Re: Electro-London Inertia
- From: "sue jahn" <suzysewnshow>
- Date: Sat, 22 Oct 2005 04:55:27 -0400
On Wed, 05 Oct 2005 15:54:38 -0400, Ken S. Tucker <dynamics@xxxxxxxxxxxx> wrote:
Sue... wrote:Ken S. Tucker wrote: > Sue... wrote: > ... > > Many thanks for the obeservation about the term 'force'. > > At some point, a poor choice between force, energy, acceleration > > or potential can hide the trees in the forest. The correct choice > > would show the clearest relation between mass, gravity and inertia > > yet be something a bit more formal than a professor riding in > > a lift. > > Sue... > > Hi Sue, Ken here... > > Your cuddling to the Electo-vacuum solution to the EFE's > (Einstein Field Equations), however in agreement with > your inclination, the solution departs from a continuum. > That is to say, the EFE's do require relations in the > way you are seeking.
The wiki URL you posted in another thread, inspired a bit of window shopping and I sort of like the way this outfit looks on induced dipoles:
I should have provided that ref to you, so you don't think I'm a TOTAL lunatic, but just partly loony:-). That wiki on GR is pretty good, the authors are trying hard, I follow the discussion.
<<Phenomena which can be modeled by null dust solutions include: a beam of massless neutrinos (treated according to classical physics), a very high-frequency electromagnetic wave, a beam of incoherent electromagnetic radiation. In particular, a plane wave of incoherent electromagnetic radiation is a linear superposition of plane waves, all moving in the same direction but having randomly chosen phases and frequencies. (Even though the Einstein field equation is nonlinear, a linear superposition of comoving plane waves is possible.) Here, each electromagnetic plane wave has a well defined frequency and phase, but the superposition does not. Individual electromagnetic plane waves are modeled by null electrovacuum solutions, while an incoherent mixture can be modeled by a null dust. >> http://en.wikipedia.org/wiki/Null_dust_solution
I don't read the shorthand well enough to know it that is what you are modeling below. I am not at all comfortable with the freewheeling interchange of E and B *outside the particle* but that may be valid way to derive forces from incoherent radiation. A null dust seems to be the best description of induced dipoles. Sue...
I think no one is satisfied yet. It seems GR is being treated as a extension of Newtons continuum theory,
The matter that fills the universe requires that we consider a continuum.
and of course that makes it's fusion with QT difficult because QT is a theory about relations,
The forces between charges requires that we consider the relation between the entities.
and not about points on a continuum. OTOH I see GR as naturally a relation theory, such as relating two simple charges "a" and "b" below.
So yes. You can't have biscuits with jam using all bread or all jam. :o)
Sue...
Regards Ken S. Tucker
> For example, take a pair of charges "a" and "b" and > they have some configurational energy, > > p = a*b/s, in ergs for example. > > Slap the behind (dividing by volume) and get the > energy density, > > T00= p/s^3 == a*b/s^4. > > Now, pause and ponder this, > > T00= (a/s^2)*(b/s^2) = E(a)*E(b) = a*b/s^4, > > where E(a) & E(b) are Electric fields of charge > "a" and some other charges. > > Sue, the above departs from the classical solution > to EFE's that uses a continum, but who cares, that's > pretty junky now. > > If you like that's Tuckers "noncontinuum solution to > the Electrovacuum EFE's", I mean that. > > Once T00 is defined that way, we can enjoy G00 by > > G_uv = T_uv , G00 = T00. > > OO scary equation, I'm shakin in my boots. > > Twist & shout, > > G00 = NABLA^2 g00 = T00. > > Solve for g00 and find, > > g00 = 1 + (a/s)(b/s), > > provided the charges don't masturbate, so terms > like self energization "a^2/s" are excluded > including a^2/s^4. > > Sue want's a solution using discrete charges > I figure we should give girls what they need. > > At this point we have a closed logic system > consistent with the EFE's and discrete, where > discrete means charge "a" is in a different > location than "b", and the metric is defined > by the relation. See, the continuum died. > > With Sues ableness to put things behind us, > we can proceed to observe the asymmetry of > the relative geodesics of charges "a" and > "b". > > I'll stop here, take questions, and if you > want, show how nonsymetrical metrics give > the EM field. > > Regards Sue > Ken S. Tucker
-- Using Opera's revolutionary e-mail client: http://www.opera.com/mail/ .
- Follow-Ups:
- Re: Electro-London Inertia
- From: Ken S. Tucker
- Re: Electro-London Inertia
- References:
- Re: Electro-London Inertia
- From: xxein
- Re: Electro-London Inertia
- From: Sue...
- Re: Electro-London Inertia
- From: Ken S. Tucker
- Re: Electro-London Inertia
- From: Sue...
- Re: Electro-London Inertia
- From: Ken S. Tucker
- Re: Electro-London Inertia
- Prev by Date: black hole question
- Next by Date: Re: Derivation of Lorentz Transformation (contd. from sci.physics.research)
- Previous by thread: Re: Electro-London Inertia
- Next by thread: Re: Electro-London Inertia
- Index(es):
Relevant Pages
|