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Constant curvature

From Wikipedia, the free encyclopedia

In mathematics, constant curvature is a concept from differential geometry. Here, curvature refers to the sectional curvature of a space (more precisely a manifold) and is a single number determining its local geometry.[1] The sectional curvature is said to be constant if it has the same value at every point and for every two-dimensional tangent plane at that point. For example, a sphere is a surface of constant positive curvature.

YouTube Encyclopedic

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  • Differential Geometry: Lecture 6 part 1: Frenet Serret Equations
  • Masoud Khalkhali, Curvature in Noncommutative Geometry
  • Differential Geometry: Lecture 28: applicationa of Gauss Bonnet

Transcription

Classification

The Riemannian manifolds of constant curvature can be classified into the following three cases:

Properties

  • Every space of constant curvature is locally symmetric, i.e. its curvature tensor is parallel .
  • Every space of constant curvature is locally maximally symmetric, i.e. it has number of local isometries, where is its dimension.
  • Conversely, there exists a similar but stronger statement: every maximally symmetric space, i.e. a space which has (global) isometries, has constant curvature.
  • (Killing–Hopf theorem) The universal cover of a manifold of constant sectional curvature is one of the model spaces:
  • A space of constant curvature which is geodesically complete is called space form and the study of space forms is intimately related to generalized crystallography (see the article on space form for more details).
  • Two space forms are isomorphic if and only if they have the same dimension, their metrics possess the same signature and their sectional curvatures are equal.

References

  1. ^ Caminha, A. (2006-07-01). "On spacelike hypersurfaces of constant sectional curvature lorentz manifolds". Journal of Geometry and Physics. 56 (7): 1144–1174. doi:10.1016/j.geomphys.2005.06.007. ISSN 0393-0440.

Further reading

This page was last edited on 26 February 2024, at 00:05
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