Time-Invariant Space: Metric ds^2 and Coordinates

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SUMMARY

The discussion focuses on the properties of time-invariant spaces characterized by the metric ds² = g_{tt}dt² + g_{xx}dx² + g_{yy}dy² + g_{zz}dz². It highlights that while spatial coordinates x, y, and z can take values in the range ]-∞, ∞[, the time coordinate t is constrained to [0, ∞[. This distinction is particularly relevant in the context of Minkowski space, where t spans the entire real line, contrasting with other spacetimes that exhibit varied coordinate behaviors. The inability to cover a manifold with a single coordinate chart is also emphasized as a fundamental aspect of general relativity.

PREREQUISITES
  • Understanding of general relativity concepts
  • Familiarity with Minkowski space and its properties
  • Knowledge of differential geometry and manifold theory
  • Basic grasp of metric tensors and their implications in spacetime
NEXT STEPS
  • Explore the implications of different metrics in general relativity
  • Study the concept of coordinate charts and their limitations in manifold theory
  • Investigate the role of time in various spacetime geometries
  • Learn about the mathematical formulation of Minkowski space and its applications
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This discussion is beneficial for physicists, mathematicians, and students of theoretical physics who are exploring the intricacies of spacetime metrics and their implications in general relativity.

alejandrito29
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Question: have some sense that in a space time with metric [tex]ds^2 = g_{tt}dt^2+ g_{xx}dx^2+ g_{yy}dy^2+g_{zz}dz^2[/tex], the coordinates [tex]x,y,z \in ]-\infty, \infty[[/tex] , but [tex]t \in [0, \infty[[/tex] ?
 
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In flat spacetime (Minkowski space), t ranges over the whole real line. In other spacetimes, there can be all kinds of different cases. In general, you can't even cover a whole manifold with a single coordinate chart.
 

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