Intuition regarding Riemann curvature tensor

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SUMMARY

The Riemann curvature tensor is defined by the inclusion of second derivatives of the metric and squares of the first derivatives, which cannot be eliminated locally by a choice of coordinates. In Riemann normal coordinates, first derivatives are zero at the origin, but as one moves away from this point, they become non-zero and vary with direction. This behavior is crucial for capturing the full curvature dynamics of a manifold. The presence of first derivatives is essential for understanding curvature changes in different directions away from the origin.

PREREQUISITES
  • Understanding of Riemannian geometry
  • Familiarity with the concept of curvature in differential geometry
  • Knowledge of Riemann normal coordinates
  • Basic grasp of metric tensors and their derivatives
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  • Study the properties of the Riemann curvature tensor in detail
  • Explore the implications of Riemann normal coordinates on curvature
  • Investigate the relationship between first and second derivatives in differential geometry
  • Learn about the applications of curvature in general relativity
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Mathematicians, physicists, and students of differential geometry who seek to deepen their understanding of curvature and its implications in various fields, including general relativity.

Hill
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TL;DR
"Why" there are terms quadratic in first derivatives of metric?
The Riemann curvature tensor contains second derivatives of metric and squares of the first derivatives. The second derivatives have to be there because they are the ones that cannot be eliminated locally by a choice of coordinates. But other than being a mathematical artifact, is there a meaning for the squares of the first derivatives to be there?
 
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The first derivatives tell you directions. Curvature can be different in different directions. And the curvature in one direction can change as you move in a different direction
 
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Hill said:
The second derivatives have to be there because they are the ones that cannot be eliminated locally by a choice of coordinates.
If you look at how this actually works, you find that in Riemann normal coordinates, which are the ones that eliminate everything that can be eliminated by a choice of coordinates, the first derivatives are zero at the origin of coordinates, i.e., at the point the coordinates are "centered" on. So at that point, the first derivatives indeed do not appear at all in the Riemann tensor.

But as soon as you move away from the origin, the first derivatives are no longer zero (because the second derivatives weren't zero at the origin), and they will be different depending on which direction you move. So you do need them to capture the complete behavior once you are away from the origin.
 
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PeterDonis said:
But as soon as you move away from the origin, the first derivatives are no longer zero (because the second derivatives weren't zero at the origin)
lndeed, a zero second derivatives w.r.t. a coordinate basis at the origin, would mean constant first derivatives in a neighborhood of the origin, but first derivatives by definition vanish at the origin in Riemann normal coordinates centered on it.
 

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