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7.4 Use the additional magnetic eld intensity terms given in Equation 7.7 to construct the power loss integral of Equation 7.8 and carry out the individual integral terms to produce Equation 7.11. This expression can be applied to the set of Ni = 8 spheres shown in Figure 7.6. In this gure, the spheres all have the same radius ai and are located at a distance xi below the copper trace of width w and length l. The blue lines in the gure relate to the induced current density on the surface of the spheres and on the surface of the trace plane due to the incident electromagnetic wave and the additional amount of current induced in the plane by the nearby magnetic dipole moments. Note that the current density is induced transversely on all conducting surfaces so that the currents seen are a transverse wave of charge that propagates in the direction of the arrows. Note that the spheres in Figure 7.6 are physically located in a geometric hexagonal close-packed (hcp) arrangement. The term (Ni a2/w l) in Equation 7.11 is, i thus, the ratio of the cross-sectional area of the spheres compared with the total area of the trace and the ratio (ai/xi) 1. In the special case of a eld of equal-radius rdlc gs1 128 Packages matching GS1-128 - NuGet Gallery
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