Discussion Overview
The discussion revolves around the concept of orthonormal bases in the context of general relativity, specifically referencing Carroll's work. Participants explore the definitions of basic vectors and their properties, particularly in relation to coordinate systems and specific examples from general relativity.
Discussion Character
- Technical explanation
- Conceptual clarification
- Debate/contested
Main Points Raised
- One participant questions whether the basic vectors defined by gradients of coordinate functions are obviously orthonormal, suggesting that this may not be the case in non-orthogonal coordinate systems.
- Another participant agrees that the basis vectors in non-orthogonal systems cannot be considered orthonormal.
- Several examples from general relativity are proposed, including the geometry of Schwarzschild, the bending of light due to the sun's gravity, and Mercury's orbit, with a query about whether these typically use orthonormal bases.
- A participant notes that while examples (1) and (2) are orthogonal, they are not orthonormal, and points out that coordinate systems with mixed differential terms indicate non-orthogonality.
- It is mentioned that even simple coordinate systems like cylindrical and spherical coordinates yield orthogonal but not orthonormal basis vectors.
Areas of Agreement / Disagreement
Participants express differing views on the orthonormality of basis vectors in various coordinate systems, indicating that there is no consensus on the use of orthonormal bases in the examples provided.
Contextual Notes
There is an acknowledgment that the definitions and properties of orthonormal bases depend on the specific coordinate systems used, and the discussion highlights the complexity of these relationships without resolving them.