Page 267 - Schaum's Outline of Theory and Problems of Advanced Calculus
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258       LINE INTEGRALS, SURFACE INTEGRALS, AND INTEGRAL THEOREMS        [CHAP. 10


                                          ðð
                              ðð
                                              @ðx; yÞ
                          (b)   dx dy and          du dv represent the area of region r,the first expressed in rectangular

                                            @ðu; vÞ
                               r          r  0
                              coordinates, the second in curvilinear coordinates.  See Page 212, and the introduction of the differ-
                              ential element of surface area for an alternative to Part (a).
                                   yi þ xj                               þ
                                        .  (a) Calculate r  F:  ðbÞ Evaluate  F   dr around any closed path and
                                  x þ y
                     10.33. Let F ¼  2  2
                          explain the results.

                                        i      j
                                                   k
                                        @     @

                                                   @

                                        @x    @y        ¼ 0 in any region excluding ð0; 0Þ:
                          ðaÞ  r   F ¼
                                                   @z
                                        y     x


                                     x þ y  x þ y
                                        2  2  2  2  0
                                       ydx þ xdy
                              þ      þ
                          (b)  F   dr ¼        .  Let x ¼   cos  ; y ¼   sin  , where ð ;  Þ are polar coordinates.  Then
                                         2
                                        x þ y 2
                                            dx ¼   sin   d  þ d  cos  ;  dy ¼   cos   d  þ d  sin
                                                      ydx þ xdy            y
                              and so                          ¼ d  ¼ d arc tan
                                                        2
                                                       x þ y 2             x
                                 For a closed curve ABCDA [see Fig. 10-22(a)below] surrounding the origin,   ¼ 0at A and   ¼ 2
                                                                                  ð 2
                              after a complete circuit back to A.  Inthis case the line integral equals  d  ¼ 2 .
                                                                                   0
                                              y                             y
                                                                              Q
                                                  B
                                                                                            P
                                       C
                                                 φ       A
                                                             x
                                            O                                  φ
                                                                                           S
                                                                                      R
                                                                                 φ 0
                                         D                                                       x
                                                                          O
                                                (a)                                 (b)
                                                              Fig. 10-22
                                 For a closed curve PQRSP [see Fig. 10-22(b) above] not surrounding the origin,   ¼   0 at P and
                                                                                        ð
                                                                                          0
                                ¼   0 after a complete circuit back to P.  Inthis case the line integral equals  d  ¼ 0.
                                                                                          0
                                 Since F ¼ Pi þ Qj; r  F ¼ 0 is equivalent to @P=@y ¼ @Q=@x and the results would seem to con-
                                                                                        y           x
                              tradict those of Problem 10.11. However, no contradiction exists since P ¼  2  2  and Q ¼  2  2
                                                                                      x þ y       x þ y
                              do not have continuous derivatives throughout any region including ð0; 0Þ, and this was assumed in
                              Problem 10.11.
                     10.34. If div A denotes the divergence of a vector field A at a point P, show that
                                                                  ðð
                                                                     A   n dS
                                                                   s
                                                       div A ¼ lim
                                                               V!0    V
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