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an investigation of dual stator winding induction machines

an investigation of dual stator winding induction machines

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are applied in this kind <strong>of</strong> <strong>dual</strong> <strong>stator</strong> <strong>winding</strong> <strong>induction</strong> machine <strong>an</strong>d the input voltage<br />

frequency <strong>of</strong> each <strong>stator</strong> <strong>winding</strong> depends on the control objectives <strong>an</strong>d is not required to<br />

be fixed. Generally, the two simult<strong>an</strong>eous MMFs have different rotating speeds <strong>an</strong>d the<br />

peak value <strong>of</strong> the combination <strong>of</strong> two simult<strong>an</strong>eous MMFs ch<strong>an</strong>ges with time. The<br />

machine design is to make sure that even in the worst case, the machine c<strong>an</strong> still avoid<br />

operating in deep magnetic saturation.<br />

Assuming the <strong>dual</strong> <strong>stator</strong> machine is wound for 2/6 pole <strong>an</strong>d neglecting the saturation,<br />

the flux density in the air gap at a given inst<strong>an</strong>t time c<strong>an</strong> be expressed as:<br />

2 / 6<br />

2<br />

[ cos(<br />

θ ) − cos(<br />

3θ<br />

) ]<br />

Bg ( θ ) = B K + δ<br />

(2.6)<br />

1<br />

1<br />

where the magnitude <strong>of</strong> the flux density induced by the 2-pole <strong>winding</strong> set is B 2 , the ratio<br />

<strong>of</strong> the magnitude <strong>of</strong> the flux density induced by the 6-pole <strong>winding</strong> set <strong>an</strong>d the 2-pole<br />

<strong>winding</strong> set is K 1 <strong>an</strong>d the phase <strong>an</strong>gle between two flux densities, which may be a time<br />

varying number , is 1<br />

δ . In the worst case, the peak value <strong>of</strong> g 2 / 6<br />

θ = θ p ; 1 K is a positive value <strong>an</strong>d the delay <strong>an</strong>gle δ 1 is zero.<br />

50<br />

B will be obtained when<br />

On the other h<strong>an</strong>d, the 4-pole single <strong>stator</strong> <strong>winding</strong> set <strong>induction</strong> machine has a flux<br />

distribution expressed as:<br />

( θ )<br />

Bg θ ) = B cos 2<br />

(2.7)<br />

4 ( 4<br />

To maintain the same magnetic saturation level produced by peak flux density, the<br />

peak flux density value <strong>of</strong> the <strong>dual</strong>-<strong>winding</strong> design will be equal to the peak flux density<br />

<strong>of</strong> the single 4-pole machine, which c<strong>an</strong> be expressed as:<br />

[ ( θ ) − K cos(<br />

3 ) ]<br />

cos<br />

2 p 1<br />

B = B<br />

θ<br />

(2.8)<br />

4<br />

p

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