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an investigation of dual stator winding induction machines

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electromagnetic torque components that brought about by the presence <strong>of</strong> rotor<br />

eccentricities.<br />

4.2 Stator Induct<strong>an</strong>ces Calculation<br />

The <strong>stator</strong> induct<strong>an</strong>ces considered here include the <strong>stator</strong> <strong>winding</strong> self-induct<strong>an</strong>ces<br />

<strong>an</strong>d the mutual induct<strong>an</strong>ces between the <strong>stator</strong> <strong>winding</strong> sets. Since the pole numbers <strong>of</strong><br />

the two <strong>stator</strong> <strong>winding</strong> sets are different, the mutual induct<strong>an</strong>ces between the two <strong>stator</strong><br />

<strong>winding</strong> sets are zero. The induct<strong>an</strong>ces calculated in this section are self <strong>an</strong>d mutual<br />

induct<strong>an</strong>ces <strong>of</strong> the ABC <strong>an</strong>d XYZ <strong>winding</strong> sets.<br />

4.2.1 Self Induct<strong>an</strong>ces <strong>of</strong> the ABC <strong>winding</strong> Set<br />

The general expression to calculate the self-induct<strong>an</strong>ce <strong>of</strong> th<br />

i <strong>winding</strong> is:<br />

2π<br />

1<br />

Lii = µ 0rl<br />

∫ ⋅ ni<br />

i<br />

g<br />

where, ( θ )<br />

i<br />

0<br />

( θ,<br />

θ )<br />

rm<br />

( θ ) ⋅ N ( θ ) ⋅ dθ<br />

n is the turn function <strong>of</strong> th<br />

<strong>winding</strong>; g( θ )<br />

θ, is the air gap function.<br />

rm<br />

i <strong>winding</strong>; ( θ )<br />

154<br />

i<br />

(4.1)<br />

N is the <strong>winding</strong> function <strong>of</strong> th<br />

i<br />

The clock diagram <strong>of</strong> the ABC <strong>winding</strong> set is shown in Figure 3.2 while the turn<br />

function <strong>of</strong> the ABC <strong>winding</strong> set is given in Figure 3.3. For phase A, the self-induct<strong>an</strong>ce<br />

is:<br />

2π<br />

1<br />

LAA = µ 0rl<br />

∫ ⋅ nA<br />

A<br />

g<br />

0<br />

( θ,<br />

θ )<br />

rm<br />

( θ ) ⋅ N ( θ ) ⋅ dθ<br />

(4.2)

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