Page 283 - Engineering Electromagnetics, 8th Edition
P. 283

CHAPTER 8   Magnetic Forces, Materials, and Inductance    265

























                                 Figure 8.14 A portion of a coil showing partial flux
                                 linkages. The total flux linkages are obtained by adding
                                 the fluxes linking each turn.

                     flux at the mean radius times the total number of turns. In order to obtain the total
                     flux linkages we must look at the coil on a turn-by-turn basis.

                                    (N ) total =   1 +   2 + ··· +   i + ··· +   N
                                               N

                                            =      i
                                              i=1
                     where   i is the flux linking the ith turn. Rather than doing this, we usually rely on
                     experience and empirical quantities called winding factors and pitch factors to adjust
                     the basic formula to apply to the real physical world.
                         An equivalent definition for inductance may be made using an energy point
                     of view,

                                                       2W H
                                                  L =                                (52)
                                                        I 2
                     where I is the total current flowing in the closed path and W H is the energy in the
                     magnetic field produced by the current. After using (52) to obtain several other general
                     expressions for inductance, we will show that it is equivalent to (49). We first express
                     the potential energy W H in terms of the magnetic fields,

                                                       B · H dν
                                                     vol                             (53)
                                               L =
                                                        I 2
                     and then replace B by ∇× A,
                                                1
                                            L =       H · (∇× A)dν
                                                I 2  vol
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