Page 271 - 35Linear Algebra
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14.6 Orthogonal Complements                                                                   271


                                                                         4
                   Example 139 Consider any line L through the origin in R . Then L is a subspace,
                        ⊥
                   and L is a 3-dimensional subspace orthogonal to L. For example, let
                                                           
                                                           1 
                                                                
                                                              1
                                                                
                                                             
                                                 L = span    
                                                             
                                                           1 
                                                                
                                                              1
                                                                
                               4
                   be a line in R . Then
                                                                            
                                             x
                                                                               
                                                                              
                                              y
                                                                            
                                 L ⊥  =        ∈ R  4   (x, y, z, w) (1, 1, 1, 1) = 0
                                              z
                                            
                                                                               
                                                                              
                                                                               
                                             w
                                                                        
                                          
                                             x
                                                                        
                                                                       
                                              y
                                                                        
                                            
                                      =        ∈ R  4   x + y + z + w = 0  .
                                              z
                                            
                                                                        
                                                                       
                                             w
                                                                        
                                                                                       ⊥
                   Using the Gram-Schmidt procedure one may find an orthogonal basis for L . The set
                                                             
                                                  1       1
                                                                 1 
                                                                    
                                                                    
                                               −1      0     0 
                                                     ,
                                                             ,
                                                              
                                                  0     −1
                                                              
                                                                 0 
                                                                    
                                                  0       0     −1
                                                                    
                                    ⊥
                   forms a basis for L so, first, we order the basis as
                                                                   
                                                        1       1      1
                                                    −1      0    0 
                                                           ,
                                      (v 1 , v 2 , v 2 ) =            .
                                                                   ,
                                                        0     −1       0
                                                                   
                                                        0       0     −1
                                ⊥
                   Next, we set v = v 1 . Then
                                1
                                                            1  
                                             1          1        2
                                 v ⊥  =     0   −  1  −1   =    1  ,
                                                              
                                  2
                                         
                                              
                                                    
                                                         
                                                                 2
                                          −1    2    0     −1 
                                             0          0        0
                                                                               
                                                                1        1
                                             1          1            2         3
                                                                               3
                                                                                 .
                                 v ⊥  =     0   −  1  −1   −  1/2   1    1 
                                                                           
                                                                                
                                         
                                                         
                                                                     2
                                                                  
                                                    
                                              
                                  3                                      = 
                                            0   2    0    3/2   −1      1  
                                                                               3
                                           −1           0            0       −1
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