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a c<br />

E<br />

Admittance diagram: As shown in Fig. 15.68.<br />

I R and I C<br />

I = 10 A ∠ 0°<br />

I 10 A �0°<br />

E � IZT ����� �10 V ��53.13°<br />

YT 1S�53.13°<br />

IR � (E �v)(G �0°)<br />

� (10 V ��53.13°)(0.6 S �0°) � 6 A ��53.13°<br />

IC � (E �v)(BC �90°)<br />

� (10 V ��53.13°)(0.8 S �90°) � 8 A �36.87°<br />

Kirchhoff’s current law: At node a,<br />

I � I R � I C � 0<br />

or I � I R � I C<br />

+<br />

E<br />

–<br />

which can also be verified (as for the R-L network) through vector<br />

algebra.<br />

Phasor diagram: The phasor diagram of Fig. 15.69 indicates that<br />

E is in phase with the current through the resistor I R and lags the capacitive<br />

current I C by 90°.<br />

Time domain:<br />

e � �2�(10) sin(qt � 53.13°) � 14.14 sin(qt � 53.13°)<br />

iR � �2�(6) sin(qt � 53.13°) � 8.48 sin(qt � 53.13°)<br />

iC � �2�(8) sin(qt � 36.87°) � 11.31 sin(qt � 36.87°)<br />

IR<br />

R 1.67 �<br />

a<br />

I C<br />

1.25 �<br />

FIG. 15.67<br />

Applying phasor notation to the network of Fig. 15.66.<br />

B C ∠ 90° = 0.8 S ∠ 90°<br />

j<br />

53.13°<br />

X C<br />

Y T = 1 S ∠ 53.13°<br />

G ∠ 0° = 0.6 S ∠ 0°<br />

FIG. 15.68<br />

Admittance diagram for the parallel R-C network of Fig. 15.66.<br />

+<br />

PARALLEL ac NETWORKS ⏐⏐⏐ 663<br />

j<br />

36.87°<br />

53.13°<br />

I R<br />

FIG. 15.69<br />

Phasor diagram for the parallel R-C network<br />

of Fig. 15.66.<br />

I C<br />

E<br />

I<br />

+

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