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Kurventheorie im konform isotropen RaumC 3 (1)
Authors:Walter O Vogel
Institution:(1) Mathematisches Institut II, Universität Karlsruhe, Kaiserstraße 12, D-76128 Karlsruhe
Abstract:LetM be a 3-dimensional manifold with metric tensorg. (M,g) is called a conformally isotropce space C 3 (1) if there exists a chart (M, phiv) of M, for which (i)phiv(M)=Ropf3, (ii) the components ofg with respect tophiv areg 11=g 22=q,g 12=g 13=g 23=g 33=0q(x 1,x2,x3) > 0, 
$$\frac{{\partial _q }}{{\partial _{x^3 } }}\left( {x^1 ,x^2 ,x^3 } \right) > 0$$
. In this note, first we consider some metric properties ofC 3 (1) . Further it is shown that there exists a unique linear connection Delta inC 3 (1) , the so-called standard connection. Finally we develop the fundamentals of the theory of curves inC 3 (1) up to Frenet's formula, and give a geometric interpretation of the conformally isotropic curvaturekappa resp. torsiontau of a curvec inC 3 (1) . It is shown, that 
$$\kappa = \frac{1}{{\sqrt q }}\kappa ^ \star ,\tau = \frac{1}{{\sqrt q }}\tau ^ \star $$
, wherekappa sstarf resp.tau sstarf are the isotropic curvature resp. isotropic torsion of the curvec in the threedimensional isotropic spaceI 3 (1) when using a special coordinate system ofC 3 (1) as the standard coordinate system ofI 3 (1) .

Herrn Prof. Dr. Oswald Giering zum 60. Geburtstag gewidmet
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