Page 654 - Mechatronics with Experiments
P. 654

640   MECHATRONICS
                                   The complete electromechanical dynamic model of this actuator can be written as
                                                                      (      )
                                                       di(t)            dL(x )      dx (t)
                                                                           g
                                                                                      g
                                             V(t) = L(x )   + R coil  i(t) +   ⋅ i(t) ⋅         (8.167)
                                                     g
                                                        dt               dx g         dt
                                                             2
                                                    1       N A x    2
                                                          o
                                          F(x , i) =−               ⋅ i                         (8.168)
                                             g
                                                    2  (         ) 2
                                                        x +  A x  y g
                                                        g
                                                            2 A y
                                                       2
                                                     d x (t)
                                                        g
                                          F(x , i) = m p    + k spring  ⋅ x (t)                 (8.169)
                                                                     g
                                             g
                                                       dt 2
                              where
                                                                   N 2
                                                    L(x ) =    (        ) A                     (8.170)
                                                       g    o               x
                                                               x +  A x  y g
                                                                g
                                                                   2 A y
                                                   dL(x )              2
                                                       g             N
                                                         =−   ⋅              ⋅ A                (8.171)
                                                    dx        0 (         ) 2   x
                                                      g
                                                                  x +  A x  y g
                                                                  g
                                                                      2A y
                              In order to simulate this solenoid, we need the following:
                                  Parameters:    , N, A , A , y , m , k spring , R coil .

                                                           p
                                                        g
                                                      y
                                             0
                                                   x
                                  Initial conditions: i(t ), x (t ), ̇ x (t ).

                                                           g 0
                                                      g 0
                                                   0
                                  Variables of interest as simulation output: F(t), x (t), V(t), i(t).

                                                                         g
                       8.4 DC SERVO MOTORS AND DRIVES
                              DC servo motors can be divided into two general categories in terms of their commutation
                              mechanism: (i) brush-type DC motors; (ii) brushless DC motors. The brush-type DC motor
                              has a mechanical brush pair on the motor frame and makes contact with a commutator
                              ring assembly on the rotor in order to commutate the current, that is to switch the current
                              from one winding to another, as a function of rotor position so that the magnetic fields of
                              the rotor and stator are always at a 90 degree angle relative to each other. In brush-type
                              permanent magnet DC motors, the rotor has the coil winding, the stator has the permanent
                              magnets.
                                   The brushless DC motor is an inside-out version of the brush-type DC motor, that
                              is, the rotor has the permanent magnets and the stator has the winding. In order to achieve
                              the same functionality of the brush-type motor, the magnetic fields of the rotor and stator
                              must be perpendicular to each other at all rotor positions. As the rotor rotates, the magnetic
                              field rotates with it. In order to maintain a perpendicular relationship between the rotor
                              and stator magnetic fields, the current in the stator must be controlled as a vector quantity
                              (both magnitude and direction) relative to the rotor position. Control of current to maintain
                              this vector relationships is called commutation. Commutation is done by solid-state power
                              transistors based on a rotor position sensor. Notice that a rotor position sensor is necessary
                              to operate a brushless DC motor, whereas a brush-type DC motor can be operated without
                              any position or velocity sensor as a torque source. When a motor is controlled in conjunction
                              with a position or velocity sensor, it is considered a “servo” motor.
                                   The field magnetics in a brush-type DC motor can be established either by permanent
                              magnets (hence the name permanent magnet DC motor) or electromagnets (hence the
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