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Unit 26: Lines of Curvature




          Proof. The proof uses the following transformation introduced by H. Lewy:             Notes

                                       (u,v)    ,   (u p,v q)    
          where p = h , and q = h . Clearly,  is continuously differentiable, and its Jacobian is:
                    u
                             v
                                               
                                              1 r  s 
                                         d      s  1 t  ,
                                                    
                                             
                                                  
                                                       
                                                    
          where r = h , s = h , and t = h . Since  det d  2 r t 0,  it follows from the inverse function
                   uu
                                  vv
                         uv
          theorem that  is a local diffeomorphism, i.e., each point has a neighborhood on which  is a
          diffeomorphism. In particular,  is open.
          In view of the convexity of the function h, we have :
          u  u 1    1  v  2   v 1    1 
                                 2
            2
                   2
                                                       2
                                              2
                                       u  u 1  v  2   v 1  u  2   u 1 p  p 1  v  2   v 1 q  q 1 
                                                                                 2
                                                                  2
                                          2
                                                                                     2
                                                                            2
                                                                     u  u 1  v  2   v 1  ,
                                                                       2
          and therefore:
                                      2
                                                       2
                                               2
                                                                2
                               u  u 1  v  2   v 1     1     1  ,
                                                        
                                                
                                                           2
                                 2
                                                   2
          i.e.,  is an expanding map. This implies immediately that  is one-to-one. Thus,  has an inverse
          (u, v) =   (, ) which is also a diffeomorphism. Consider now the function
                  –1
                                                  
                                               
                                           
                                        
                                f    i    u p i(v q) 2u      i  2v   ,
                     1.
          where  i    In view of
                                                  1
                                                       
                                                             s  
                                   1
                                            
                                   
                                 d      u    u      2 r t    1 t  1 r   ,
                                                        s
                                       v
                                                
                                                       
                                                            
                                                   
                                          v 
                                            
          it is straightforward to check that f satisfies the Cauchy-Riemann equations, and consequently
          f is analytic. In fact, f is an entire functions and so is f. Furthermore,
                                    (t r) 2is      2       4
                                      
                                         
                                                      1
                               f ( )        ,  f ( )         1,
                                
                                                
                                                 
                                 
                                      2 r t              2 r t
                                                            
                                       
                                         
                                                          
          and Liouville’s Theorem gives that f is constant. Finally, the relations:
                                       2                      2
                                                 
                                   1 f          i f    f  1 f
                                     
                                                            
                                f     2  ,  s    2  ,  t   2  ,
                                   1   f     1   f    1   f
          show that r, s, t are constants.
          26.5 Theorema Egregium
          In this section, we prove that the Gauss curvature can be computed in terms of the first fundamental
          form and its derivatives. We then prove the Fundamental Theorem for surfaces in  , analogous
                                                                             3
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