rolandk
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Has anyone a derivation at hand of the Christoffel symbol by permuting of indices in a free fall system?
Roland
Roland
The discussion centers on the derivation of the Christoffel symbols in the context of geodesic motion, specifically within a free-fall system. Roland highlights the geodesic deviation equation, which relates the second derivative of the geodesic to the Christoffel symbols, as outlined in "Gravitation" by Misner, Thorne, and Wheeler (MTW). The specific example provided shows that for the equation \(\ddot{\theta} - \sin(\theta) \cos(\theta) (\dot{\phi})^2 = 0\), the Christoffel symbol \(\Gamma^{\theta}{}_{\phi \phi} = -\sin(\theta) \cos(\theta)\) is derived, while other symbols are zero. The conversation also touches on the definitions of Christoffel symbols as presented in various texts, including works by Dirac and Ramond.
PREREQUISITESStudents and researchers in theoretical physics, particularly those focusing on general relativity and differential geometry, will benefit from this discussion.
Yup. See - http://www.geocities.com/physics_world/ma/chris_sym.htmrolandk said:Has anyone a derivation at hand of the Christoffel symbol by permuting of indices in a free fall system?
Roland
What's with the atttitude dude?? I don't delete portions of my web pages due to the comment of a readed who is a bit ignorant on the subject. As for "giving it" to you, I wasn't. I was giving it to Roland.dextercioby said:Well,Pete,either u or Dirac[1] have it all mixed up.I'd go for you,as Dirac got a Nobel prize and I've been taught GR from his book[1].
Your formula #2 is valid for contravariant vectors ([1],eq.3.3,page 6) (a.k.a.vector,which is defined on the tangent bundle to a flat/curved \mathbb{M}_{4})...So how about getting it all done correctly or,don't give that link anymore and exlude it from your post.
Daniel.
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[1]P.A.M.Dirac,"General Relativity",1975.
So why bother with me? Seems that you're unwilling to entertain the possibility that you made an error. In any case Eq. #2 in my page is the transformation properties of the components of a contravariant vector.dextercioby said:Alright,u didn't get it..
There is a minor point I'd like to make to add to those of mine above. There are four symbols in tensor analysis which are tightly related. In certain circumstances they are identical. In most circumstances you'll see in GR they are identical. Two of the symbols are referred to as the Christoffel symbols (of the first and second kind) and the affine connection symbols (of the first and second kind). The affine connection has a capital gamma as a kernal lettter. There is also two terms referred to as "affine geometry" and "metric geometry.rolandk said:Has anyone a derivation at hand of the Christoffel symbol by permuting of indices in a free fall system?
Roland