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In [[Riemannian geometry]], the '''geodesic curvature''' <math>k_g</math> of a curve <math>\gamma</math> measures how far the curve is from being a [[geodesic]]. In a given manifold <math>\bar{M}</math>, the '''geodesic curvature''' is just the usual '''curvature''' of <math>\gamma</math> (see below), but when <math>\gamma</math> is restricted to lie on a submanifold <math>M</math> of <math>\bar{M}</math> (e.g. for [[Curvature#Curves on surfaces|curves on surfaces]]), geodesic curvature refers to the curvature of <math>\gamma</math> in <math>M</math> and it is different in general from the curvature of <math>\gamma</math> in the ambient manifold  <math>\bar{M}</math>. The (ambient) curvature <math>k</math> of <math>\gamma</math> depends on two factors: the curvature of the submanifold <math>M</math> in the direction of <math>\gamma</math> (the [[normal curvature]] <math>k_n</math>), which depends only from the direction of the curve, and the curvature of <math>\gamma</math> seen in <math>M</math> (the geodesic curvature <math>k_g</math>), which is a second order quantity. The relation between these is <math>k = \sqrt{k_g^2+k_n^2}</math>. In particular geodesics on <math>M</math> have zero geodesic curvature (they are "straight"), so that <math>k=k_n</math>, which explains why they appear to be curved in ambient space whenever the submanifold is.


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==Definition==
Consider a curve <math>\gamma</math> in a manifold <math>\bar{M}</math>, parametrized by [[arclength]], with unit tangent vector <math>T=d\gamma/ds</math>. Its curvature is the norm of the [[Covariant derivative#Derivative along curve|covariant derivative]] of <math>T</math>: <math>k = \|DT/ds \|</math>. If <math>\gamma</math> lies on <math>M</math>, the '''geodesic curvature''' is the norm of the projection of the covariant derivative <math>DT/ds</math> on the tangent space to the submanifold. Conversely the '''normal curvature''' is the norm of the projection of <math>DT/ds</math> on the normal bundle to the submanifold at the point considered.
 
If the ambient manifold is the euclidean space <math>\mathbb{R}^n</math>, then the covariant derivative <math>DT/ds</math> is just the usual derivative <math>dT/ds</math>.
 
==Example==
Let <math>M</math> be the unit sphere <math>S^2</math> in three dimensional Euclidean space. The normal curvature of <math>S^2</math> is identically 1, independently of the direction considered. Great circles have curvature <math>k=1</math>, so they have zero geodesic curvature, and are therefore geodesics. Smaller circles of radius <math>r</math> will have curvature <math>1/r</math> and geodesic curvature <math>k_g = \sqrt{1-r^2}/r</math>.
 
==Some results involving geodesic curvature==
 
*The geodesic curvature is no other than the usual curvature of the curve when computed intrinsically in the submanifold <math>M</math>. It does not depend on the way the submanifold <math>M</math> sits in <math>\bar{M}</math>.
 
* Geodesics of <math>M</math> have zero geodesic curvature, which is equivalent to saying that <math>DT/ds</math> is orthogonal to the tangent space to <math>M</math>.
 
*On the other hand the normal curvature depends strongly on how the submanifold lies in the ambient space, but marginally on the curve: <math>k_n</math> only depends on the point on the submanifold and the direction <math>T</math>, but not on <math>DT/ds</math>.
 
*In general Riemannian geometry, the derivative is computed using the [[Levi-Civita connection]] <math>\bar{\nabla}</math> of the ambient manifold: <math>DT/ds = \bar{\nabla}_T T</math>. It splits into a tangent part and a normal part to the submanifold: <math>\bar{\nabla}_T T = \nabla_T T + (\bar{\nabla}_T T)^\perp</math>. The tangent part is the usual derivative <math>\nabla_T T</math> in <math>M</math> (it is a particular case of Gauss equation in the [[Gauss-Codazzi equations]]), while the normal part is <math>\mathrm{I\!I}(T,T)</math>, where <math>\mathrm{I\!I}</math> denotes the [[second fundamental form]].
 
*The [[Gauss–Bonnet theorem]].
 
==See also==
* [[Curvature]]
* [[Darboux frame]]
* [[Gauss–Codazzi equations]]
 
== References ==
*{{citation | last = do Carmo|first =Manfredo P. | title=Differential Geometry of Curves and Surfaces | publisher=Prentice-Hall | year=1976 | isbn = 0-13-212589-7}}
* {{citation|first=Heinrich|last=Guggenheimer|author-link=Heinrich Guggenheimer|title=Differential Geometry|year=1977|publisher=Dover|chapter=Surfaces|isbn=0-486-63433-7}}.
* {{springer|id=G/g044070|title=Geodesic curvature|first=Yu.S.|last=Slobodyan|year=2001}}.
 
==External links==
* {{Mathworld|urlname=GeodesicCurvature|title=Geodesic curvature}}
 
 
 
[[Category:Geodesic (mathematics)]]
[[Category:Manifolds]]

Revision as of 19:33, 20 January 2014

In Riemannian geometry, the geodesic curvature kg of a curve γ measures how far the curve is from being a geodesic. In a given manifold M¯, the geodesic curvature is just the usual curvature of γ (see below), but when γ is restricted to lie on a submanifold M of M¯ (e.g. for curves on surfaces), geodesic curvature refers to the curvature of γ in M and it is different in general from the curvature of γ in the ambient manifold M¯. The (ambient) curvature k of γ depends on two factors: the curvature of the submanifold M in the direction of γ (the normal curvature kn), which depends only from the direction of the curve, and the curvature of γ seen in M (the geodesic curvature kg), which is a second order quantity. The relation between these is k=kg2+kn2. In particular geodesics on M have zero geodesic curvature (they are "straight"), so that k=kn, which explains why they appear to be curved in ambient space whenever the submanifold is.

Definition

Consider a curve γ in a manifold M¯, parametrized by arclength, with unit tangent vector T=dγ/ds. Its curvature is the norm of the covariant derivative of T: k=DT/ds. If γ lies on M, the geodesic curvature is the norm of the projection of the covariant derivative DT/ds on the tangent space to the submanifold. Conversely the normal curvature is the norm of the projection of DT/ds on the normal bundle to the submanifold at the point considered.

If the ambient manifold is the euclidean space n, then the covariant derivative DT/ds is just the usual derivative dT/ds.

Example

Let M be the unit sphere S2 in three dimensional Euclidean space. The normal curvature of S2 is identically 1, independently of the direction considered. Great circles have curvature k=1, so they have zero geodesic curvature, and are therefore geodesics. Smaller circles of radius r will have curvature 1/r and geodesic curvature kg=1r2/r.

Some results involving geodesic curvature

  • The geodesic curvature is no other than the usual curvature of the curve when computed intrinsically in the submanifold M. It does not depend on the way the submanifold M sits in M¯.
  • Geodesics of M have zero geodesic curvature, which is equivalent to saying that DT/ds is orthogonal to the tangent space to M.
  • On the other hand the normal curvature depends strongly on how the submanifold lies in the ambient space, but marginally on the curve: kn only depends on the point on the submanifold and the direction T, but not on DT/ds.

See also

References

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