Page 665 - Mechatronics with Experiments
P. 665

ELECTRIC ACTUATORS: MOTOR AND DRIVE TECHNOLOGY  651
                             ground voltage. In order to eliminate this problem, when H-bridges are controlled (i.e.,
                             by a microcontroller), either in software or hardware, a dead time (or delay) is introduced
                             between the ON to OFF command to one transistor and OFF to ON command to the other
                             transistor (this one is delayed in microsecond range) in order to avoid a short circuit. Most
                             microcontrollers have PWM output peripheral where this delay is programmable by writing
                             to a setup register associated with the PWM output channel.
                                  If the top two transistors are both turned ON and the bottom two are turned OFF (or
                             the reverse; top two transistors are OFF, bottom two transistors are ON), the terminals of the
                             motor winding are effectively shorted without connection to the power supply, V (t) = 0.0.
                                                                                             t
                             This results in the so-called dynamic braking.
                                                                   d  (t)
                                                     V (t) = R ⋅ i(t) +                        (8.177)
                                                       t
                                                                    dt
                                                                      di(t)
                                                                               ̇
                                                        0 = R ⋅ i(t) + L ⋅  + k ⋅   (t)        (8.178)
                                                                             e
                                                                       dt
                                                                    di(t)
                                                       ̇
                                                 − k ⋅   (t) = R ⋅ i(t) + L                    (8.179)
                                                    e
                                                                     dt
                             Due to the back EMF voltage, there will be a current developed in the motor winding
                             (hence torque) in the opposite direction to the rotation speed. As a result, it will brake
                             (slow down) the motion. The generated current is approximately proportional to the speed,
                             hence the dynamic braking torque is large at high speeds and small at low speeds. One of
                             the transistors and the diode on the other side provides the conductive path. Let us assume
                             the top two transistors were turned ON, and the bottom two were OFF. Then for CW motion
                             of the motor, Q1 transistor and D2 diode provide the conductive path for current flow from
                             left to right across the motor. For CCW direction, Q2 diode and D1 transistor provide the
                             conductive path for current flow from right to left (opposite). Similar behavior occurs if the
                             bottom two transistors were ON and the top two transistors were OFF.
                                  By controlling the current magnitude through the power transistors, the magnitude
                             of the torque is controlled. In very small size motors (fractional horsepower), linearly
                             operated transistor amplifiers are used. The pulse width modulation (PWM) circuit operates
                             the transistors in all ON or all OFF modes in order to increase the efficiency. The linear
                             amplifiers provide lower noise but are less efficient than the PWM amplifiers. The most
                             important difference between the linear mode and PWM mode of operating the power
                             transistors is the efficiency. Power loss at the transistor is approximately the voltage drop
                             across the transistor times the current it conducts,

                                                           P loss  = V CE  ⋅ i CE              (8.180)

                             In the linear mode of operation, that is 50% turned ON, the voltage V  across the transistor
                                                                                   CE
                             will be 50% of the supply voltage and the current will be the equal to the current amplification
                             gain of the transistor (between the base current and output current). Both values are finite
                             values, and there is significant power loss across the power transistor in linear operating
                             mode. In PWM mode, the transistors are always in one of two states: fully ON or fully
                             OFF. When the transistor is fully ON, voltage drop across the transistor is almost zero,
                             V   ≈ 0.0, hence P  = 0. When the transistor is fully OFF, the i  is almost zero, hence
                               CE            loss                                 CE
                             hence P loss  = 0. As a result, the PWM mode of operation of a transistor results in much
                             less power loss than the linear mode of operation. The only drawback of the PWM mode
                             of operation compared to linear mode of operation is that in PWM mode there will be
                             more noise in the current due to the switching frequency. Typical switching frequencies
                             for the PWM mode of operation for power transistors is in the range of 2–20 kHz. The
                             PWM switching frequency should be significantly larger than the desired current control
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