Page 396 - Power Electronics Handbook
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Electrical machine control   385

























                                                         structure



        Figure 14.36 Magnetic position sensor



        amplification. However, the induced signals in the coils build up gradually,
        this giving slower turn-on and greater dissipation in the switches, as well as
        possible uncertainty in the exact switching point. The presence of  leakage
        flux also means that there is always some induced signal in the coils. Since
        all signals are a.c. they have usually to be rectified before being used to
        operate the switches.
          Optical sensors are generally less robust than magnetic systems but are
        also much smaller and lighter. They have therefore tended to be used in
        motors  for  special applications such  as  aerospace.  Figure  14.37 shows a
        schematic of  an optical system where  a light shield with  an  aperture is
        connected  to  the  rotor  and  revolves around  a  stationary  light  source.
        Photocells  placed  at  the  four  switch  points  detect  the  commutation
        positions for the motor, as before. Generally, the output signals from the
        light detectors are weak and need further amplification before they can be
        used to operate the stator switches. However, the signals can be made to
        rise sharply and since they are generally d.c.  no rectification is required.
          A  sensor  which  has  been  extensively used  in  many  small electronic
        commutator motors is the Hall effect device. It combines the robustness of
        magnetic sensors with the lightness of  optical devices. The Hall effect is
        well known. A current I, passed between the two faces of a thin conductor
        or a semiconductor placed in a transverse magnetic field B would result in a
        redistribution  of  charge carriers  within the  device and  induce  a voltage
        across  it  in  a  direction  perpendicular  to  both  the  current  flow  and  the
        magnetic field. This voltage, known as the Hall voltage, is proportional to
        Z,  and B.
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