On Wed, 8 Dec 2004 01:00:48 -0900, you wrote:

>At 5:41 PM 12/7/4, John Fields wrote:
>[snip]
>>
>>>The real beauty of your idea (is it original?)
>>
>>---
>>As far as I know, it is.  The lightbulb going off was due to something
>>of Fred Sparber's or Frank Znidarsik's (sp?) that I read a few years
>>ago on vortex,  and since then I've been looking but haven't been able
>>to find anything quite like it.  A month or so ago I talked to Hal
>>Puthoff about it and he also thought it was novel, so maybe it is.
>
>You may want to check out the thread: "Qball: Electrostatic Sphere Field
>Evaluator". A sample post late in the thread follows below.  I wrote (and
>posted) a basic program to integrate the effects of a spherical
>distribution of charge, and sample data.  We learned a few things from the
>exercise if you recall...

---
Yes.  I particularly liked the following paragraph, and especially
liked the sentence following it:

"
>>Now let's attempt to look at your initial problem of the bubble universe
>>and an infinitely dense surrounding.  The confinement force is now an
>>expansion force, due to gravity being attractive, but all else is really
>>the same, except for dealing with the infinite nature of the infinitely
>>dense volume outside the bubble. To begin this we can examine a single
>>shell, but only a finite portion of mass m in the shell, uniformly
>>distributed.  This gives us a finite mass density in the shell.  Such a
>>shell has zero force inside it, as we saw earier.  We can now sum
>>(integrate) an infinite number of such shells, all of the same fixed
>>radius, each having mass m, so that the total mass in the resulting shell
>>is infinite.  Since the force of each shell everywhere is zero, the same
>>is true of the final infinite sum.  We can then sum (integrate) the shells
>>at every radius r, with r-> inf. Since the force inside every shell is
>>everywhere zero, this must be true inthe final sum.  There is thus no
>>force of gravity exerted by the external volume on the universe.
>>
>>Of ourse one tiny change in density out in that infinitely dense volume ...
"
---
 :-)


-- 
John Fields


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