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652    CHAPTER 18  The Potential Equation

                                 18.5.2  The Right Quarter-Plane
                                 The right quarter-plane has the nonnegative horizontal and vertical axes as boundary. The
                                 Dirichlet problem for this region is
                                                            2
                                                          ∇ u(x, y) = 0for x > 0, y > 0,
                                                             u(x,0) = f (x) for x ≥ 0,

                                 and
                                                             u(0, y) = g(y) for y ≥ 0.
                                    This problem can be treated by solving separately the cases that either f (x) or g(y) is iden-
                                 tically zero. Separation of variables applies to both cases, and the solution of the given problem
                                 is the sum of the solutions of these simpler problems.
                                    We will demonstrate a different method for the case that g(y) = 0. Notice that if we fold
                                 the upper half-plane across the vertical axis we obtain the right quarter-plane. This suggests that
                                 we might be able to use the solution for the upper half-plane to solve the problem for the right
                                 quarter-plane. To do this, let

                                                                   f (x)   for x ≥ 0
                                                           w(x) =
                                                                  anything  for x < 0.
                                 where by “anything” we mean we will fill in this part shortly. We now have a Dirichlet problem
                                 for the upper half-plane with the data function u(x,0) = w(x). We know the solution u hp of this
                                 problem for the upper half-plane:
                                                                  y     ∞  w(ξ)
                                                        u hp (x, y) =              dξ.
                                                                  π  −∞ y + (ξ − x) 2
                                                                         2
                                 Write this as
                                                       y      0  w(ξ)           ∞   w(ξ)
                                             u hp (x, y) =               dξ +               dξ .
                                                               2
                                                                                  2
                                                       π   −∞ y + (ξ − x) 2   0  y + (ξ − x) 2
                                 Change variables in the first integral on the right by letting ζ =−ξ:
                                                         w(ξ)               w(−ζ)
                                                     0                   ∞
                                                                 dξ =               (−1)dζ.
                                                                           2
                                                       2
                                                   −∞ y + (ξ − x) 2    0  y + (ζ + x) 2
                                 For uniformity in notation, replace the dummy variable of integration on the right with ξ to write
                                                      y      0  w(−ξ)             ∞   w(ξ)
                                            u hp (x, y) =              (−1)dξ +               dξ
                                                                                    2
                                                             2
                                                      π   ∞ y + (ξ + x) 2       0  y + (ξ − x) 2
                                                      y     ∞     w(−ξ)       f (ξ)
                                                   =                    +              dξ.
                                                              2
                                                                           2
                                                      π  0   y + (ξ + x) 2  y + (ξ − x) 2
                                 In the last integral, we used the fact that w(ξ) = f (ξ) for ξ ≥ 0. Now fill in the “anything” in the
                                 definition of w. Notice that the last integral will vanish at points (0, y) on the positive y-axis if
                                 f (ξ) + w(−ξ) = 0for ξ ≥ 0. This will occur if w(−ξ) =− f (ξ).Make w the odd extension of
                                 f to the entire line. In this way, we obtain the solution for the upper half-plane:
                                                        y     ∞     1            1
                                              u hp (x, y) =               −              f (ξ)dξ.
                                                                             2
                                                        π  0   y + (ξ − x) 2  y + (ξ + x) 2
                                                                2
                                 But this function is also harmonic on the right quarter-plane, vanishes when x = 0, and equals
                                 f (x) if x ≥ 0 and y = 0. Therefore, this function is also the solution of the problem for the right
                                 quarter-plane (in this case of zero data along the positive y-axis).



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