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Let's be more precise in use of "informal language" in gravity theory.

Science, order, and creativity - Google Books Result

books.google.com/books?isbn=0415171822...

David Bohm, F. David Peat - 2000 - Philosophy - 316 pages

Weyl's story shows the enormous power of informal language, which forms a significant part of the tacit infrastructure of science. ...

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Niels Bohr: Reflections on Subject and Object - Google Books Result

books.google.com/books?isbn=1930832001...

Paul McEvoy - 2001 - Philosophy - 540 pages

He then asked Bohm in essence what was special about the Aharonov-Bohm effect. Bohmreplied that it is a contribution to clarifying the informal language that ...

History of Twentieth-Century Philosophy of Science Book 7

www.philsci.com/book7-4.htm - Cached

He later refers to such supplementary description as informal language. Bohm's conclusion that mathematical physics must be supplemented with informal ...

Subject: Re: nonlocalizability of the gravity energy

Zielinski wrote:

I replied: No, free massive test objects move along timelike geodesics (inside local light cone) of curved space-time. Locally only inside the small LIF they appear to move on Minkowski geodesics (in segments small compared to radii of curvature).

Z:

I replied: Formally, in the tetrad formalism. The gravity field (meaning #3) is the motion of an LIF described by a SO1,3 Lorentz group 4-vector e^I, I = 0 (timelike), 1,2,3 (spacelike) of Cartan 1-forms each of which is GCT scalar invariant!

e^I is a SPIN 1 gravity field (meaning #3)

Einstein's SPIN 2 gravity curvature field (meaning #2)

ds^2 = e^IeI = (Minkowski)IJe^Ie^J = guv(LNIF)e^u(LNIF)e^v(LNIF)

however, adding Lorentz group SPINS

1 + 1 = 0, 1, 2

i.e. in terms of dimensions of the finite irreducible representations (2S + 1)

3x3 = 1 + 3 + 5

so what happened to spin 0 Brans gravity and repulsive spin 1 anti-gravity?

Higgs mechanism gives them large mass. Are they part of the nuclear force?

In sense of renormalization group running of the coupling constant ---> Salam's strong short-range Yukawa gravity?

You can actually show that free test objects move along geodesics in GR. A Minkowski manifold is just a special case.

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I don't get Jim's point

Category: MyBlog

Written by Jack Sarfatti

Published on Monday, 29 August 2011 15:40

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