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| Tags: black, hole, picture, singularity |
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On Apr 2, 2006, at 7:55 PM, Jack Sarfatti wrote: Not only that Paul, but the singularities future and past are not TINY POINTS in space, they are INFINITE 3D SPACES AT r*(r = 0) = 0. We slice into 3 + 1 relative to r*, i.e. dr* = 0 on each slice, and this is an INFINITE SPACE INSIDE THE FINITE EVENT HORIZON OF TOTAL AREA 4pi(2M)^2 from the HUGE SPACE WARP OF THE SINGULARITIES! YOUR MIND PICTURE IS COMPLETELY WRONG. YOU ARE THINKING OF A POINT SINGULARITY. THE WHOLE 3D SPACE (t,theta,phi) is singular as r* -- 0 where also r --- 0. Your Euclidean intuition is completely wrong here! Maybe that's Abram's error. It is certainly Puthoff's in his PV SSS exponential metric down to r -- 0. Remember spatial infinity is made finite in Penrose's projection. Everything is warped like an Escher picture. pastedGraphic.tiff I & III are outside the 2 event horizon mouths in different parallel universes of the Einstein-Rosen bridge i.e. r 2M IV is inside the horizon with the past spacelike singularity II is inside the horizon with the future spacelike singularity Both r* = 0 and r = 0 on both of those spacelike singularities that are INFINITE 3D SPACES where the 4th rank curvature tensor is infinite everywhere. r* is the interior time and t the interior radial coordinate. They REVERSE outside of r = 2M where r* = - infinity (non-rigorously). penrose.gif http://images.google.com/imgres?imgu...f%3D1%26sa%3DG On Apr 2, 2006, at 6:38 PM, Paul Zielinski wrote: Jack Sarfatti wrote: On Apr 2, 2006, at 5:38 PM, Paul Zielinski wrote: OK, I guess I should have taken the trouble to do the algebra. You mean you didn't? You wasted everyone's time with this nonsense! Only one or two e-mails. Jack, you haven't proved that Abrams was wrong about the arguments used by Kruskal-Fronsdal. You have simply offered a counterexample that if valid shows that one need not rely on a Hilbert-type error in order to get an event horizon with an interior. So if this is the only substitution that De Witt uses, it would seem that his treatment does not rely on the error allegedly made by Hilbert. EXACTLY! OK. in 1917 with his r - r*^2 = C(r). If, as you say, all De Witt needs in order to establish the existence of a coordinate-independent Penrose- type event horizon at r = 2GM/c^2 is this substitution. Of course, Abrams' argument was that the Kruskal-Szekeres-Fronsdal extensions relied on Hilbert's error, which they may well have done, notwithstanding De Witt's and other contemporary approaches to solution of the SSS problem.. My question now is, how does De Witt's model relate to those extensions? Is De Witt's manifold the same as the original extended Hilbert manifold? Or is it something different? WHO CARES? Well, I'm curious. THAT'S IRRELEVANT! DEWITT HAS THE FINKELSTEIN-KRUSKAL MAX ANALYTIC EXTENSION USING ONLY r* = r + 2Mln|r/2M - 1| and a previous case of Rindler space related to Minkowski space for 1 + 1 space-time. |
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