Page 102 - Servo Motors and Industrial Control Theory -
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5.3   Torque–Displacement Characteristic of a Stepping Motor    95

                        torque due to phase
                                                    Resultant torque
                  cw
                 torque

                                                   Torque due to phase 2
             ccw rotor                                               cw rotor
            displacement                                             displacement




                  ccw                 ¼ rotor  ¼ rotor
                 torque               tooth    tooth
                                      pitch    pitch


                          180      90       0        90      180
                                     Rotor position, θ, deg.
            Fig. 5.6   Torque–displacement characteristic of generalized stepping motor



                                     T: =nKI sin( )⋅⋅  θ                  (5.1)
                                             1
                                      m      t
            In equation (5.1), n is number of phases energized, T  is the developed torque,  K
                                                                             1
                                                      m
                                                                             t
            is motor torque constant, I is the current which may be written as
                                        I: =  N RT  φ ⋅                   (5.2)

            where N , φ are numbers of rotor teeth and step angle. For a specific motor,  nK,  1 t
                   RT
            are constants and Eq. (5.1) may be written as
                                      T : =  K I sin()⋅ ⋅  θ              (5.3)
                                            2
                                       m    t
            where  K  is constant and I is the current flowing in the stator windings and θ is
                   2
                   t
            the rotor position. Equation (5.3) is nonlinear and to study the dynamic behavior of
            stepping motors, it must be linearized as
                                     T: =  K I K   ⋅ −  θ ⋅θ              (5.4)
                                      m
                                            t
            where

                          K : =  d  T  θ=         K : =  K sin( )⋅  θ     (5.5)
                                                         2
                                       : constant
                            t
                                dI  m               t    t
                               d
                         K : =  dθ  T m  I : constant K : = K ⋅⋅          (5.6)
                                                        2
                                       =
                                                          I cos( ) θ
                                                   θ
                           θ
                                                        t
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