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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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In a symmetrical machine the self inductance of each phase is equal and the mutual inductance<br />

between any two phases is equal,<br />

LAA LBB LCC L<br />

LAB LBA LAC LCA LBC LCB M<br />

thus the set of flux linkages can be written as Equation (B.8).<br />

A LiA MiB MiC AR<br />

B MiA LiB MiC BR<br />

Mi Mi Li C A B C CR<br />

(B.8)<br />

When the phase resistance is considered the voltage equation can be written for each phase as<br />

Equation (B.9).<br />

d<br />

vAN RiA A<br />

dt<br />

d<br />

vBN RiB B<br />

(B.9)<br />

dt<br />

d<br />

vCN RiC C<br />

dt<br />

Substituting in Equation (B.8) yields the full voltage equations, Equation (B.10). Using the bEMF<br />

and matrix form this is given as Equation (B.11).<br />

vAN RiA Li A Mi B Mi C AR<br />

vBN RiBMi A Li B Mi C BR<br />

v Ri Mi Mi Li <br />

CN C A B C CR<br />

vAN R iA L M M iA eA d<br />

v<br />

<br />

<br />

<br />

R<br />

<br />

i<br />

<br />

<br />

<br />

M L M<br />

<br />

i<br />

<br />

<br />

<br />

e<br />

<br />

BN B B B<br />

dt <br />

v CN R i C M M L i C e C <br />

(B.10)<br />

(B.11)<br />

This report considers only isolated neutral motors thus the currents must sum to zero. The linear<br />

dependence of the currents is expressed by 0 the expression; this can be arranged in the<br />

three different ways shown in Equation (B.12).<br />

i i i<br />

i i i<br />

i i i<br />

B C A<br />

A C B<br />

A B C<br />

(B.12)<br />

Writing out Equation (B.11) by hand, substituting Equation (B.12) and simplifying gives<br />

Equation (B.13). The result is that although the mutual inductances still exists, the isolation of the<br />

neutral decouples the circuits.<br />

274

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