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Unit 21: New Spherical Indicatrices and their Characterizations




          Let  =  (s ) be M  Bishop  spherical image of a  regular curve   =  (s).  We follow  the  same  Notes
                         1
                   
          procedure  to investigate the relations  among Bishop and Frenet-Serret  invariants. Thus,  we
          differentiate
                                            d ds
                                             
                                          '        k T.
                                                      1
                                            ds ds
                                              
          First, we have
                                               ds
                                      T  = T and       k .                        (4)
                                               ds    1
          So, one can calculate

                                            ds
                                       '
                                      T   T    ds     k M  k M 2
                                                    1
                                                       2
                                                 1
                                       
          or
                                                  k
                                           '
                                         T   M   k 2 1  M .
                                                1
                                                      2
                                          
          Since, we express
                                                       2
                                                     k 
                                            
                                       K   T   1    2                           (5)
                                            
                                        
                                                    k 1 
          and
                                             M     k
                                        N   K  1   k K 2    M .
                                                        2
                                         
                                                   1
          Cross product of T  × N  gives us the binormal vector field of M  spherical image of  = (s)
                                                            1
                                            k       1
                                        B   k K 2    M  K  M .
                                                        2
                                                 1
                                         
                                            1
          Using the formula of the torsion, we write
                                                  '
                                            k 1    k  
                                                2
                                       T     k 1   .                             (6)
                                             2
                                        
                                            k  k 2 2
                                             1
          Considering equations (5) and (6) by the Theorem 1, we get:
          Corollary 2. Let  = (s ) be the M  Bishop spherical image of the curve  = (s). If  = (s) is a
                                      1
                             
          B-slant helix, then, the M  Bishop spherical indicatrix (s ) is a circle in the osculating plane.
                              1
                                                       
          Theorem 2. Let  = (s ) be the M  Bishop spherical image of a regular curve  = (s). There exists
                                    1
                            
          a relation among Frenet-Serret invariants (s ) and Bishop curvatures of  = (s) as follows:
                                              
                                       k 2  s  K T ds .                             (7)
                                             2
                                       k 1     0      


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