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a c<br />

I<br />

Admittance diagram: As shown in Fig. 15.64.<br />

B L ∠ –90° = 0.4 S ∠ –90°<br />

j<br />

G ∠ 0° = 0.3 S ∠ 0°<br />

53.13°<br />

+<br />

Y T = 0.5 S ∠ –53.13°<br />

E<br />

I � �EYT � (20 V �53.13°)(0.5 S ��53.13°) � 10 A �0°<br />

I R and I L<br />

FIG. 15.64<br />

Admittance diagram for the parallel R-L network of Fig. 15.62.<br />

� ZT<br />

E �v<br />

IR ���(E�v)(G �0°)<br />

R �0°<br />

� (20 V �53.13°)(0.3 S �0°) � 6 A �53.13°<br />

E �v<br />

IL ���(E�v)(BL ��90°)<br />

XL �90°<br />

� (20 V �53.13°)(0.4 S ��90°)<br />

� 8 A ��36.87°<br />

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

I � IR � IL � 0<br />

or<br />

I � IR � IL 10 A �0° � 6 A �53.13° � 8 A ��36.87°<br />

10 A �0° � (3.60 A � j 4.80 A) � (6.40 A � j 4.80 A) � 10 A � j 0<br />

and 10 A �0° � 10 A �0° (checks)<br />

Phasor diagram: The phasor diagram of Fig. 15.65 indicates that<br />

the applied voltage E is in phase with the current IR and leads the current<br />

IL by 90°.<br />

Power: The total power in watts delivered to the circuit is<br />

PT � EI cos vT � (20 V)(10 A) cos 53.13° � (200 W)(0.6)<br />

� 120 W<br />

or PT � I 2 R � �V 2 RG � (20 V) 2 V<br />

(0.3 S) � 120 W<br />

2 R<br />

�<br />

R<br />

PARALLEL ac NETWORKS ⏐⏐⏐ 661<br />

j<br />

I R<br />

53.13°<br />

36.87°<br />

FIG. 15.65<br />

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

of Fig. 15.62.<br />

E<br />

I L<br />

I<br />

+

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