Page 21 - Introduction to Continuum Mechanics
P. 21

6 indicia! Notation




        representing








                                                                  '
        We note that x j = a jmx m , j= 1,2,3, is the same as Eq. (2A2.3) and e j  = Q mje m, j=1,2,3 is the
        same as Eq. (2A2.4). However,

                                             a i = b j
        is a meaningless equation. The free index appearing in every term of an equation must be the
        same. Thus the following equations are meaningful
                                           a i + k i = c i
                                        a i + b ic jd j = 0
        If there are two free indices appearing in an equation such as



        then the equation is a short-hand writing of 9 equations; each has a sum of 3 terms on the
        right-hand side. In fact,
                             T 11 = A 1mA 1m = A 11A 11 + A 12 A 12 +A 13 A l3

                             T 12 =A 1mA 2m =A 11A 21 +A 12A 22 +A 13A 23
                             T 13 = A 1mA 3m = A 11A 31 + A 12A 32 + A 13A 33




                                                    +
                             T 33 = A 3mA 3m = A 31A 31  A 32A 32 + A 33A 33
        Again, equations such as
                                            T ij = T ik
        have no meaning,


        2A3 Kronecker Delta
          The Kronecker delta, denoted by d ij, is defined as




          That is,
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