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- < [[General relativity]] General relativity is an extension to the idea of special relativity in order ...5 KB (803 words) - 19:56, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...1 KB (185 words) - 19:52, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...1 KB (220 words) - 00:28, 21 March 2007
- <[[General relativity]] [[Category:General relativity]] ...2 KB (327 words) - 04:25, 31 July 2007
- ( << Back to [[General relativity]]) ...3 KB (583 words) - 09:56, 17 November 2007
- < [[General relativity]] In General Relativity we write our (4-dimensional) coordinates as <math>(x^0,x^1,x^2,x^3)</math>. ...2 KB (361 words) - 19:52, 2 July 2006
- <[[General relativity]] ...r delta tensor, which is 1 whenever <math>i = j</math> and 0 otherwise. In general, instead of components <math>\delta_{ij}</math>, we have <math>g_{ij}</math ...2 KB (381 words) - 19:53, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...3 KB (581 words) - 02:26, 3 December 2007
- < [[General relativity]] vector. We can be more general and talk about tensors that turn a ...6 KB (1,173 words) - 09:22, 9 October 2007
- <[[General relativity]] [[Category:General relativity]] ...847 bytes (146 words) - 19:56, 2 July 2006
- < [[General relativity]] ...]] is a rank 1 tensor, and a [[scalar|scalar]] is rank 0. Tensors can, in general, have rank greater than 2, and often do. ...11 KB (1,814 words) - 00:17, 8 April 2007
- < [[General relativity]] As a final note, it should be mentioned that in General Relativity we will always have a special tensor called the "metric tensor" which will ...4 KB (727 words) - 19:56, 2 July 2006
- <[[General relativity]] ...r momentum|angular momentum]], and [[wikipedia:mass|mass]] <math>M</math>. General properties of such a black hole are described in the article [[wikipedia:ch ...2 KB (251 words) - 19:56, 2 July 2006
- [[Category:General relativity]] ...631 bytes (104 words) - 19:53, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...1 KB (254 words) - 19:54, 2 July 2006
- <[[General relativity]] In General Relativity we write our (4-dimensional) coordinates as <math>(x^0,x^1,x^2,x^3)</math>. ...2 KB (338 words) - 19:03, 29 March 2007
- <[[General relativity]] ..._{\mu\nu}</math> is a (symmetric 4 x 4) [[Wikipedia:metric tensor (general relativity)|metric tensor]] ...9 KB (1,329 words) - 03:05, 28 December 2006
- [[Category:General relativity]] ...342 bytes (54 words) - 02:40, 20 December 2006
Page text matches
- <[[General relativity]] ...r delta tensor, which is 1 whenever <math>i = j</math> and 0 otherwise. In general, instead of components <math>\delta_{ij}</math>, we have <math>g_{ij}</math ...2 KB (381 words) - 19:53, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...847 bytes (146 words) - 19:56, 2 July 2006
- <[[General relativity]] In General Relativity we write our (4-dimensional) coordinates as <math>(x^0,x^1,x^2,x^3)</math>. ...2 KB (338 words) - 19:03, 29 March 2007
- <[[General relativity]] [[Category:General relativity]] ...1 KB (185 words) - 19:52, 2 July 2006
- < [[General relativity]] In General Relativity we write our (4-dimensional) coordinates as <math>(x^0,x^1,x^2,x^3)</math>. ...2 KB (361 words) - 19:52, 2 July 2006
- [[Category:General relativity]] ...342 bytes (54 words) - 02:40, 20 December 2006
- <[[General relativity]] ...r momentum|angular momentum]], and [[wikipedia:mass|mass]] <math>M</math>. General properties of such a black hole are described in the article [[wikipedia:ch ...2 KB (251 words) - 19:56, 2 July 2006
- <[[General relativity]] [[Category:General relativity]] ...1 KB (220 words) - 00:28, 21 March 2007
- ...slight modications apply to quantum mechanics, electrodynamics and general relativity - in other words to all of physics. ...f a system with constraints. We can formulate electrodynamics and general relativity with the principle, and it also provides a powerful (but not so easy) route ...2 KB (279 words) - 19:12, 28 August 2006
- <[[General relativity]] [[Category:General relativity]] ...1 KB (254 words) - 19:54, 2 July 2006
- < [[General relativity]] General relativity is an extension to the idea of special relativity in order ...5 KB (803 words) - 19:56, 2 July 2006
- By comparison of these equations with the general expression for force in gauge theory, we find that the electromagnetic forc == Relativity == ...5 KB (929 words) - 03:52, 10 July 2007
- <[[General relativity]] [[Category:General relativity]] ...2 KB (327 words) - 04:25, 31 July 2007
- < [[General relativity]] vector. We can be more general and talk about tensors that turn a ...6 KB (1,173 words) - 09:22, 9 October 2007
- [[Category:General relativity]] ...631 bytes (104 words) - 19:53, 2 July 2006
- < [[General relativity]] As a final note, it should be mentioned that in General Relativity we will always have a special tensor called the "metric tensor" which will ...4 KB (727 words) - 19:56, 2 July 2006
- <[[General relativity]] ..._{\mu\nu}</math> is a (symmetric 4 x 4) [[Wikipedia:metric tensor (general relativity)|metric tensor]] ...9 KB (1,329 words) - 03:05, 28 December 2006
- ## One easy way to find this is by symmetry. In general (esp. if the final height is not the same as the initial height), we can us # This problem uses what is called [[Wikipedia:Galilean relativity|Galilean relativity]]. Arithmatics used here are approximately correct only at speeds much less ...3 KB (498 words) - 05:21, 25 December 2007
- ...a consequence of [[Albert Einstein]]'s [[theory of relativity|theories of relativity]] and [[classical theories of gravitation|related theories]] under which a ...r time]] at different positions as described by a [[metric tensor (general relativity)|metric tensor]] of [[spacetime]]. The existence of gravitational time dil ...9 KB (1,389 words) - 12:43, 31 December 2006
- <[[General relativity]] [[Category:General relativity]] ...3 KB (581 words) - 02:26, 3 December 2007