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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure 2.26 – Rotor-stator flux linkage for a sinusoidal and arbitrary trapezoidal motor.<br />

The expressions for torque and bEMF were derived previously as Equations (2.31)-(2.32) and<br />

Equations (2.36)-(2.37).<br />

(2.31): ( ) N<br />

D Y<br />

B sin(<br />

) i(<br />

t)<br />

T r<br />

p r<br />

(2.32): ( ) K<br />

sin( ) i(<br />

t)<br />

T r<br />

t r<br />

(2.36): e( ) NDYB sin( ) (<br />

t)<br />

r p r<br />

(2.37): e( ) K sin( ) (<br />

t)<br />

r e r<br />

Comparing Equations (2.43)-(2.44), (2.31)-(2.32), and (2.36)-(2.37) makes clear the equivalence<br />

shown in Equation (2.48).<br />

R Ke Kt NDY Bp<br />

(2.48)<br />

Equation (2.48) shows that the units of e K and t<br />

K are the units of flux linkage, Wb( turns) <br />

.<br />

Further, the derivative of Equation (2.44) with respect to rotor position is Equation (2.49).<br />

d<br />

R( r) Rsin( r)<br />

(2.49)<br />

d r<br />

Comparing Equation (2.49) with Equations (2.32) and (2.37) makes clear the relationships shown<br />

in Equations (2.50) and (2.51).<br />

d<br />

Tt () R( r)<br />

it ()<br />

(2.50)<br />

d r<br />

d<br />

et () R( r) ()<br />

t<br />

(2.51)<br />

d r<br />

Similar to Equation (2.48), these can be written as Equation (2.52).<br />

44

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