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Unit 24: Two Fundamental Form





                                      
                                                                    
          Proof. Let    V . The unit normal  N( ) of X at       is perpendicular to  T X.  By Proposition 1, we  Notes
                                                                   
          have  T  ( ) X  T X. Thus,  N( )  is perpendicular to  T  ( ) X,  as is   ( ) .     It follows that the two
                                                             N
                               
                       
                 
                      
                                                     
                                     
          vectors are co-linear, and hence  N( )   N  ( ) .     But since  is orientation preserving, the two
                         
                                                                
          pairs (X , X ) and  X ,X   2   have the same orientation in the plane  T X.  Since also, the two triples
                          1
                1
                   2
                                                               
          X1  ( ) ,X2 ( ) ,N ( )              and  X ( ),X ( ),N( )    2        have the same orientation in  , it follows
                                                                              3
                                       
                                        1
                    
              N
                       
                        
          that   ( )    N( ).
          24.2 The First Fundamental Form
          Definition 6. A symmetric bilinear form on a vector space V is function  B : V V     satisfying:
          1.   B(aX + bY,Z) = aB(X,Z) + bB(Y,Z), for all X, Y  V and a, b  R.
          2.   B(X, Y) = B(Y, X), for all X, Y  V.
          The symmetric bilinear form B is positive definite if B(X, X)  0, with equality if and only if
          X = 0.
          With any symmetric bilinear form B on a vector space, there is associated a quadratic form Q(X)
          = B(X, X). Let V and W be vector spaces and let  T : V   W  be a linear map. If B is a symmetric
          bilinear form on W, we can define a symmetric bilinear form T* Q on V by T* Q(X, Y) = Q(TX,
          TY). We call T* Q the pull-back of Q by T. The map T is then an isometry between the inner-
          product spaces (V, T* Q) and (W,Q).
                 Example: Let V =   and define B(X, Y) = X  Y , then B is a positive definite symmetric
                                3
          bilinear form. The associated quadratic form is Q(X) = |X| .
                                                          2
                 Example: Let  A be  a symmetric  2 ×  2 matrix,  and let  B(X, Y)  = AX    Y, then  B is  a
          symmetric bilinear form which is positive definite if and only if the eigenvalues of A are both
          positive.

                               3
          Definition 7. Let  X : U    be a parametric surface. The first fundamental form is the symmetric
          bilinear form g defined on each tangent space T  X by:
                                                 u
                                    g(Y, Z) = Y  Z,  Y, Z  T X.
                                                          u
          Thus, g is simply the restriction of the Euclidean inner product in above Example to each tangent
          space of X. We say that g is induced by the Euclidean inner product.

          Let g  = g(X , X), and let Y = y  X  and Z = z  X  be two vectors in T  X, then
                                            i
                                  i
                                                              u
                                              i
                                    i
              ij
                      j
                   i
                                      g(Y,Z) = g  y  z. j                               ...(3)
                                                 i
                                               ij
          Thus, the so-called coordinate representation of g is at each point u   U an instance of above
                                                                 0
          example. In fact, if A = (g ), and B(, ) =   A for     as in the above example, then B is the
                                                        
                              ij
          pull-back by  dX :  2   T X  of the restriction of the Euclidean inner product on T  X.
                               u
                       u
                                                                            u
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