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Article #5796Re: Fermat's principle and curved spacetime
From: Koobee Wublee
Date: Sun, 20 Jan 2008 04:34
Date: Sun, 20 Jan 2008 04:34
77 lines
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4057 bytes
On Jan 19, 5:46 am, Dieter Heidorn wrote: > Koobee Wublee schrieb: > > The equation is correct for gravitational redshift. <shrug> > > Of course, because Einstein derived the c-equation in his 1911 work from > the correct equation for gravitational red-shift. The sequence of his > steps was: > > equivalence principle > > --> red-shift: nu_1 = nu_2 (1 + V/c^2) > > --> varying speed of light: c = c_0 (1 + V/c^2) > > --> deflection angle for bending of light: alpha = 2 GM / (c^2 R) Einstein did not derive anything. In this case, he merely stated them. <shrug> There are at least two ways to state what the speed of light is as a gradient. ** c = c_0 (1 - U) ** c = c_0 / (1 + U) Where ** U = G M / c^2 / r Both cases are the same if (1 >> U). However, at the extreme boundaries, they are drastically different. > > This equation will lead to a wrong value of the gravitational > > redshift. This is another example where GR is contradictory of itself > > because it does not agree with the metric derivation as you have shown > > above. > > You can take this as contradiction only, if gravitational red-shift > would depend on a variable speed of light. In fact this is not correct > in GR. Gravitational red-shift depends on the metric, so I wrote a few > lines above: > > The gravitiational red-shift depends on the metric: > > nu_B / nu_A = sqrt(g_00(r_A)/g_00(r_B)) > > In weak fields the following approximation holds: > > nu_B / nu_A = 1 + Delta V/c^2 In physics in general, we have C = nu lambda Where ** nu = frequency ** lambda = wavelength There is no way you can get away with the red-shift not dependent on the speed if the speed does indeed vary. Thus, I stand by my conclusion that the subject of gravitational redshift is one instance where this interpretation to the field equations is contradicting itself. <shrug> > You can find this in Einsteins 1916 work: > > Die Grundlage der allgemeinen Relativitätstheorie. > AdP 49, 769 (1916) > (§22, pp 818 - 820)http://www.physik.uni-augsburg.de/annalen/history/papers/1916_49_769-... > > (Sorry, but I don't know where to find an english translation of this work.) Sorry, ich lese nicht Deutsch.
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X-Google-Thread: 10f545,e60ad8b8bd890c74 X-Google-Thread: 10b271,4fd262761489fde X-Google-Thread: f74ae,4fd262761489fde X-Google-Thread: fa4c1,4fd262761489fde X-Google-Thread: 1139f8,4fd262761489fde X-Google-Attributes: gid10f545,gid10b271,gidf74ae,gidfa4c1,gid1139f8,public,usenet X-Google-Language: ENGLISH,ASCII Path: arc1-ca.pugleaf.net!g2news1.google.com!postnews.google.com!1g2000hsl.googlegroups.com!not-for-mail From: Koobee Wublee <koobee.wublee@gmail.com> Newsgroups: sci.physics.relativity, sci.physics, sci.astro, fr.sci.physique, fr.sci.maths Subject: Re: Fermat's principle and curved spacetime Date: Sat, 19 Jan 2008 20:34:08 -0800 (PST) Organization: http://groups.google.com Lines: 79 Message-ID: <a3fb1ad6-5537-4bc1-a0c3-c18a27fcad78@1g2000hsl.googlegroups.com> References: <acc87498-7d1a-4bf8-b205-e24b29b6f04b@s8g2000prg.googlegroups.com> <v2Wjj.38861$lD6.27743@newssvr27.news.prodigy.net> <f45cdd6a-6cba-49f6-aef9-089ac65e4d1b@k2g2000hse.googlegroups.com> <fmr47v$fqo$03$1@news.t-online.com> <3783ed0d-aae7-4f13-b98e-cfe1317f8846@i29g2000prf.googlegroups.com> <fmsv04$dkv$01$1@news.t-online.com> NNTP-Posting-Host: 69.229.111.174 Mime-Version: 1.0 Content-Type: text/plain; charset=ISO-8859-1 Content-Transfer-Encoding: quoted-printable X-Trace: posting.google.com 1200803648 11141 127.0.0.1 (20 Jan 2008 04:34:08 GMT) X-Complaints-To: groups-abuse@google.com NNTP-Posting-Date: Sun, 20 Jan 2008 04:34:08 +0000 (UTC) Complaints-To: groups-abuse@google.com Injection-Info: 1g2000hsl.googlegroups.com; posting-host=69.229.111.174; posting-account=PTS84AoAAACr67p51zvy0Hlr3LkoIUcc User-Agent: G2/1.0 X-HTTP-UserAgent: Mozilla/4.0 (compatible; MSIE 6.0; Windows NT 5.1; SV1; InfoPath.1),gzip(gfe),gzip(gfe)