universe, per unit area of charged conductor surface. IE; the
NET ELECTROSTATIC FORCE is not zero - it is outward. If our scheme says
the conducting surface is in equilibrium under only electrostatic forces,
this (largely Gauss based conclusion) is in question. I really hope
something is wrong with my reasoning here, because it looks to me like
any classical model has to include some non-electrostatic force to
achieve equilibrium here (as we feel forced to do within the nucleus).
Please straighten me out!

Bob Sciamanda
Physics, Edinboro Univ of PA (ret)
trebor@velocity.net
http://www.velocity.net/~trebor

-----Original Message-----
From: Brian McInnes <bmcinnes@pnc.com.au>
To: phys-l@atlantis.uwf.edu <phys-l@atlantis.uwf.edu>
Date: Saturday, October 10, 1998 8:59 AM
Subject: Re: IONS/metal pedagogy


Hi Bob,

----------
You wrote
The problem is that this raises a perhaps much more
serious problem. If the excess charge on a conducting surface is in
equilibrium under only electrostatic forces, then Gauss' law is in
trouble. Again - what do we give up? Is not the internal field zero?
must not a negative surface charge terminate a field line from the
outside? Something of the classical model of a conductor and its
surface
must give. (And this might be the way to go!)


I am probably missing something but I can't see that Gauss' law is in
trouble.
As I suggested yesterday and Joseph covered in much more detail today
(times
are Australian) the surface charges can be in equilibrium under
electrostatic forces alone as a result of a (small) relocation of
electrons
in the metal.
The internal field will be zero. Agree, because a static situation has
been
set up.
There will be field lines terminating on the charges on the surface.
Agree,
because there will be a field outside the metal.
But why is Gauss' law in trouble? What am I missing?

Brian McInnes