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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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peak value is represented as an uppercase letter. Power system engineers use RMS-valued<br />

phasors exclusively but both peak- and RMS-valued space vectors are found in the motor control<br />

literature. Because peak space vectors are used in this report, peak phasors will also be used.<br />

Further, this report uses the cosine as reference; the sine reference is used in a portion of the<br />

literature but seems to complicate the math. The phasor is seen to represent a scalar quantity as<br />

the real part of a complex vector that is made to rotate at angular velocity ω.<br />

jt jt <br />

et () E cos( t)<br />

ReEeReE e<br />

(3.24)<br />

p p<br />

~ <br />

j0<br />

E E pe<br />

<br />

E p0<br />

(3.25)<br />

The phasor of Equation (3.25) is defined as the reference phasor because the scalar signal it<br />

represents has its peak value whent 0 . By definition then, the reference line must be the real<br />

axis and the phasor diagram therefore represents the snapshot in time when t 0 . The phasor<br />

diagram “captures” all phasors when at the reference signal peaks just like a digital storage<br />

oscilloscope set to trigger upon detection of a peak. Phasors for other sinusoids are defined with a<br />

phase measured relative to the reference phasor; traces on an oscillogram have a phase defined<br />

from the trigger point of the reference waveform. For example, the applied terminal voltage,<br />

Equation (3.26), is represented in phasor form as in Equation (3.27). Figure 3.17 shows clearly<br />

how the phase ( ) of a V is defined relative to a E .<br />

j jt jt <br />

vt () Vcos( t) ReVeeReV e<br />

(3.26)<br />

p p<br />

V V e V <br />

(3.27)<br />

j<br />

p p<br />

According to the discussion in the previous chapter, the bEMF is the time derivative of the rotor-<br />

stator flux linkage, which is Ra ,<br />

for phase-A. In the phasor domain the time derivative<br />

corresponds to multiplication by jω. Therefore the bEMF a<br />

E~ will always lead Ra ,<br />

in phase by<br />

90° and its amplitude will be proportional to rotor speed; this agrees with the development of the<br />

previous chapter and the relationship is shown in Figure 3.19. Following a convention used in<br />

[27], phasors of electromagnetic quantities are represented with a hollow diamond head.<br />

85

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