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Unit 30: Geodesic Curvature and Christoffel Symbols




          Then, we have a map from  to S , where (u, v) is mapped to the point N(u, v) on S  associated  Notes
                                                                             2
                                     2
          with N(u,v). This map is denoted as N :   S . It is interesting to study the derivative dN of the
                                               2
          Gauss map N :  S  (or N : X  S ). As we shall see, the second fundamental form can be defined
                         2
                                    2
          in terms of dN. For every (u, v)  , the map dN (u,v)  is a linear map dN (u,v)  :     .
                                                                             2
                                                                        2
          It can be viewed as a linear map from the tangent space T (u,v) (X) at X(u, v) (which is isomorphic to
           ) to the tangent space to the sphere at N(u, v) (also isomorphic to  ).
                                                                  2
           2
          Recall that dN (u,v)  is defined as follows: For every (x, y)   ,
                                                          2
                                       dN (u,v) (x, y) = N x + N y.
                                                   u
                                                        v
                                                                    .
          Thus, we need to compute Nu and Nv. Since N is a unit vector, N N = 1, and by taking
                               .
          derivatives, we have Nu N = 0 and N v  .  N = 0.
          Consequently, N  and N  are in the tangent space at (u, v), and we can write
                        u
                              v
                                          N  = aX  + cX ,
                                                 u
                                            u
                                                     v
                                          N  = bX  + dX .
                                            v
                                                u
                                                     v
          Lemma 2. Given a surface X, for any point p = X(u, v) on X, the derivative dN (u,v)  of the Gauss map
          expressed in the basis (X , X ) is given by the equation
                              u
                                 v
                                                       x
                                            
                                             x  
                                      dN (u,v)    a b   ,

                                               
                                                      
                                                       y
                                             y
                                               c d 
          where the Jacobian matrix J(dN (u,v) ) of dN (u,v)  is given by
                                      1
                                      
                       a b     E  F   L  M 
                            =          
                        c d    F  G  M  N 
                                 1    MF LG NF MG 
                            =       2               .
                                 
                                                 
                              EG F   LF ME   MF NE 
                                        
          The equations
                     J(dN  )  =   a b 
                         (u,v)     
                                c d
                                 1    MF LG NF MG 
                                                 
                                         
                            =       2                 .
                                 
                                                 
                                        
                              EG F   LF ME   MF NE 
          are know as the Weingarten equations (in matrix form).
          If we recall the expressions for the Gaussian curvature and for the mean curvature
              GL – 2FM + EN
          H =              ,
                2(EG – F )
                       2
              LN – M 2
          K =        ,
              EG – F 2
          we note that the trace a + d of the Jacobian matrix J(dN (u,v) ) of dN (u,v)  is –2H, and that its determinant
          is precisely K.
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