From Wikipedia, the free encyclopedia
|
This article is within the scope of WikiProject Physics, which collaborates on articles related to physics. |
Stub |
This article has been rated as Stub-Class on the assessment scale. |
??? |
This article has not yet received an importance rating within physics. |
Help with this template This article has been rated but has no comments. If appropriate, please review the article and leave comments here to identify the strengths and weaknesses of the article and what work it will need.
|
|
This article has been automatically assessed as Stub-Class by WikiProject Physics because it uses a stub template.
- If you agree with the assessment, please remove {{Physics}}'s auto=yes parameter from this talk page.
- If you disagree with the assessment, please change it by editing the class parameter of the {{Physics}} template, removing {{Physics}}'s auto=yes parameter from this talk page, and removing the stub template from the article.
|
To-do list for Curvature invariant (general relativity): |
edit · history · watch · refresh |
Task for expert:
- add material explaining how the following are related to the principle invariants:
- characteristic polynomial of Riemann tensor (as operator on bivectors),
- Hodge duals of curvature two-forms,
- Fermi normal coordinate chart,
- electric-electric, electric-magnetic, magnetic-magnetic parts of Riemann tensor in GEM formalism (correspond essentially to electrogravitic, magnetogravitic, topogravitic parts).
Task for anyone:
- spell check
- improve diction
- note anything unclear on talk page
|
[edit] Merge from Kretschmann scalar
Pretty much speaks for itself, but see Talk:Kretschmann scalar. ---CH 18:27, 24 December 2005 (UTC)