Discussion Overview
The discussion revolves around the interpretation of energy conservation in the context of a laboratory on Earth, as presented in Schutz's work on geodesics and gravitational fields. Participants explore the implications of the geodesic equation and its application to non-geodesic paths, particularly in a weak gravitational field.
Discussion Character
- Exploratory
- Debate/contested
- Technical explanation
- Conceptual clarification
Main Points Raised
- One participant questions how the expression for a geodesic applies to a lab on Earth, suggesting that the lab does not follow a geodesic and thus challenges the conservation of momentum in this context.
- Another participant asserts that conserved quantities can apply to all valid paths, not just geodesics.
- Concerns are raised about the presentation of the example in Schutz, with emphasis on whether the derived expression is valid for any trajectory or specifically for geodesics.
- Some participants discuss the implications of forces other than gravity affecting trajectories and how this relates to energy conservation.
- There is a suggestion that the conservation law discussed may pertain to a ball in free fall within the lab's frame, rather than the lab itself.
- Several participants highlight the importance of symmetry and the existence of a timelike Killing vector field in establishing conserved quantities in stationary gravitational fields.
- One participant notes that while the geodesic equation is derived for geodesics, the conservation of energy can still apply to orbits of the timelike Killing vector field, which includes the lab's worldline.
- Another participant emphasizes that the conservation of energy is linked to the time independence of the metric components in the chosen coordinate system.
Areas of Agreement / Disagreement
Participants express differing views on the applicability of the geodesic equation to the lab's worldline. While some argue that conservation laws can apply to non-geodesic paths, others maintain that the derivation in Schutz is specifically for geodesics. The discussion remains unresolved regarding the interpretation of energy conservation in this context.
Contextual Notes
Participants note that the derivation of the geodesic equation may not encompass all trajectories, particularly those influenced by additional forces. The discussion also highlights the dependence on the choice of coordinates and the implications of symmetry in gravitational fields.