Page 175 - Engineering Electromagnetics, 8th Edition
P. 175

CHAPTER 6  Capacitance              157













                                        Figure 6.7 The remaining of the
                                        streamlines have been added to
                                        Fig. 6.6b by beginning each new line
                                        normally to the conductor and
                                        maintaining curvilinear squares
                                        throughout the sketch.

                         The simplest ratio we can use is unity, and the streamline from B to B shown in

                     Figure 6.6b was started at a point for which  L t =  L N . Because the ratio of these
                     distances is kept at unity, the streamlines and equipotentials divide the field-containing
                     region into curvilinear squares, a term implying a planar geometric figure that differs
                     from a true square in having slightly curved and slightly unequal sides but which
                     approaches a square as its dimensions decrease. Those incremental surface elements
                     in our three coordinate systems which are planar may also be drawn as curvilinear
                     squares.
                         We may now sketch in the remainder of the streamlines by keeping each small
                     box as square as possible. One streamline is begun, an equipotential line is roughed
                     in, another streamline is added, forming a curvilinear square, and the map is gradually
                     extended throughout the desired region. The complete sketch is shown in Figure 6.7.
                         The construction of a useful field map is an art; the science merely furnishes
                     the rules. Proficiency in any art requires practice. A good problem for beginners is
                     the coaxial cable or coaxial capacitor, since all the equipotentials are circles while the
                     flux lines are straight lines. The next sketch attempted should be two parallel circular
                     conductors, where the equipotentials are again circles but with different centers. Each
                     of these is given as a problem at the end of the chapter.
                         Figure 6.8 shows a completed map for a cable containing a square inner conductor
                     surrounded by a circular conductor. The capacitance is found from C = Q/V 0 by
                     replacing Q by N Q  Q = N Q   , where N Q is the number of flux tubes joining
                     the two conductors, and letting V 0 = N V  V, where N V is the number of potential
                     increments between conductors,

                                                      N Q  Q
                                                 C =
                                                      N V  V
                     and then using Eq. (19),

                                                 N Q   L t    N Q
                                             C =          =                          (20)
                                                 N V  L N     N V
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