Page 270 - Engineering Electromagnetics, 8th Edition
P. 270

252                ENGINEERING ELECTROMAGNETICS

                                     values of µ r would range from 10 to 100, 000. Diamagnetic, paramagnetic, and
                                     antiferromagnetic materials are commonly said to be nonmagnetic.


                                        D8.6. Find the magnetization in a magnetic material where: (a) µ = 1.8 ×
                                                                                                  3
                                                                                         28
                                        10 −5  H/m and H = 120 A/m; (b) µ r = 22, there are 8.3 × 10 atoms/m , and
                                                                                    2
                                        each atom has a dipole moment of 4.5 × 10 −27  A · m ;(c) B = 300 µT and
                                        χ m = 15.
                                        Ans. 1599 A/m; 374 A/m; 224 A/m


                                        D8.7. The magnetization in a magnetic material for which χ m = 8isgivenin
                                                           2
                                        a certain region as 150z a x A/m. At z = 4 cm, find the magnitude of: (a) J T ;
                                        (b)J;(c) J B .
                                                    2
                                                            2
                                        Ans. 13.5 A/m ; 1.5 A/m ;12A/m 2

                                     8.7 MAGNETIC BOUNDARY CONDITIONS
                                     We should have no difficulty in arriving at the proper boundary conditions to apply to
                                     B, H, and M at the interface between two different magnetic materials, for we have
                                     solved similar problems for both conducting materials and dielectrics. We need no
                                     new techniques.
                                        Figure 8.10 shows a boundary between two isotropic homogeneous linear materi-
                                     als with permeabilities µ 1 and µ 2 . The boundary condition on the normal components






















                                             Figure 8.10 A gaussian surface and a closed path are
                                             constructed at the boundary between media 1 and 2, having
                                             permeabilities of µ 1 and µ 2 ,respectively. From this we determine the
                                             boundary conditions B N1 = B N2 and H t1 − H t2 = K , the component
                                             of the surface current density directed into the page.
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