Describing 4-vectors in space-time

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    4-vectors Space-time
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SUMMARY

The discussion centers on the mathematical representation of 4-vectors in space-time, specifically the transformation of a 4-vector using a metric tensor. The formula presented, u^{\alpha}=u_{\beta}g^{\alpha\beta}, illustrates how to derive a new 4-vector in a specified metric space. The concept of local vector fields is introduced, emphasizing their variability across different points on a manifold, particularly in curved spaces where they reside in the tangent space.

PREREQUISITES
  • Understanding of 4-vectors in physics
  • Familiarity with metric tensors in differential geometry
  • Knowledge of vector spaces and dual vector spaces
  • Concept of manifolds and tangent spaces
NEXT STEPS
  • Study the properties of metric tensors in general relativity
  • Explore the concept of local vector fields in curved manifolds
  • Learn about the isomorphism between vector spaces and dual vector spaces
  • Investigate applications of 4-vectors in physics, particularly in relativity
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Physicists, mathematicians, and students studying general relativity or differential geometry, particularly those interested in the mathematical foundations of space-time concepts.

jfy4
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I have a question...

I would like to generically describe a 4-vector locally in space-time. Would i go about that by simply taking a 4-vector and multiplying it by a metric? like

[tex]u^{\alpha}=u_{\beta}g^{\alpha\beta}[/tex]

with [tex]u^{\alpha}[/tex] the new 4-vector in the space specified by the metric?
 
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I'm not sure what you mean; what you've just written down is the notion of vector spaces and dual vector spaces being isomorphic, with the isomorphism given by the metric.

"Local vector fields" are vector fields which can change from point to point on your manifold. On curved manifolds these vectors live in the tangent space at that point.
 

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