The concept of a point charge is well known to have some problems.
Suppose we consider a point charge to be really a spherically
symmetric charge distribution of radius r equal to epsilon with
epsilon having the property that epsilon squared is greater than zero
and and any higher power of epsilon is equal to zero.
This would seem to describe a sphere that is not the boundary of a
ball since it encloses no volume.
Aside from the fact that this sounds weird, can anyone explain to me
what kind of difficulties this approach to the point charge problem
has that other approaches don't? Conversely, it does seem to address
at least the problem that a volume (or surface) integral containing
this object would yield a finite charge even though right at the
location of the charge the density would be infinite (since the volume
at the location of the charge is zero), or am I mistaken?
Thanks,
Armin
Arnold Neumaier - 15 Nov 2007 17:04 GMT
ANS schrieb:
> The concept of a point charge is well known to have some problems.
> Suppose we consider a point charge to be really a spherically
[quoted text clipped - 6 lines]
> what kind of difficulties this approach to the point charge problem
> has that other approaches don't?
You lose the property that your numbers form a field. This makes
almost all mathematical tools lose their force, or at least they must
be carefully reconsidered to see what still works. Working with such
infinitesimal numbers is called nonstandard analysis - all significant
results of interest for physics proved with nonstandard analysis
(such as the existence of solutions to the Boltzmann equation) have
been also proveed with normal analysis, and usually the latter
was more versatile.
Arnold Neumaier
maxwell - 15 Nov 2007 18:01 GMT
> The concept of a point charge is well known to have some problems.
> Suppose we consider a point charge to be really a spherically
[quoted text clipped - 14 lines]
>
> Armin
A point is a point. It is not a limit of something originally
finite. This is why the 'point' electron presents a challenge to EM
theory that is constructed totally around calculus with its notion of
limiting processes. The Dirac delta 'function' is not a function (or
'distribution') that has legitimacy in calculus: one of the major
ironies in Paul Dirac's life.