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Direct Torque Control with Space Vector Modulation (DTC-SVM) of ...

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Modeling and control modes <strong>of</strong> PM synchronous motor drives<br />

For the PM synchronous motor the amplitude <strong>of</strong> stator flux<br />

Ψ<br />

s<br />

is established by<br />

permanent magnet. Operation <strong>with</strong> stator flux amplitude belong the nominal value <strong>of</strong><br />

rotor flux amplitude<br />

Ψ<br />

PM<br />

increases the amplitude <strong>of</strong> stator phase current. Please note<br />

that maximum amplitude <strong>of</strong> the stator current vector is calculated as:<br />

higher value may damage the PM (complete demagnetization).<br />

I<br />

s<br />

Ψ<br />

≤<br />

L<br />

PM<br />

d<br />

, and<br />

From the Fig. 2.8 it can be observed that rated torque is achieved for torque angle<br />

0< < 25 <br />

electrical degree.<br />

δ Ψ<br />

e[ ] M Nm<br />

M<br />

er<br />

[ Nm ]<br />

M<br />

es<br />

[ Nm ]<br />

δ Ψ<br />

[deg]<br />

Figure 2.8. Variation <strong>of</strong> synchronous torque M es<br />

, reluctance torque M<br />

er<br />

and resultant<br />

torque M as a function <strong>of</strong> torque angle (for constant stator flux equal value <strong>of</strong> PM).<br />

e<br />

2.1.3 Mechanical motion equation<br />

The equation <strong>of</strong> rotor motion dynamics describes the mechanical equilibrium <strong>of</strong> a drive<br />

system. Taking the moment <strong>of</strong> inertia to be constant ( J = const.<br />

) and neglecting friction<br />

and elastic torque we can write:<br />

where,<br />

M<br />

e<br />

= Ml + Md<br />

(2.59)<br />

Ml<br />

is the external torque on the motor shaft, and<br />

M<br />

dΩ<br />

dt<br />

where: J is total moment <strong>of</strong> inertia,<br />

M<br />

d<br />

the dynamic torque<br />

m<br />

d<br />

= J<br />

(2.60)<br />

Ω<br />

m<br />

angular speed <strong>of</strong> the rotor.<br />

22

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