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Unit 29: Geodesics




          Thus, we have:                                                                        Notes

                1         1   i  j   1     i  j  i      1    k  i  j  i y . j
                                   
                                                           j 
                                           g
                                                       
                                                                        
                                                  
                                
                     ,
                                ij
                                                       ij
                                                                    ij,k
                                                                             ij
                2   g     s 0    2  g     s 0    2  ij  s 0      g     s 0    2  g y    g   
                         
                                               
                                      
                                                              
          Since Y vanishes at the endpoints, we can substitute into E (0),  and integrate by parts the second
                                                        
                                                        
          term to get:
                                          b d       1
                                                  
                                                         i
                                                 i
                                   
                                  E (0)         g    g ik,j     k  y . j
                                                
                                                         
                                         a dt  ij  2        
                                           
          Since:
                             d    i   i  g  i  k   i  1     g   i  k ,
                                      
                                                   
                                              
                                                                 
                                 
                            dt   g    g    ij,k    g    2  g ij,k    kj,i    
                                ij
                                      ij
                                                  ij
          We now see that:
                                  i
                                                     m
                                                          j
                       
                     E (0)    b  g    1  g   g   g      k  y dt    b   g    ,Y  dt.
                                 
                                                     
                            a      ij  2  mj,k  kj,m  mk ,j     a    
          Since  E (0) 0  for all vector fields Y along  which vanish at the endpoints, we conclude that
                
                    
                
              0,  and  is a geodesic.
             
             
          The  Schwartz inequality  implies  the  following inequality  between  the  length  and  energy
          functional for a curve .
          Lemma 2. For any curve , we have
                                           2
                                                   
                                          L  2E (b a),
                                                
                                            
          with equality if and only if  is parametrized proportionally to arc length.
          Finally, the last lemma we state to prove Theorem 1, exhibits the relationship between the L and
          E functionals.
          Lemma 3. A locally energy-minimizing curve is locally length-minimizing. Furthermore, if  is
          locally length-minimizing  and   is a reparametrization of    by arc  length, then    is  locally
          energy-minimizing.
          Proof. Suppose that  is locally energy-minimizing, and let  be a fixed endpoint variation of .
          For each s, let   s (t):[a,b]  U  be a reparametrization of the curve  t    (t;s)  proportionally to
          arc length. Let  (t;s)   s (t),  then it is not difficult to see, using say the theorem on continuous
                       
          dependence  on  parameters  for  ordinary  differential  equations,  that    is  also  smooth.  By
                                                2
                                                        
          Lemma 1,  is a geodesic, hence by Lemma 5,  L  2E (b a).  It follows that:
                                                     
                                                 
                       2
                                                                 2
                             2
                                                                       2
                                                            
                      L (0)   L   2E (b a)   2E (0)(b a) 2E (s)(b a)   L (s)  L (s).
                                     
                                                   
                                                
                                                                 
                                                                       
                                  
                             
                       
                                                       
                                           
          Thus,  is locally length-minimizing proving the first statement in the lemma.
          Now suppose that  is locally length-minimizing, and let  be a reparametrization of  by arc
          length. Then  is also locally length-minimizing, hence for any fixed-endpoint variation   of ,
          we have:
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