Page 435 - Electromagnetics
P. 435

c ˜
                                                     ˜
                        Finally, using Ampere’s law ∇× H = jω˜  E in the source free region V , and taking the
                        curl in the first term outside the integral, we have
                                     N                                N
                            ˜                       1       ˜                       ˜
                            E(r,ω) =   ∇× ∇×           (ˆ n × H)GdS +   ∇×     (ˆ n × E)GdS .  (6.37)
                                                   jω˜  c
                                    n=1         S n                  n=1     S n
                        Similarly
                                      N                                N
                           ˜                         1       ˜                       ˜
                           H(r,ω) =−     ∇× ∇×          (ˆ n × E)GdS +   ∇×    (ˆ n × H)GdS .  (6.38)
                                                    jω ˜µ
                                      n=1         S n                 n=1     S n
                        These expressions together constitute the Franz formula for the vector Huygens principle
                        [192].

                        6.3.3   Love’s equivalence principle

                          Love’s equivalence principle allows us to identify the equivalent Huygens sources for the
                        fields within a bounded, source-free region V . It then allows us to replace a problem in
                        the bounded region with an “equivalent” problem in unbounded space where the source-
                        excluding surfaces are replaced by equivalent sources. The field produced by both the
                        real and the equivalent sources gives a field in V identical to that of the original problem.
                        This is particularly useful since we know how to compute the fields within an unbounded
                        region by employing potential functions.
                          We identify the equivalent sources by considering the electric and magnetic Hertzian
                        potentials produced by electric and magnetic current sources. Consider an impressed
                                                                               eq
                                                                              ˜
                                              eq
                                             ˜
                        electric surface current J s and a magnetic surface current J ms flowing on the closed
                        surface S in a homogeneous, isotropic medium with permeability ˜µ(ω) and complex
                                    c
                        permittivity ˜  (ω). These sources produce
                                                           eq
                                                          ˜

                                                           J s (r ,ω)
                                              ˜
                                              Π e (r,ω) =         G(r|r ; ω) dS ,              (6.39)
                                                              c
                                                         S jω˜  (ω)
                                                           ˜ eq
                                                          J ms (r ,ω)
                                              ˜
                                             Π h (r,ω) =          G(r|r ; ω) dS ,              (6.40)
                                                         S jω ˜µ(ω)
                        which in turn can be used to find
                                                                          ˜
                                                             ˜
                                                ˜
                                               E =∇ × (∇× Π e ) − jω ˜µ∇× Π h ,
                                               ˜
                                                                          ˜
                                                            ˜
                                                       c
                                               H = jω˜  ∇× Π e +∇ × (∇× Π h ).
                        Upon substitution we find that

                                    ˜                    1    ˜ eq              ˜ eq
                                    E(r,ω) =∇ × ∇ ×         J G dS +∇ ×      [−J ]GdS ,
                                                                                ms
                                                             s
                                                      S jω˜  c              S

                                    ˜                     1    ˜ eq              ˜ eq
                                   H(r,ω) =−∇ × ∇ ×           −J G dS +∇ ×       J GdS .
                                                                ms
                                                                                  s
                                                       S jω ˜µ                 S
                        These are identical to the Franz equations (6.37) and (6.38) if we identify
                                                                          ˜
                                                         ˜
                                                J ˜ eq  = ˆ n × H,  J ˜ eq  =−ˆ n × E.         (6.41)
                                                 s
                                                                ms
                        These are the equivalent source densities for the Huygens principle.
                        © 2001 by CRC Press LLC
   430   431   432   433   434   435   436   437   438   439   440