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12.7 Lifting Green’s Theorem to R 3  399

                                        is normal to the sphere and oriented outward. This vector has magnitude 2/z, so a unit outer
                                        normal is
                                                                 z     x  y       1
                                                             n =     i + j + k = (xi + yj + zk).
                                                                 2  z    z        2
                                        We need
                                                                           1  2   2   2
                                                                     F · n = (x + y + z ).
                                                                           2
                                        Then
                                                                     1

                                                                                2
                                                                            2
                                                                        2
                                                           flux =      (x + y + z )dσ
                                                                     2


                                                                 1                     x 2  y 2
                                                                                2
                                                                            2
                                                                        2
                                                               =      (x + y + z ) 1 +   +   dA
                                                                 2   D                 z 2  z 2

                                                                 1      2   2   2  x + y + z 2
                                                                                        2
                                                                                    2

                                                               =      (x + y + z )           dA
                                                                 2   D                 z 2
                                                                 1                      1
                                                                                2 3/2
                                                                        2
                                                                            2
                                                               =      (x + y + z )            dA
                                                                 2   D               4 − x − y  2
                                                                                         2

                                                                           1
                                                               = 4               dA.
                                                                            2
                                                                     D  4 − x − y  2
                                                                   2
                                                                       2
                                                               2
                                        Here we used the fact that x + y + z = 4on  . Converting to polar coordinates, we have
                                                                             √
                                                                          2π     3  1
                                                                flux = 4        √      rdr dθ
                                                                        0   0    4 −r 2
                                                                                   √
                                                                               2 1/2  3
                                                                    = 8π[−(4 −r ) ] 0  = 8π.
                               SECTION 12.6        PROBLEMS
                                                                              2
                                                                                               2
                                                                                           2
                                                                                  2
                            In each of Problems 1 through 6, find the mass and center  x + y = 1and x + y = 9, with δ(x, y, z) = xy/

                                                                                   2
                            of mass of the shell  .                           1 + 4x + 4y .
                                                                                        2
                                                                                                        2
                                                                                                    2
                            1.   is a triangle with vertices (1,0,0),(0,3,0) and  5.   is the paraboloid z = 6 − x − y for z ≥ 0, with
                                                                                            2   2
                              (0,0,2), with δ(x, y, z) = xz + 1.             δ(x, y, z) = 1 + 4x + 4y .
                            2.   is the part of the sphere x + y + z = 9 above the  6.   is the part of the sphere of radius 1 about the origin,
                                                   2
                                                       2
                                                           2
                              plane z = 1, and the density function is constant.  lying in the first octant. The density is constant.
                                                     2   2                 7. Find the flux of F = xi + yj − zk across the part of the
                            3.   is the cone z = x + y for x + y ≤9, δ = constant
                                                 2
                                             2
                              = K.                                           plane x + 2y + z = 8 in the first octant.
                                                                 2
                            4.   is the part of the paraboloid z = 16 − x − y 2  8. Find the flux of F = xzi − yk across the part of the
                                                                                       2
                                                                                          2
                                                                                   2
                              in the first octant and between the cylinders   sphere x + y + z = 4 above the plane z = 1.
                            12.7        Lifting Green’s Theorem to R       3
                                        The fundamental results of vector integral calculus are the theorems of Gauss and Stokes. In this
                                        section we will show how both can be viewed as natural generalizations of Green’s theorem from
                                        two to three dimensions.
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                                   October 14, 2010  14:53  THM/NEIL   Page-399        27410_12_ch12_p367-424
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