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2/6  Electrical and electronics principles
                                                    e = N(di#J/dt)                         (2.25)
                                                    where e is the instantaneous  induced e.m.f.
                                                      Equation  (2.25)  forms  the  basis  of  all  electrical  power
                                                    generation  machines  and  is  a  statement  of  the  fact  that  an
                                                    electric current can be produced by the movement of magnetic
                                                    flux relative to a coil. In all rotating electrical generators it is
                                                    actually the coil which is moved relative to the magnetic field.
                                                    The net result, however, is exactly the same.
                                                      The direction  of  the induced  emf. is always such that  it
                                                    tends to set up a current to oppose the motion (or the change
                                                    of  magnetic  flux)  which  was  responsible  for  inducing  the
                                                    e.m.f. This is essentially a statement  of  Lenz’s law. In many
                                                    texts, therefore, the right-hand side of equation (2.25) is often
                                    Area a          shown as a negative quantity.
                                                      The  motion,  or  change  of  flux,  is  associated  with  the
                                                    application  of  a mechanical  force  which ultimately  provides
                                                    the torque required to drive the electric generator.  Figure 2.6
                                                    shows  a  single  conductor  of  length  1 metres,  carrying  an
                                                    induced current I  and lying perpendicular  to a magnetic field
      Figure 2.4  Toroid                            of  flux density, B T.
                                                      The force applied causes the conductor to move through  a
       The group (pull) is termed the permeance and the inverse of   distance  dx metres.  The mechanical  work  done is therefore
      permeance  is the reluctance,  S. Thus equation (2.20) may be   F. dx. The electrical energy produced is given as the product
      rewritten  as                                  of  the power developed and the time duration, i.e. e . I. dt.
      i#J  = FIS                             (2.22)
      Equation  (2.22)  represents  an  electromagnetic  version  of
      Ohm’s law.
       Alternatively,  equation (2.20) can be expressed as
      _- i#JF
        - PT
      or
      B  = pH                                (2.23)
      where B  = i#J/u is the magnetic flux density (in webers/m2, or
      Tesla (T)) and H  = F/l is the magnetic intensity  (in Nm).

      2.1.13  Permeability
      The permeability  of  free  space,  PO, is  numerically  equal  to
      4a x  lo-’.  The absolute  permeability  of  other  materials  is
      related  to  the  permeability  of  free  space  by  the  relative
      permeability,  i.e.
      P  = Po  ‘ PLr                         (2.24)
        For  air  and  other  non-magnetic  materials,  the  absolute
      permeability  is  the  same  constant.  For  magnetic  materials,
      absolute permeability is not a fixed constant but varies non-
      linearly  with  the  flux  density.  The  non-linear  variation  of
      permeability is conveniently displayed as a functional plot of
      magnetic flux density, B, against magnetic intensity, H. Figure
      2.5  illustrates  a  number  of  B-H  curves  for  some  common
      materials.
        Also shown in Figure 2.5 is the B-H  curve for air, the only
      straight-line relationship in the diagram. It is apparent that for
      an applied magnetic intensity, the magnetic flux developed in
      a  coil  with  a  ferrous  core  is  many  times  greater  than  that
      through  a  similar  coil  with  an  air  core.  In  most  practical
      systems, therefore,  a ferrous  core is normally  used,  since it
      greatly facilitates the establishment of  a magnetic flux.

      2.1.14  Faraday’s law                                              5000            10 000
      Faraday’s  law  states that  the  e.m.f.  induced  in  a  magnetic   Magnetic intensity H (A/rn)
      circuit  is equal to the rate  of  change of  flux linkages  in the
      circuit, and is given as                       Figure 2.5  6-H  curves for some common materials
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