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N A<br />

17.7 �-Y, Y-� CONVERSIONS<br />

The �-Y, Y-� (or p-T, T-p as defined in Section 8.12) conversions for<br />

ac circuits will not be derived here since the development corresponds<br />

exactly with that for dc circuits. Taking the �-Y configuration shown<br />

in Fig. 17.46, we find the general equations for the impedances of the Y<br />

in terms of those for the �:<br />

Z 1<br />

Z 3<br />

Z 2<br />

ZBZC<br />

Z1 � �� ZA � ZB<br />

� ZC ZAZC<br />

Z2 � �� ZA � ZB<br />

� ZC ZAZB<br />

Z3 � �� ZA � ZB<br />

� ZC Z B<br />

FIG. 17.47<br />

The T and p configurations.<br />

Z C<br />

(17.13)<br />

(17.14)<br />

(17.15)<br />

Forthe impedances of the � in terms of those for the Y, the equations are<br />

Z1Z2 � Z1Z3 � Z2Z3 ZB � ���<br />

(17.16)<br />

Z1Z2 � Z1Z3 � Z2Z3 ZA � ���<br />

(17.17)<br />

Z1Z2 � Z1Z3 � Z2Z3 ZC � ���<br />

(17.18)<br />

Note that each impedance of the Y is equal to the product of the<br />

impedances in the two closest branches of the �, divided by the sum<br />

of the impedances in the �.<br />

Further, the value of each impedance of the � is equal to the sum of the<br />

possible product combinations of the impedances of theY, divided by the<br />

impedances of theY farthest from the impedance to be determined.<br />

Drawn in different forms (Fig. 17.47), they are also referred to as the T<br />

and p configurations.<br />

Z2<br />

Z1<br />

Z3<br />

Z A<br />

�-Y, Y-� CONVERSIONS ⏐⏐⏐ 771<br />

a b<br />

ZC Z 1<br />

Z B<br />

Z 3<br />

c<br />

FIG. 17.46<br />

�-Y configuration.<br />

Z 2<br />

Z A

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