Get Lorentzian Spherically Symmetric Metric to Sylvester Form

Click For Summary
SUMMARY

The discussion focuses on transforming a Lorentzian spherically symmetric spacetime metric into Sylvester normal form, which requires achieving a diagonal matrix with entries of 1 or -1. The transformation involves orthogonal diagonalization of the symmetric matrix using its eigenvectors, resulting in a diagonal matrix with one negative and the rest positive entries. Rescaling the coordinates is necessary to finalize the transformation. The Schwarzschild spacetime is provided as a specific example of this process.

PREREQUISITES
  • Understanding of Lorentzian geometry and metrics
  • Familiarity with orthogonal diagonalization of symmetric matrices
  • Knowledge of eigenvalues and eigenvectors
  • Basic concepts of coordinate transformations in general relativity
NEXT STEPS
  • Study the process of orthogonal diagonalization in linear algebra
  • Learn about the properties of Lorentzian metrics in general relativity
  • Investigate the Schwarzschild solution and its implications in spacetime geometry
  • Explore coordinate transformations and their effects on metric signatures
USEFUL FOR

Researchers, physicists, and students in theoretical physics, particularly those focusing on general relativity and spacetime geometry transformations.

tut_einstein
Messages
31
Reaction score
0
Hi,

I'm trying to determine the exact transformation that brings a spherically symmetric spacetime metric in spherical coordinates to the Sylvester normal form (that is, with just 1 or -1 on its main diagonal, with all other elements equal to zero.) Assuming that the metric has Lorentzian signature, does anyone know how to determine the exact transformation that achieves this?

Thanks.
 
Physics news on Phys.org


This is essentially nothing more than the orthogonal diagonalisation of a symmetric matrix that you probably did loads of times when you first learned about matrices. The coordinate transformation can be calculated from the matrix of eigenvectors. This gives a diagonal matrix, which should have one negative and the rest positive entries. Then you just have to rescale the coordinates to make the entries -1 and +1.
 


henry_m said:
Then you just have to rescale the coordinates to make the entries -1 and +1.

tut_einstein, this, in general, results in a non-holonomic basis. i.e., one that is not induced by any coordinate system. As a specific example, consider Schwarzschild spacetime,

https://www.physicsforums.com/showthread.php?t=102902
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K