Page 478 - Engineering Electromagnetics, 8th Edition
P. 478

460                ENGINEERING ELECTROMAGNETICS

                                     Finally, using the capacitance and the external inductance expressions, we obtain a
                                     value for the characteristic impedance,

                                                              L ext  1  µ     −1
                                                        Z 0 =     =       cosh (d/2a)                (24)
                                                               C     π
                                     13.1.5 Two-Wire (Low Frequencies)
                                     At low frequencies where a uniform current distribution may be assumed, we again
                                     must modify the L and R expressions, but not those for C and G. The latter two are
                                     again expressed by (20) and (22):
                                                                       π
                                                               C =
                                                                       −1
                                                                   cosh (d/2a)
                                                                       πσ
                                                              G =
                                                                       −1
                                                                   cosh (d/2a)
                                     The inductance per unit length must be increased by twice the internal inductance of
                                     a straight round wire,
                                                               µ 1

                                                                         −1
                                                           L =      + cosh (d/2a)                    (25)
                                                               π 4
                                     The resistance becomes twice the dc resistance of a wire of radius a, conductivity σ c ,
                                     and unit length:
                                                                        2
                                                                  R =   2                            (26)
                                                                      πa σ c
                                        D13.3. The conductors of a two-wire transmission line each have a radius of
                                                                      7
                                        0.8 mm and a conductivity of 3 × 10 S/m. They are separated by a center-to-

                                        center distance of 0.8 cm in a medium for which   = 2.5,µ r = 1, and σ =
                                                                                 r
                                        4×10 −9  S/m. If the line operates at 60 Hz, find: (a) δ;(b) C;(c) G;(d) L;(e) R.
                                        Ans. 1.2 cm; 30 pF/m; 5.5 nS/m; 1.02 µH/m; 0.033 	/m


                                     13.1.6 Microstrip Line (Low Frequencies)
                                     Microstrip line is one example of a class of configurations involving planar conduc-
                                     tors of finite widths on or within dielectric substrates; they are usually employed
                                     as device interconnects for microelectronic circuitry. The microstrip configuration,
                                     shown in Figure 13.5, consists of a dielectric (assumed lossless) of thickness d and of
                                     permittivity   =   r   0 , sandwiched between a conducting ground plane and a narrow

                                     conducting strip of width w. The region above the top strip is air (assumed here) or
                                     a dielectric of lower permittivity.
                                        The structure approaches the case of the parallel-plate line if w   d. In a
                                     microstrip, such an assumption is generally not valid, and so significant charge den-
                                     sities exist on both surfaces of the upper conductor. The resulting electric field, origi-
                                     nating at the top conductor and terminating on the bottom conductor, will exist within
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