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AN2388 Datasheet(PDF) 14 Page - STMicroelectronics |
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AN2388 Datasheet(HTML) 14 Page - STMicroelectronics |
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14 / 54 page ![]() Vector control of AC induction machines AN2388 14/54 2.3 Block diagram of the vector control The basic scheme of torque control with IFOC is shown below: Figure 11. Block diagram of I.F.O.C. Two phase currents go into some transformation module (Clarke and Park). The projection outputs of the Clark block are indicated with isα and isβ. These two components of the current provide the input of the Park transformation that gives the current in the d,q rotating reference frame aligned with the rotor flux vector. The exact rotor flux angular position (θλr) is necessary to calculate the two components ids and iqs. The ids and iqs components are compared to the references idref (the flux reference) and iqref (the torque reference). The torque command iqref is the output of the speed regulator. The flux command idref indicates the right rotor flux command for every speed reference within the nominal value. The current regulator outputs are Vdref and Vqref . They are processed into the inverse Park transformation. The outputs of this are Vαref and Vβref, which are the components of the stator vector voltage in the α,β orthogonal reference frame. These are the inputs of the Space Vector PWM. The outputs of this block are the gate signals that drive the inverter. The main block of the vector control is the Current Model block. This block needs the rotor resistance and rotor inductance as parameters and knowledge of these, with the highest accuracy, greatly affects the performance of the control. 2.4 The current model (rotor flux estimator) Knowledge of the rotor flux space vector magnitude and position are key for the AC induction motor vector control. Knowing the rotor magnetic angular position allows to establish, in fact, the rotational co-ordinate system (d, q). . The current model consists of implementing the following two equations of the motor in the d-q reference frame: b mR r qs r b s mR mR r ds i T i n dt d f i dt di T i ω θ ω λ + = = + = 1 |
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