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book   Mobk070    March 22, 2007  11:7








                                     COMPLEX VARIABLES AND THE LAPLACE INVERSION INTEGRAL           117
                                                   y
                                                  1                B

                                                                   A
                                                   0
                                                                            x
                                                           1      2



                   FIGURE 7.5: Integration of an analytic function along two paths



                   in two dimensions. We mention here that it is also important in the study of incompressible,
                   inviscid fluid mechanics and in other areas of science and engineering. You will undoubtedly
                   meet with it in some of you clurses.

                   Example 7.4.

                                                   f = z 2  f = 2z


                                                   f = sin z  f = cos z
                                                   f = e az  f = ae az



                   Integrals
                   Consider the line integral along a curve C defined as x = 2y from the origin to the point
                   x = 2, y = 1, path OB in Fig. 7.5.


                                                            2
                                                           z dz
                                                         C

                        We can write

                                                                    2
                                                                          2
                                                  2
                                             2
                                                       2
                                            z = x − y + 2ixy = 3y + 4y i
                   and dz = (2 + i)dy
                        Thus
                                 1                                      1
                                                                                  2   11

                                                                           2
                                           2
                                      2
                                  (3y + 4y i)(2 + i)dy = (3 + 4i)(2 + i)  y dy =   +    i
                                                                                  3   3
                               y=0                                    y=0
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