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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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j0 j0 j0<br />

aˆ<br />

1 0 1<br />

bˆ<br />

<br />

<br />

j e e e <br />

1<br />

3<br />

<br />

2 2<br />

<br />

j120 j2 /3j j e e e a<br />

(3.35)<br />

1 3<br />

<br />

j120 j2 /3 j<br />

2<br />

cˆ<br />

j e e e a<br />

2 2<br />

Similar to the CRT example presented earlier, the MMF produced due to the combined effect of<br />

current in the three windings could be represented by an MMF space vector. In the CRT example<br />

the relationship between voltage and the force it produces is a constant of proportionality and in a<br />

machine the relationship between current and the MMF it produces is also a constant of<br />

proportionality—the same as that in Equation (3.1). Using this constant, the concept of Equations<br />

(3.32)-(3.34) from the CRT example, and the directionality of the magnetic axes of windings<br />

shown in Figure 3.1, the MMF produced by current space vector could be described as Equation<br />

(3.36). 22<br />

Ne Ne <br />

() ˆ () ˆ Ne<br />

<br />

f i () ˆ<br />

A t i B t iC t<br />

2<br />

a <br />

2<br />

b <br />

2<br />

c<br />

<br />

(3.36)<br />

Further, the CRT example showed that the constant of proportionality could be pulled out front<br />

and the force space vector could be described by defining a voltage space vector. The similar case<br />

here is to define the MMF space vector by defining a current space vector as shown in Equation<br />

(3.37), where the current space vector is given by Equation (3.38).<br />

Ne<br />

<br />

f () ˆ () ˆ<br />

<br />

i () ˆ<br />

A t i B t iC<br />

t <br />

2<br />

<br />

a b c<br />

(3.37)<br />

<br />

<br />

<br />

i i () ˆ () ˆ () ˆ<br />

A t i B t iC<br />

t <br />

<br />

a b c<br />

(3.38)<br />

<br />

The basis vectors in Equation (3.36)-(3.38) are typically represented by one of the rectangular or<br />

polar notations in Equation (3.35). Therefore the current space vector, for example, is typically<br />

written in the form of Equation (3.39) or Equation (3.40); this report will favor the form of<br />

Equation (3.40). In addition a very important transformation constant (k) has been added to scale<br />

the result to account for the fact that the basis vectors are not linearly independent; it will be<br />

discussed in detail later but for simplicity its importance will be minimized for now by selecting<br />

k=1 until further notice.<br />

22<br />

Until the section titled “The SV as a Distribution,” the reader is asked to ignore the idea of sinusoidally<br />

distributed quantities in a machine.<br />

97

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