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Space Vector Modulated – Direct Torque Controlled (DTC – SVM ...

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2. Voltage Source Inverter Fed Induction Motor Drive<br />

The times t 1 and t 2 are obtained from simple trigonometrical relationships and can be<br />

expressed in the following equations:<br />

2 3<br />

t<br />

1<br />

= MTs<br />

sin( π 3 −α<br />

)<br />

(2.24a)<br />

π<br />

2 3<br />

t<br />

2<br />

= MTs<br />

sin( α )<br />

(2.24b)<br />

π<br />

Where M is a modulation index, which for the space vector modulation is defined as:<br />

M<br />

U<br />

=<br />

U<br />

c<br />

1( six−step)<br />

U<br />

c<br />

=<br />

2<br />

U<br />

π<br />

dc<br />

(2.25)<br />

where:<br />

U<br />

c<br />

- vector magnitude, or phase peak value,<br />

U1 ( six − step)<br />

- fundamental peak value ( U dc<br />

π )<br />

2 of the square-phase voltage<br />

wave.<br />

The modulation index M varies from 0 to 1 at the square-wave output. The length of<br />

the U c vector, which is possible to realize in the whole range of α is equal to<br />

3<br />

U<br />

3<br />

This is a radius of the circle inscribed of the hexagon in Fig. 2.13. At this condition the<br />

modulation index is equal:<br />

dc<br />

.<br />

M<br />

=<br />

3<br />

U<br />

3<br />

2<br />

U<br />

π<br />

dc<br />

dc<br />

= 0.907<br />

(2.26)<br />

This means that 90.7% of the fundamental at the square wave can be obtained. It<br />

extends the linear range of modulation in relation to 78.55% in the sinusoidal<br />

modulation techniques (Fig. 2.10).<br />

After calculation of t 1 and t 2 from equations (2.24) the residual sampling time is<br />

reserved for zero vectors U 0 and U 7 .<br />

t =<br />

s<br />

− ( + = t + t<br />

(2.27)<br />

0 ,7<br />

T t1<br />

t2<br />

)<br />

0<br />

7<br />

24

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