Page 243 - 35Linear Algebra
P. 243

13.2 Change of Basis                                                                          243


                              i
                   Here, the p are constants, which we can regard as entries of a square ma-
                              k
                               i
                   trix P = (p ). The matrix P must have an inverse since we can also write
                               k
                                                                     0
                   each v j uniquely as a linear combination of the v ;
                                                                     k
                                                        X
                                                             0
                                                               k
                                                   v j =    v q .
                                                             k j
                                                         k
                      Then we can write
                                                     X X
                                                                i k
                                                v j =        v i p q .
                                                                k j
                                                      k   i
                       P
                            i k
                   But     p q is the k, j entry of the product matrix PQ. Since the expression
                          k  k j
                   for v j in the basis S is v j itself, then PQ maps each v j to itself. As a result,
                   each v j is an eigenvector for PQ with eigenvalue 1, so PQ is the identity, i.e.
                                               PQ = I ⇔ Q = P    −1  .

                      The matrix P is called a change of basis matrix. There is a quick and
                   dirty trick to obtain it; look at the formula above relating the new basis
                            0
                               0
                                     0
                   vectors v , v , . . . v to the old ones v 1 , v 2 , . . . , v n . In particular focus on v 0 1
                               2
                                     n
                            1
                   for which
                                                                 
                                                                  p 1
                                                                    1
                                                                  p
                                                                 2
                                            0

                                           v = v 1 , v 2 , · · · , v n  .  .
                                                                 1
                                                                   .
                                            1
                                                                 . 
                                                                  p n
                                                                   1
                   This says that the first column of the change of basis matrix P is really just
                                                   0
                   the components of the vector v in the basis v 1 , v 2 , . . . , v n .
                                                   1
                         The columns of the change of basis matrix are the components
                            of the new basis vectors in terms of the old basis vectors.
                                          0
                                                0
                                                   0
                   Example 130 Suppose S = (v , v ) is an ordered basis for a vector space V and that
                                                   2
                                                1
                   with respect to some other ordered basis S = (v 1 , v 2 ) for V
                                                1  !                 1  !
                                               √                     √
                                         0
                                                             0
                                        v =     2      and v =        3    .
                                         1     √ 1           2     − √ 1
                                                2  S                  3  S
                                                                  243
   238   239   240   241   242   243   244   245   246   247   248