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Article #883Re: An easy problem in general relativity
From: Mcinnes B T (Dr)
Date: Sat, 08 Aug 1992 01:07
Date: Sat, 08 Aug 1992 01:07
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1879 bytes
OK, now that I have your attention: let me be more precise. Certainly there is a parameter in the S solution which tells you what the mass of this thing would be, calculated a la Kepler, if it were a Newtonian source...which it isn't. For certain purposes this is no doubt useful. But I am thinking of mass as a measure of "quantity of matter". So let me ask again: How much matter is there in the whatever-it-is that the Schwarzschild solution describes? [People have objected, quite rightly, to my use of the word "object"...another piece of bait, I must confess.] After all, there must be some matter there, right? I mean, "matter tells spacetime how to curve", right? And so there must be some matter there, "causing" spacetime to curve, otherwise it would not know how to curve...right? All right, to quit fooling, what I am driving at is this: The amount of matter in this spacetime is zero. Exactly zero. There is no matter "in the singularity", because this statement does not make sense. It's not that I am averse to delta functions etc: by all means, tell me that a Newtonian point source can be represented by a delta function, so that the point source has a non-zero mass. Just don't tell me that this situation is in any way comparable to the S solution. I ask because I am trying to understand why people consider the presence [actually, absence!] of singularities in classical GR to be some kind of blemish on the theory.
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Newsgroups: sci.physics Path: arc1-ca.pugleaf.net!sparky!uunet!wupost!usc!cs.utexas.edu!qt.cs.utexas.edu!yale.edu!jvnc.net!nuscc!matmcinn From: matmcinn@nuscc.nus.sg (Mcinnes B T (Dr)) Subject: Re: An easy problem in general relativity Message-ID: <1992Aug8.010716.16818@nuscc.nus.sg> Organization: National University of Singapore References: <1992Aug7.161604.21263@galois.mit.edu> Date: Sat, 8 Aug 1992 01:07:16 GMT Lines: 22