Geodesic Deviation Equation Solved

unscientific
Messages
1,728
Reaction score
13
Taken from my lecturer's notes on GR:

GR9.png


I'm trying to understand what goes on from 2nd to 3rd line:

N^\beta \nabla_\beta (T^\mu \nabla_\mu T^\alpha) - N^\beta \nabla_\beta T^\mu \nabla_\mu T^\alpha = -T^\beta \nabla_\beta N^\mu \nabla_\mu T^\alpha

Using commutator relation ## T^v \nabla_v N^\alpha = N^v\nabla_v T^\alpha ## we swap the 'N' for the 'T' in the last term of the second line:

N^\beta \nabla_\beta (T^\mu \nabla_\mu T^\alpha) - T^\beta \nabla_\beta N^\mu \nabla_\mu T^\alpha = -T^\beta \nabla_\beta N^\mu \nabla_\mu T^\alpha

N^\beta \nabla_\beta \left(\frac{D T^\alpha}{D\lambda}\right) - T^\beta \nabla_\beta N^\mu \nabla_\mu T^\alpha = -T^\beta \nabla_\beta N^\mu \nabla_\mu T^\alphaThis means that ## \nabla_\beta \left(\frac{D T^\alpha}{D\lambda}\right) = 0 ##. Why is this so?
 
Physics news on Phys.org
May I ask what is T and N?
Nevertheless, it looks like the thing you have in the parenthesis (T^a \nabla_a T^b) should be the geodesic equation?
 
Use the product rule on the second term of the second line.
 
George Jones said:
Use the product rule on the second term of the second line.

That would just take me back to the first line.
 
ChrisVer said:
May I ask what is T and N?
Nevertheless, it looks like the thing you have in the parenthesis (T^a \nabla_a T^b) should be the geodesic equation?

##T## and ##N## are tangent vectors and normal vectors correspondingly, with ##T## describing movement along a geodesic and ##N## describing movement from one geodesic to another.

I thought the geodesic equation is ##\frac{d^2x^\beta}{d\tau^2} + \Gamma^\beta _{\mu v} \frac{d x^\mu}{d\tau} \frac{d x^v}{d\tau} ##?

I reduced the term in the brackets to ## \nabla_\beta \left(\frac{D T^\alpha}{D\lambda}\right) ##. I'm trying to understand why it is zero.
 
The geodesic equation by writting U^a = \frac{dx^a}{d \tau} (the velocity vector/ is it tangent to the trajectory??) can be written in the form : U^a D_a U^b=0 (that's why that expression even though I didn't know what it stands for reminded me of the geodesics equation)
 
  • Like
Likes unscientific
ChrisVer said:
The geodesic equation by writting U^a = \frac{dx^a}{d \tau} (the velocity vector/ is it tangent to the trajectory??) can be written in the form : U^a D_a U^b=0 (that's why that expression even though I didn't know what it stands for reminded me of the geodesics equation)

For a curve on space-time ##x^\alpha = x^\alpha (\lambda)##, we define the absolute derivative of a vector ##V^\mu## along that path to be expression ## \frac{D V^\mu}{D\lambda} = T^\alpha \nabla_\alpha V^\mu ##. For ##V^\mu = T^\mu##, we get ## \frac{D T^\mu}{D\lambda} = T^\alpha \nabla_\alpha T^\mu ##

If the vector ##T^\mu## is parallely transported along the path, ##\frac{D T^\mu}{D\lambda} =0 ##. This is obviously true for the tangent vector ##T^\alpha## ,so ##\frac{D T^\alpha}{D\lambda} =0 ##

Using ## T^\alpha = \frac{dx^\alpha}{d\lambda} ## and expanding, it simply gives the geodesic equation:

\frac{d^2 x^\alpha}{d \lambda^2} + \Gamma^{\alpha}_{\mu v} \frac{dx^\mu}{d\lambda} \frac{dx^v}{d\lambda} = 0
 
Last edited:
unscientific said:
That would just take me back to the first line.

Oops, I misread your first post.
 
Back
Top