- #1
jfy4
- 649
- 3
Mentz114 said:OK. Having done this for boosted frames, I guessed that the coframe would be of the form
[tex]
\vec{e_0}= a\ dt\ -\ e03\ dz ,\ \ \ \vec{e_1}= a\ dx,\ \ \ \vec{e_2}= a\ dy,\ \ \ \vec{e_3}= e33\ dz
[/tex]
where e03 and e33 are unknown. Working out the sum of the tensor products shown in my previous post gives
[tex]
\left[ \begin{array}{cccc}
-{a}^{2} & 0 & 0 & -a\ e03 \\
0 & {a}^{2} & 0 & 0 \\
0 & 0 & {a}^{2} & 0 \\
-a\ e03 & 0 & 0 & {e33}^{2}-{e03}^{2}
\end{array} \right]
[/tex]
and it's trivial to solve for e03 and e33 so this matrix is the required metric.
I've also done this with a frame basis where the target is the inverse metric.
Mentz was kind enough to give me this explanation for co-frame basis for a specific metric that I specified. However, I was wondering if there is a general procedure for finding the co-frame basis vectors for a general Einstein metric. I see the procedure involves the tensor product of the basis vectors with (maybe all?) unknown entries. I am not sure how to pick which parts of these basis-vectors would be unknowns, and which would be knowns. If someone could give me a nice run down that would be great.
Thanks,