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an investigation of dual stator winding induction machines

an investigation of dual stator winding induction machines

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The turn function <strong>of</strong> the th<br />

i rotor loop is:<br />

[ 0,<br />

θi<br />

)<br />

[ θi<br />

, θi<br />

+ α r )<br />

[ θ + α , 2π<br />

)<br />

⎧0<br />

θ ∈<br />

⎪<br />

n i ( θ ) = ⎨1<br />

θ ∈<br />

(3.50)<br />

⎪<br />

⎩0<br />

θ ∈ i r<br />

The <strong>winding</strong> function c<strong>an</strong> be expressed as:<br />

⎧ α r<br />

⎪−<br />

θ ∈[<br />

0,<br />

θi<br />

)<br />

2π<br />

⎪ α r<br />

N i ( θ ) = ⎨1<br />

− θ ∈[<br />

θi<br />

, θi<br />

+ α r )<br />

(3.51)<br />

⎪ 2π<br />

⎪ α r − θ ∈[<br />

θi<br />

+ α r , 2π<br />

)<br />

⎪⎩<br />

2π<br />

where, α r is the th<br />

i rotor loop pitch. Since a symmetrical equally spaced rotor bar<br />

structure is considered in the <strong>an</strong>alysis, all the rotor loops have the same pitch α r .<br />

None <strong>of</strong> the turn <strong>an</strong>d <strong>winding</strong> functions shown in Figure 3.6 take the skew <strong>of</strong> the rotor<br />

into the consideration. If the rotor is skewed, the turn function <strong>an</strong>d <strong>winding</strong> function are<br />

shown in Figure 3.7.<br />

1<br />

α<br />

− r<br />

2π<br />

0<br />

α<br />

1 − r<br />

2π<br />

Figure 3.7 Rotor<br />

β<br />

θi<br />

β<br />

θi<br />

θ i + α r<br />

θ α − β<br />

i + r<br />

θ i + α r<br />

θ i + α r − β<br />

106<br />

2π<br />

2π<br />

(a)<br />

(b )<br />

th<br />

i rotor loop turn <strong>an</strong>d <strong>winding</strong> function for skewed rotor, (a) turn function, (b)<br />

<strong>winding</strong> function.

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