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3.2 Electromagnetic Drive                       71

         Here 0 is calculated from the initial conditions £ = 0,0 = 0 0, and 0 = 0, and has the form









         3.2    Electromagnetic Drive

           An electromagnet used in machine design for drive purposes usually consists of a
         housing 1, a coil 2, an armature 3, and a spring 4, as shown schematically in Figure
         3.10. The armature slides in guides 5, which are made of a nonmagnetic material so
         as to create minimal friction between the armature and the guides. The housing, arma-
         ture, guide bushing, and air gap constitute the magnetic circuit. The coil carries the
         electric circuit.
            In this case the computation includes the determination of the current changes in
         the coil, the magnetic flux in cross sections of the magnetic circuit, the pulling force
         developed by the magnet, the influence of the air gap, and the speed of motion of the
         armature. The initial data for these computations include the geometric dimensions,
         the structure and materials of the magnet, and the parameters of the voltage. These
         computations cannot be completed analytically. The equations are cumbersome, and
         there are no analytical methods of solution for such nonlinear differential equations.
           However, to simplify the equations, the following assumptions may be made:

            • There are no energy losses in the form of eddy current and hysteresis;
            • Reluctance of the air gap is proportional to its length;
            • There is no leakage flux or reluctance in the magnetic circuit.






























        FIGURE 3.10 Layout of an electromagnet.
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