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a c<br />

Using Eq. (15.32), we obtain<br />

G 0.3 S<br />

Fp � cos vT �����0.6 lagging<br />

YT 0.5 S<br />

Impedance approach: The input current I can also be determined<br />

by first finding the total impedance in the following manner:<br />

Z<br />

ZT �<br />

RZLZC ��� � 2 � �53.13°<br />

ZRZL � ZLZC � ZRZC and, applying Ohm’s law, we obtain<br />

E 100 V �53.13°<br />

I � �� ��� �50 A �0°<br />

Z 2 � �53.13°<br />

T<br />

15.9 CURRENT DIVIDER RULE<br />

The basic format for the current divider rule in ac circuits is exactly<br />

the same as that for dc circuits; that is, for two parallel branches with<br />

impedances Z 1 and Z 2 as shown in Fig. 15.76,<br />

Z<br />

I1 � �<br />

2IT Z<br />

� or I2 � �<br />

1IT �<br />

Z1 �<br />

Z1 �<br />

I T = 5 A 30°<br />

Z 2<br />

R<br />

1 �<br />

X C<br />

X L<br />

8 �<br />

2 �<br />

FIG. 15.78<br />

Example 15.16.<br />

(15.33)<br />

EXAMPLE 15.15 Using the current divider rule, find the current<br />

through each impedance of Fig. 15.77.<br />

Solution:<br />

Z<br />

IR �<br />

LIT (4 � �90°)(20 A �0°) 80 A�90°<br />

� ���� ���<br />

ZR � ZL 3 � �0° � 4 � �90° 5 �53.13°<br />

� 16 A �36.87°<br />

Z (3 � �0°)(20 A �0°) 60 A�0°<br />

IL �<br />

RIT � ���� ���<br />

ZR � ZL 5 � �53.13° 5 �53.13°<br />

� 12 A ��53.13°<br />

EXAMPLE 15.16 Using the current divider rule, find the current<br />

through each parallel branch of Fig. 15.78.<br />

Solution:<br />

ZC IT (2 � ��90°)(5 A �30°) 10 A��60°<br />

IR-L ��� ���� ���<br />

ZC � ZR-L �j 2 ��1 ��j 8 � 1 � j 6<br />

10 A��60°<br />

��� � 1.644 A ��140.54°<br />

6.083 �80.54°<br />

Z 2<br />

I T<br />

CURRENT DIVIDER RULE ⏐⏐⏐ 667<br />

I = 20 A<br />

0°<br />

I 1<br />

I 2<br />

Z 1<br />

Z 2<br />

I R<br />

R 3 �<br />

X L<br />

I T<br />

FIG. 15.76<br />

Applying the current divider rule.<br />

FIG. 15.77<br />

Example 15.15.<br />

I L<br />

4 �

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