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an investigation of dual stator winding induction machines

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dλ<br />

v = R ⋅ i +<br />

(3.58)<br />

dt<br />

where, v , i <strong>an</strong>d λ are the terminal voltage, current flow <strong>an</strong>d flux linkage in each circuit;<br />

R is the matrix <strong>of</strong> resist<strong>an</strong>ce. Applying this general equation to the <strong>dual</strong> <strong>stator</strong> <strong>winding</strong><br />

<strong>induction</strong> machine leads to the full model.<br />

3.7.1 Stator Voltage Equation<br />

For the ABC <strong>winding</strong> set, the <strong>stator</strong> voltage equation is expressed as:<br />

v = R i + pλ<br />

(3.59)<br />

abc<br />

abc abc<br />

abc<br />

where, R abc is a diagonal 3× 3 matrix, in which the diagonal value depends on the<br />

d<br />

resist<strong>an</strong>ces per phase <strong>of</strong> the ABC <strong>winding</strong> set; p represents the operator <strong>an</strong>d<br />

dt<br />

⎛v<br />

a ⎞ ⎛ia<br />

⎞ ⎛λ<br />

a ⎞<br />

⎜ ⎟ ⎜ ⎟ ⎜ ⎟<br />

v abc = ⎜v<br />

b ⎟ , i abc = ⎜ib<br />

⎟ , λ abc = ⎜λ<br />

b ⎟ .<br />

⎜ ⎟<br />

⎝v<br />

⎜ ⎟<br />

c ⎠ ⎝i<br />

⎜ ⎟<br />

c ⎠ ⎝ λc<br />

⎠<br />

The flux linkage c<strong>an</strong> be written as the contribution <strong>of</strong> three components as:<br />

λ = λ + λ + λ<br />

(3.60)<br />

abc s1s1<br />

s1s2<br />

s1r<br />

The first term in equation (3.60) represents the ABC <strong>winding</strong> set <strong>stator</strong> flux linkage<br />

due to the ABC <strong>winding</strong> <strong>stator</strong> currents, the second term is the flux linkage due to the<br />

XYZ <strong>winding</strong> set <strong>stator</strong> currents <strong>an</strong>d the last term is the contribution <strong>of</strong> the rotor current.<br />

More detailed expl<strong>an</strong>ations <strong>of</strong> each term will be developed separately in the following<br />

sub-sections.<br />

111

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