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Unit 26: Lines of Curvature




          Taking note of the fact that X  = X , we now interchange j and l and subtract to obtain (18) and  Notes
                                      ilj
                                 ijl
          (19).
          Equation (18) is called the Gauss Equation, and Equation (19) is called the Codazzi Equation. The
          Gauss Equation has the following corollary which has been coined Theorema Egregium. It’s
          discovery marked the beginning of intrinsic geometry, the geometry of the first fundamental
          form.

          Corollary 1. Let  X : U    be a parametric surface. Then the Gauss curvature K of X can be
                                3
                                                        g
          computed in  terms of only its first fundamental form     and its derivatives up to second
                                                         ij
          order:
                                     1
                                                          n
                                                    n
                                 K   g ij   m    m     m nm     m  ,
                                                             nj
                                                          im
                                     2
                                          ij,m
                                                    ij
                                               im,j
          where    are the Christoffel symbols of the first kind.
                 m
                 ij
          Proof.
          We now show, in a manner quite analogous to Theorem 6, that provided they satisfy the Gauss-
          Codazzi Equations, the first and second fundamental form uniquely determine the parametric
          surface up to rigid motion.
                                                                            g
                                               2
                                                                                     
          Theorem 7 (Fundamental Theorem). Let U    be open and simply connected, let   : U   S 2 2
                                                                             ij
                                                                                    
               k
                        
          and    : U  S 2 2    be smooth,  and suppose  that  they satisfy  the Gauss-Codazzi  Equations
                ij
                                                                       k
                                                               g
          (18)–(19). Then there is a parametric surface  X : U    such that    and    are its first and
                                                     3
                                                                 ij
                                                                        ij
          second fundamental  forms.  Furthermore,  X is  unique up  to rigid  motion: if  X  is  another
                                                                            
          parametric surface  with the same first  and second fundamental forms,  then there is a  rigid
          motion R of   such that  X R X.
                               
                     3
                                
                                   
          Proof. We consider the following over-determined system of partial differential equations for
          X ,X ,N: 6
              2
           1
                                       X   m ij  X  k N,                       ...(20)
                                               m
                                        i,j
                                                   ij
                                               im
                                       N   k g X ,                              ...(21)
                                                 m
                                        i
                                             ij
                 m
          where    is defined in terms of     by (16). The integrability conditions for this system are:
                                      g
                 ij
                                       ij
                                         m X   k N   m il  X  k N  j        ...(22)
                                                  
                                         ij
                                                            il
                                                        m
                                           m
                                               ij
                                                  l
                                        k g X m   k g X  lj  jm  m  .        ...(23)
                                          jm
                                         ij
                                               l
                                                         i
          The proof of Theorem 18 also shows that the Gauss-Codazzi Equations (18)–(19) imply (22) if Xi
          and N satisfy (20) and (21). We now check that (19) also implies (23). First note that since    is
                                                                                   m
                                                                                   ij
          defined by (16), we have
                                            1
                                      m g mn    2  g ni,j   g nj,i   g ij,n  .
                                      ij
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