Discussion Overview
The discussion revolves around the concept of four momentum in General Relativity (GR), particularly how it differs from Special Relativity (SR) and the implications of curved spacetime on its definition and interpretation. Participants explore the relationship between four momentum and four velocity, as well as the distinctions between covariant and contravariant forms of momentum.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- One participant notes that in SR, four momentum is defined as p^α=mU^α, but questions whether this holds in curved space, suggesting that four momentum may be a covector in GR.
- Another participant agrees that both p^α and p_α can be referred to as "the four momentum," but emphasizes the need to distinguish between the four momentum vector and covector.
- A participant expresses confusion regarding the definition of p_0=-E in the context of the Schwarzschild metric, questioning the rationale behind defining p^0=g^{00}p_0=(1-{2M}/r)^{-1}E.
- One participant clarifies that p_0=±p^0=±E holds only in metrics where the 00 component is ±1, and discusses the relationship between vector and covector momentum as p_{\mu}=g_{\mu\nu}p^{\nu}.
- There is mention of additional relevant posts in the thread that may provide further insights.
Areas of Agreement / Disagreement
Participants express varying levels of understanding and interpretations regarding the definitions and relationships of four momentum in GR, indicating that there is no consensus on the matter. Some participants agree on the distinction between covariant and contravariant forms, while others raise questions about specific definitions and conventions.
Contextual Notes
Participants highlight that the interpretation of four momentum can depend on the specific metric being used, and that the definitions may not always align with intuitive notions from SR. There are also unresolved questions regarding the conventions used in defining momentum in different contexts.