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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<strong>Control</strong> methods <strong>of</strong> PM Synchronous motor<br />
b)<br />
U DC<br />
M e _ ref<br />
Fig. 4.5<br />
I sd _ ref<br />
I sq _ ref<br />
-<br />
e Isd<br />
-<br />
e Isq<br />
PI<br />
PI<br />
U sd<br />
U sq<br />
Reference<br />
Voltage<strong>Vector</strong><br />
Calculation<br />
U s _ ref<br />
ϕ Us _ ref<br />
<strong>Space</strong><br />
<strong>Vector</strong><br />
Modulator<br />
S A<br />
S B<br />
S C<br />
Inverter<br />
γ s<br />
I sd<br />
I sq<br />
dq/ABC<br />
current<br />
sensors<br />
I s<br />
γ m<br />
rotor<br />
position<br />
sensor<br />
PMSM<br />
Figure 4.7 <strong>Vector</strong> control structure for PM synchronous motor <strong>with</strong>: a) hysteresis current<br />
control, b) synchronous PI current control<br />
4.3 <strong>Direct</strong> torque control (<strong>DTC</strong>)<br />
The name direct torque control is deliver by the fact that, on the basis <strong>of</strong> the errors<br />
between the reference and the estimated values <strong>of</strong> torque and flux, it is possible to<br />
directly control the inverter states <strong>with</strong>out inner current control loop as for FOC<br />
[32,34,35,50] and [57-66].<br />
The basic idea <strong>of</strong> this control rely on stator voltage vector equation <strong>of</strong> AC motor.<br />
U<br />
dΨ<br />
s<br />
s<br />
= RsIs<br />
+ (4.1)<br />
dt<br />
Making the assumption that ohmic voltage drop on the stator resistor can be neglected<br />
the equation for stator flux vector takes the form:<br />
Ψ =∫ ( U ) dt<br />
(4.2)<br />
s<br />
s<br />
It can be said that the stator voltage vector has directly influence on control stator flux<br />
vector. Using a three phase voltage source inverter to supply the AC motor, there are six<br />
non-zero vectors and two zero voltage vectors. The active vectors change the amplitude<br />
and position <strong>of</strong> stator flux vector, while the zero vectors stop the stator flux vector as<br />
shown in Fig. 4.8.<br />
57