Clairaut relation for geodesics of Hopf tubes (Q879188)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Clairaut relation for geodesics of Hopf tubes |
scientific article; zbMATH DE number 5150224
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Clairaut relation for geodesics of Hopf tubes |
scientific article; zbMATH DE number 5150224 |
Statements
Clairaut relation for geodesics of Hopf tubes (English)
0 references
8 May 2007
0 references
The theorem of L. C. Clairaut is known: If \(\theta\) is the angle between the tangent to the curve and a circle of latitude, and if \(r\) is the radius of this circles, then \(r\cos \theta =\) const. along the curve. By using the hopf maps \(\pi:S^3\rightarrow S^2\), the authors have constructed a Riemannian metrics \(h^f\) on the 3-sphere. Then the authors considered the Hopf tube over an immersed curve \(\nu\) in \(S^2\) is the complete lift \(\pi^{-1}(\nu)\) of \(\nu\), and it is proved that any geodesic of this Hopf tube satisfies the Clairaut relation. Also it is proved that if the sphere \(S^3\) is equipped with a familly \(h^f\) of Lorentzian metrics, then it is obtained a new Clairaut relation for timelike geodesics of the Lorentzian Hopf tube.
0 references
Hopf map
0 references
generalized Klauza-Klein metric
0 references
0.7236636877059937
0 references
0.7076108455657959
0 references
0.7075663805007935
0 references
0.7048383951187134
0 references