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Re: capacitance of a disk



At 16:41 2/8/01 -0500, Carl Mungan wrote:
...start with two concentric spheres, work out the capacitance,
then let the radius of the outer sphere go to infinity to get the
capacitance of an isolated sphere.

If you try the same thing for a parallel-plate capacitor C = A*e0/d
and let d go to infinity, you get zero which is obviously wrong. I
assume this is because we neglected the fringing field, which is only
valid if d << sqrt(A).

So what is the capacitance of an isolated disk? ...

Carl E. Mungan

Assume that the expression I mentioned earlier for the capacitance
of concentric spheres has been experimentally verified to
the accuracy given,
i.e Capacitance = R1R2/(R1+R2) 111.27 pF/m
for
R1 radius of inner sphere meters
R2 radius of outer sphere meters

As R2 grows very large, its capacitance tends towards
R1 111.27 pF/m

As R2 grows very large, the influence of asperities
on the inner shape declines,
so that its projected area dominates the expression.

In terms of its area, the capacitance of a sphere is
4 pi R1^2 m^2 := R1 111.27 pF/m

The area of a disk of radius R is given by
2 pi R^2 + 2 pi R t = 2 pi R (R + t)
(t thickness in meters)

Where R2 is very large, its capacitance is in the ratio

(2 pi R)(R + t)/(4 pi R1^2)
to that of the sphere.

So the capacitance of the isolated disk is

(R + t)/2R1 R1 111.27 pF/m = (R + t) 55.64 pF/m


(This is a plausibility argument, one step better
I'm sure you will agree, than demonstration by
loud assertion, and two steps better than proof
by arm-waving...)


brian whatcott <inet@intellisys.net> Altus OK
Eureka!