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Unit 21: New Spherical Indicatrices and their Characterizations




          21.1 Preliminaries                                                                    Notes

          To meet the requirements in the next sections, here, the basic elements of the theory of curves in
          the space E  are briefly presented; a more complete elementary treatment can be found further.
                   3
          The Euclidean 3-space E  provided with the standard flat metric given by
                              3
                                                       2
                                                   2
                                              2
                                         ,   dx   dx  dx ,
                                                       3
                                              1
                                                   2
          where (x , x , x ) is a rectangular coordinate system of E . Recall that, the norm of an arbitrary
                                                        3
                 1
                    2
                      3
                    3
          vector a  E  is given by  a   a,a .   is called a unit speed curve if velocity vector v of 
                                         3
          satisfies  v  = 1. For vectors v, w  E  it is said to be orthogonal if and only if  v,w  0.  Let
          v = v(s) be a regular curve in E . If the tangent vector of this curve forms a constant angle with a
                                   3
          fixed constant vector U, then this curve is called a general helix or an inclined curve. The sphere
          of radius r > 0 and with center in the origin in the space E  is defined by
                                                         3
                                  S = {p = (p ; p ; p ) E : p; p = r }.
                                   2
                                                    3
                                                             2
                                                  
                                                3
                                           1
                                             2
          Denote by {T, N, B} the moving Frenet-Serret frame along the curve  in the space E . For an
                                                                               3
          arbitrary curve  with first and second curvature, K and T in the space E , the following Frenet-
                                                                    3
          Serret formulae are written under matrix form
                                                       T
                                       T'     0  K  0   
                                                     
                                                       N ,
                                            
                                         
                                       N'   K  0  T   
                                                       B
                                       B'     0   T  0   
                                                      
          where
                                       T,T   N,N   B,B  1,
                                    T,N = T,B = T,N = N,B = 0.
          Here, curvature functions are defined by K = K(s) =  T'(s)  and T(s) =  N,B .
          Let u = (u , u , u ), v = (v , v , v ) and w = (w ,w ,w ) be vectors in E and e , e , e  be positive
                                                                  3
                                                                            3
                                                    3
                                    3
                     2
                               1
                                 2
                        3
                  1
                                               1
                                                                        1
                                                  2
                                                                          2
          oriented natural basis of E . Cross product of u and v is defined by
                               3
                                               e 1  e 2  e 3
                                        u × v =  u 1  u 2  u .
                                                       3
                                               v 1  v 2  v 3
          Mixed product of u; v and w is defined by the determinant
                                               u 1  u 2  u 3
                                      [u, v, w] =  v 1  v 2  v .
                                                        3
                                               w 1  w 2  w 3
          Torsion of the curve  is given by the aid of the mixed product
                                              ', '', '''    
                                          T          .
                                                K 2
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