Spacetime Interval & Metric: Equivalent?

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SUMMARY

The spacetime interval is invariant, represented mathematically as ##ds^2=g_{ab}dx^a dx^b##, while the spacetime metric ##g_{ab}## is a tensor. Although these statements are closely related, they are not equivalent; the interval is a scalar derived from the contraction of the metric tensor with infinitesimal vectors. The spacetime interval, ##ds^2##, is a scalar quantity that remains unchanged under Lorentz transformations, distinguishing it from four-vectors.

PREREQUISITES
  • Understanding of tensor calculus, specifically tensor notation and operations.
  • Familiarity with the concept of Lorentz transformations in the context of special relativity.
  • Knowledge of differential geometry, particularly the properties of metrics and intervals.
  • Basic comprehension of four-vectors and their scalar products.
NEXT STEPS
  • Study the properties of tensors in differential geometry.
  • Learn about Lorentz transformations and their implications in special relativity.
  • Explore the mathematical formulation of spacetime intervals in various coordinate systems.
  • Investigate the relationship between metrics and curvature in general relativity.
USEFUL FOR

Physicists, mathematicians, and students of relativity who seek a deeper understanding of the relationship between spacetime intervals and metrics in the context of tensor analysis.

jmatt
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This may seem an odd question but it will clear something up for me. Are "The spacetime interval is invariant." and the "The spacetime metric is a tensor." exactly equivalent statements? Does one imply more or less information than the other?

Thanks!
 
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They aren't exactly equivalent, but they are closely related. The space time interval is ##ds^2=g_{ab}dx^a dx^b##. Because the metric ##g_{ab}## is a tensor, contracting it with (infinitesimal) vectors ##dx^{a}## will yield an invariant scalar ##ds^2##.
 
Matterwave said:
They aren't exactly equivalent, but they are closely related. The space time interval is ##ds^2=g_{ab}dx^a dx^b##. Because the metric ##g_{ab}## is a tensor, contracting it with (infinitesimal) vectors ##dx^{a}## will yield an invariant scalar ##ds^2##.
Thanks! A little confused why you referred to ##ds^2## as a scalar. Isn't it a four-vector?
 
jmatt said:
Thanks! A little confused why you referred to ##ds^2## as a scalar. Isn't it a four-vector?
Nope. It's the scalar product of (differential) four-vectors.
 
jmatt said:
Thanks! A little confused why you referred to ##ds^2## as a scalar. Isn't it a four-vector?

Why would it be a 4 vector? What are the 4 components that you are thinking of? It is a scalar because it's just 1 single number, which does not change under an arbitrary Lorentz transformation.
 
Got it now. Thanks very much.
 

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