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658 ⏐⏐⏐ SERIES AND PARALLEL ac CIRCUITS<br />

Y L – Y C<br />

j<br />

Y C<br />

Y L<br />

0.2136 S<br />

20.56°<br />

Y R<br />

Y T<br />

FIG. 15.59<br />

Admittance diagram for the network of<br />

Fig. 15.58.<br />

+<br />

1<br />

1<br />

YL � BL ��90° � � ��90° � � ��90°<br />

XL<br />

8 �<br />

� 0.125 S ��90° � 0 � j 0.125 S<br />

1<br />

1<br />

YC � BC �90° � � �90° � � �90°<br />

XC 20 �<br />

� 0.050 S ��90° � 0 � j 0.050 S<br />

b. YT � YR � YL � YC � (0.2 S � j 0) � (0 � j 0.125 S) � (0 � j 0.050 S)<br />

� 0.2 S � j 0.075 S � 0.2136 S ��20.56°<br />

1<br />

c. ZT ���� � 4.68 � �20.56°<br />

0.2136 S ��20.56°<br />

or<br />

ZRZLZC ZT ����<br />

ZRZL � ZLZC � ZRZC (5 � �0°)(8 � �90°)(20 � ��90°)<br />

�������<br />

(5 � �0°)(8 � �90°) � (8 � �90°)(20 � ��90°)<br />

� (5 � �0°)(20 � ��90°)<br />

800 � �0°<br />

�����<br />

40 �90° � 160 �0° � 100 ��90°<br />

800 �<br />

800 �<br />

��� ���<br />

160 � j 40 � j 100 160 � j 60<br />

800 �<br />

���<br />

170.88 ��20.56°<br />

� 4.68 � �20.56°<br />

d. The admittance diagram appears in Fig. 15.59.<br />

On many occasions, the inverse relationship YT � 1/ZT or ZT �<br />

1/YT will require that we divide the number 1 by a complex number<br />

having a real and an imaginary part. This division, if not performed in<br />

the polar form, requires that we multiply the numerator and denominator<br />

by the conjugate of the denominator, as follows:<br />

1 1<br />

1 (4 ��j 6 �) 4 � j 6<br />

YT����� � �� ��<br />

� �� ���22 ZT 4 ��j 6 � 4 ��j 6 � (4 ��j 6 �) 4 � 6<br />

4 6<br />

and YT � � S � j � S<br />

52 52<br />

To avoid this laborious task each time we want to find the reciprocal<br />

of a complex number in rectangular form, a format can be developed<br />

using the following complex number, which is symbolic of any impedance<br />

or admittance in the first or fourth quadrant:<br />

1<br />

�<br />

a 1 � jb 1<br />

1<br />

�<br />

a1 � jb1 a1 � j b1 �<br />

a1 � j b1 � � �� � �<br />

a 1 � j b 1<br />

�a 2 1 � b 2 1<br />

1 a1<br />

or �� � �2 (15.27)<br />

a1 � jb1 a1 � b 2 b1<br />

� � j �2 1 a1 � b 2 �<br />

1<br />

Note that the denominator is simply the sum of the squares of each<br />

term. The sign is inverted between the real and imaginary parts. A few<br />

examples will develop some familiarity with the use of this equation.<br />

a c

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