Discussion Overview
The discussion revolves around the characterization of the object ##T^{ik}v_k##, where ##T^{ik}## is the stress-energy tensor and ##v_k## is a future-pointing, time-like four vector. Participants explore whether this object is future-pointing and not space-like, focusing on mathematical properties and conditions that must be satisfied.
Discussion Character
- Technical explanation
- Mathematical reasoning
- Debate/contested
Main Points Raised
- One participant asks how to determine that ##T^{ik}v_k## is future-pointing and not space-like.
- Another participant inquires about the dot product of two future-pointing timelike vectors in the context of the discussion.
- It is suggested to compute the squared length of the vector ##T^{ik}v_k## to analyze its properties.
- A participant proposes an expression for the squared length involving the metric tensor, but expresses uncertainty about its implications.
- Another participant confirms the expression for the squared length and notes that for the vector to be timelike, its squared length must have the same sign as ##v_k v^k##, hinting at conditions on the components of ##T^{ij}##.
- One participant presents their calculations for the squared length but struggles to derive conditions for ##T^{ik}## from them.
- A later reply challenges the accuracy of the earlier calculations, suggesting a different form for the expansion of ##T^{ik} v_k T_{ij} v^j##.
Areas of Agreement / Disagreement
Participants express differing views on the calculations and conditions for ##T^{ik}##, indicating that there is no consensus on the correct approach or results.
Contextual Notes
Participants note that the vector ##T^{ik}v_k## is not always timelike and that specific conditions on the components of ##T^{ij}## are necessary for it to be classified as such. There are unresolved mathematical steps and assumptions regarding the properties of the stress-energy tensor.