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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure D.1 show that the PS and NS phasors vectorially sum to zero but the ZS phasors sum to a<br />

cophasal phasor whose magnitude is three times that of the ZS phasors. Since the PS and NS<br />

components sum to zero we will call them 0 components. Since the ZS component does not<br />

sum to zero it could be called the 0 component but since only the ZS component has this<br />

property it will be called the ZS component. The consequence of this is that in analyzing<br />

symmetrical three-phase systems we can group the harmonic components into 0 components<br />

and a ZS component. As will be shown, the reason for the separate treatment is that ZS<br />

component affects three-phase systems differently than do 0 components.<br />

The ZS component has been defined in the traditional manner using phasors. From Figure D.3 it<br />

is seen that in three-phase systems the ZS component is composed of the odd multiples of three;<br />

these are called the triplen harmonics. But also, any common-mode component among the phase<br />

variables in a set is a ZS component. If a common mode component were plotted against time it<br />

would be found to have a spectra consisting of only triplens and/or a DC component. Thus, this<br />

report defines the ZS component to be the common-mode component; this is commonly implied in<br />

the literature but is often unstated.<br />

that ZS current would flow, the current would produce zero net MMF, which obviously cannot rotate.<br />

Third, the SV cannot capture ZS terms even if they were present (this is true for any space vector).<br />

312

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