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Unit 14: Notation and Summation Convention




          It follows from equations (5) and (7) that                                            Notes

                                            x'   x 
                                       a     k    i  ,                           ...(8)
                                        ki
                                             x i   x' k
          and from equation (4) that


                                      e i  x   i   e ' j  x   ' j   e ,        ...(9)
                                                    '
                                                    k
                                         x' k  dx ' k
          since x/x  =  , and from equations (8) and (9) that
                    k
                j
                       jk
                                           '
                                          e  a e ,                               ...(10)
                                           k
                                               ki i
          and
                                                '
                                          e  a e .                               ...(11)
                                           i
                                              ki k
          Equations (10) and (11) are the transformation rules for base vectors. The nine elements of a  are
                                                                                   ij
          not all independent, and in general,
                                             a   a .
                                                  ik
                                              ki
          A relation similar to equations (5) and (7),
                                     '
                                    u   a u , and u  a u ' k                    ...(12)
                                         ki
                                      k
                                                 i
                                                     ki
                                           i
                                           '
                                         '
          is obtained for a vector u since  u e  u e ,  which is similar to equation (4) except that the ui are
                                           k
                                         k
                                    i i
          the components of a vector and the x  are coordinates of a point.
                                        i
          The magnitude |u| = (u u )  of the vector u is independent of the orientation of the coordinate
                                1/2
                               i
                              i
          system, that is, it is a scalar invariant; consequently,
                                             '
                                                    '
                                      u u  =  u  a a u .                         ...(13)
                                                    k
                                                ki
                                             k
                                                  ji
                                         i
                                       i
          Eliminating u  from equation (12) gives
                     i
                                             '
                                                    '
                                           u  a a u ,
                                             k
                                                ki
                                                    j
                                                  ji
                         '
                    '
          and since  u   kj u ,
                         j
                    k
                                          a a  =  .                              ...(14)
                                           ki ji
                                                kj
          Similarly, eliminating u  from equation (12) gives
                             k
                                          a a  =  .                              ...(15)
                                           ik jk
                                                 ij
          It follows from equation (14) or (15) that
                                         {det[a ]}  = 1,                          ...(16)
                                               2
                                             ij
          where det [a ] denotes the determinant of a . The negative root of equation (16) is not considered
                    ij
                                            ij
          unless  the  transformation  of  axes  involves a  change  of  orientation  since,  for the  identity
          transformation x  =  x ,   a   =     and  det[ ]  =  1. Consequently,  det[a ]  = 1,  provided  the
                            '
                             i
                                    ik
                                                                     ik
                                              ik
                        i
                                ik
          transformations involve only right-handed systems (or left-handed systems).
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