Direct Torque Control with Space Vector Modulation (DTC-SVM) of ...
Direct Torque Control with Space Vector Modulation (DTC-SVM) of ...
Direct Torque Control with Space Vector Modulation (DTC-SVM) of ...
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Sensorless Speed <strong>Direct</strong> <strong>Torque</strong> <strong>Control</strong> <strong>with</strong> <strong>Space</strong> <strong>Vector</strong> <strong>Modulation</strong> (<strong>DTC</strong>-<strong>SVM</strong>)<br />
Ψ PM<br />
I sA<br />
ABC<br />
Is<br />
α<br />
αβ<br />
Isd<br />
L d<br />
Ψ sd<br />
dq<br />
Ψ sα<br />
Ψ s<br />
I sB<br />
αβ<br />
Is<br />
β<br />
dq<br />
I sq<br />
L q<br />
Ψ sq<br />
αβ<br />
Ψ sβ<br />
θ Ψs<br />
γ m<br />
Figure 6.7. Current model based stator flux estimator.<br />
6.3.3 Voltage model based flux estimator <strong>with</strong> ideal integrator<br />
The stator flux linkage can be obtained by using terminal voltages and currents. It is the<br />
integral <strong>of</strong> terminal voltages minus the resistance voltage drop:<br />
dΨ sα<br />
= ( Us α − RsIs<br />
α<br />
)<br />
(6.7)<br />
dt<br />
dΨ sβ<br />
= ( Usβ<br />
− RsIsβ<br />
)<br />
(6.8)<br />
dt<br />
However, at low speed (frequencies) some problems arise, when this technique is<br />
applied, since the stator voltage becomes very small and the resistive voltage drops<br />
become dominant, requiring very accurate knowledge <strong>of</strong> the stator resistance R s<br />
and<br />
very accurate integration. The stator resistance can vary due to temperature changes.<br />
This effect can also be taken into consideration by using the thermal model <strong>of</strong> the<br />
machine. Drifts and <strong>of</strong>fsets can greatly influence the precision <strong>of</strong> integration. The<br />
overall accuracy <strong>of</strong> the estimated flux linkage vector will also depend on the accuracy<br />
<strong>of</strong> the monitored voltages and currents.<br />
The most know classical voltage model obtains the flux components in stator<br />
coordinates ( α,<br />
β ) by integrating the motor back electromotive force E , E<br />
sα<br />
sβ (see Fig.<br />
6.8). The method is sensitive for only one motor parameter, stator resistance R s<br />
.<br />
However, the application <strong>of</strong> pure integrator is difficult because <strong>of</strong> dc drift and initial<br />
value problems.<br />
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