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a c<br />

or E � V R � V L � V C<br />

which can also be verified through vector algebra.<br />

Phasor diagram: The phasor diagram of Fig. 15.38 indicates that<br />

the current I is in phase with the voltage across the resistor, lags the<br />

voltage across the inductor by 90°, and leads the voltage across the<br />

capacitor by 90°.<br />

Time domain:<br />

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

vR � �2�(30) sin(qt �53.13°) � 42.42 sin(qt � 53.13°)<br />

vL � �2�(70) sin(qt � 36.87°) � 98.98 sin(qt � 36.87°)<br />

vC � �2�(30) sin(qt � 143.13°) � 42.42 sin(qt � 143.13°)<br />

A plot of all the voltages and the current of the circuit appears in Fig.<br />

15.39.<br />

–<br />

�<br />

2<br />

98.98 V<br />

70.70 V<br />

42.42 V<br />

36.87°<br />

0<br />

53.13°<br />

90°<br />

v L<br />

�<br />

FIG. 15.39<br />

Waveforms for the series R-L circuit of Fig. 15.35.<br />

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

PT � EI cos vT � (50 V)(10 A) cos 53.13° � (500)(0.6) � 300 W<br />

or PT � I 2 R � (10 A) 2 (3 �) � (100)(3) � 300 W<br />

or<br />

PT � PR � PL � PC � VRI cos vR � VLI cos vL � VC I cos vC � (30 V)(10 A) cos 0° � (70 V)(10 A) cos 90° � (30 V)(10 A) cos 90°<br />

� (30 V)(10 A) � 0 � 0 � 300 W<br />

Power factor: The power factor of the circuit is<br />

Fp � cos vT � cos 53.13° � 0.6 lagging<br />

Using Eq. (15.9), we obtain<br />

R 3 �<br />

Fp � cos v �����0.6 lagging<br />

ZT<br />

5 �<br />

�<br />

2<br />

e<br />

v R<br />

i<br />

3<br />

�<br />

2<br />

v C<br />

V C<br />

SERIES CONFIGURATION ⏐⏐⏐ 643<br />

j<br />

I<br />

V L –<br />

V C<br />

36.87°<br />

53.13°<br />

V R<br />

E<br />

V L<br />

FIG. 15.38<br />

Phasor diagram for the series R-L-C circuit of<br />

Fig. 15.35.<br />

2�<br />

5<br />

�<br />

2<br />

3�<br />

�t<br />

+

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