Unifying Curvatures with Riemann Tensor

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SUMMARY

The discussion focuses on the unification of curvature definitions for curves and surfaces through the Riemann Tensor. Specifically, it highlights that the Riemann curvature tensor component R_{1,1,1,1} equals zero, indicating no curvature for a curve in \(\mathbb{R}^2\) or \(\mathbb{R}^3\). In contrast, R_{1,2,1,2} corresponds to the Gaussian curvature of surfaces. The Gaussian curvature K for a one-dimensional curve can be calculated using K=-R_{1212}/det(g), leveraging the Nash-Kuiper theorem to embed the curve in higher-dimensional manifolds.

PREREQUISITES
  • Understanding of Riemannian geometry
  • Familiarity with the Riemann curvature tensor
  • Knowledge of Gaussian curvature
  • Concept of embeddings in higher-dimensional manifolds
NEXT STEPS
  • Study the Nash-Kuiper theorem and its implications for curvature
  • Explore the Gauss-Codazzi equations in detail
  • Learn about the properties and applications of the Riemann curvature tensor
  • Investigate the relationship between main curvatures and Gaussian curvature
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Mathematicians, physicists, and students of differential geometry interested in the relationships between curvature in different dimensions and the applications of the Riemann Tensor in theoretical frameworks.

bchui
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I always wonder how the definitions of curvatures of curves and surfaces be unified by the Riemann Tensor symbols.
For surfaces, I know R_{1,2,1,2} corresponds to the Gaussian curvature of a surface. How come R_{1,1,1,1}=0 and not corresponds to the curvature of a curve in \RE^2 or in \Re^3 ?:confused:
 
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Recall that:

[tex]R_{ijkl}=\dfrac{\partial \Gamma_{ijl}}{\partial u^k}- \dfrac{\partial \Gamma_{ijk}}{\partial u^l}+\Gamma^h_{ik}\Gamma_{jhl}-\Gamma^h_{il}\Gamma_{jhk}[/tex]

So that:

[tex]R_{1111}=\dfrac{\partial \Gamma_{111}}{\partial u^1}-\dfrac{\partial \Gamma_{111}}{\partial u^1}+\Gamma^h_{11}\Gamma_{1h1}-\Gamma^h_{11}\Gamma_{1h1}\\<br /> =0[/tex]

For any finite dimensional Riemannian manifold. Moreover, we can still calculate the Gaussian curvature, [tex]K[/tex] for a 1-D curve via

[tex]K=-\dfrac{R_{1212}}{\text{det}g}[/tex]

by first viewing the curve as an embedding in a higher dimesional manifold, in particular [tex]\mathbb{R}^2[/tex] or higher--which is possible via the Nash-Kuiper theorem--allowing the appropriate number of terms to appear in the calculation.

There you have it!
 
Last edited:
How about the curvature of a curve on the plane?
Applying Gauss-Codazzi equation and we have [tex]R_{1,1,1,1}=0[/tex] and the Gaussian curvature of the plane [tex]\Re^2[/tex] is also zero!
The difference is that the curvatures of curves are the "main curvatures" [tex]k_1,k_2[/tex] while the "curvature tensors" [tex]R_{i,j,k,l}[/tex] has something to do with the Gaussian curvatures [tex]K=k_1k_2[/tex]
 

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