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an investigation of dual stator winding induction machines

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In section 10.2, the fundamentals <strong>of</strong> vector control <strong>an</strong>d indirect rotor flux orientation<br />

control are introduced based on the <strong>induction</strong> machine dynamic model. Then the<br />

derivation <strong>of</strong> the indirect rotor flux orientation control scheme is presented in section<br />

10.3. The design methods for current controllers, flux controller <strong>an</strong>d speed controller are<br />

discussed in section 10.4. In section 10.5, computer simulation results <strong>of</strong> indirect rotor<br />

flux orientation control <strong>of</strong> the <strong>dual</strong> <strong>stator</strong> <strong>winding</strong> <strong>induction</strong> machine are shown. Full-<br />

order flux observer design <strong>an</strong>d determination <strong>of</strong> observer gains are the topics <strong>of</strong> section<br />

10.6 <strong>an</strong>d 10.7 respectively. The sensorless control scheme uses a flux observer <strong>an</strong>d a<br />

speed estimator instead <strong>of</strong> the encoder. The methodology for properly choosing the<br />

observer gains is presented in section 10.7. A brief introduction <strong>of</strong> D-decomposition<br />

method is given in section 10.8. Controller design methods for the speed estimator is the<br />

topic <strong>of</strong> section 10.9. The speed controller design method is described in section 10.10.<br />

Finally, the simulation results for sensorless control are given in section 10.11 <strong>an</strong>d<br />

conclusions c<strong>an</strong> be found in section 10.12.<br />

10.2 Indirect Flux Orientation Control<br />

The original idea <strong>of</strong> vector control for <strong>induction</strong> <strong>machines</strong> comes from the model <strong>of</strong><br />

dc <strong>machines</strong>. In the dc machine, the electromagnetic torque results from the interaction<br />

between excitation field <strong>an</strong>d armature current, which c<strong>an</strong> be controlled independently.<br />

The excitation field is the result <strong>of</strong> field current or a perm<strong>an</strong>ent magnet. The torque<br />

equation <strong>of</strong> dc <strong>machines</strong> is given as:<br />

P<br />

Te = λaf<br />

ia<br />

(10.1)<br />

2<br />

343

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