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594 ⏐⏐⏐ THE BASIC ELEMENTS AND PHASORS<br />

Or, since I eff �<br />

(W) (14.16)<br />

then P � � (W) (14.17)<br />

V 2<br />

� � I effR<br />

R<br />

Inductor<br />

In a purely inductive circuit, since v leads i by 90°, |vv � vi| � v �<br />

|�90°| � 90°. Therefore,<br />

VmIm VmIm P �� cos 90° � �(0) � 0 W<br />

2<br />

2<br />

The average power or power dissipated by the ideal inductor (no<br />

associated resistance) is zero watts.<br />

Capacitor<br />

In a purely capacitive circuit, since i leads v by 90°, |vv � vi| � v �<br />

|�90°| � 90°. Therefore,<br />

VmIm VmIm P �� cos(90°) � �(0) � 0 W<br />

2<br />

2<br />

The average power or power dissipated by the ideal capacitor (no<br />

associated resistance) is zero watts.<br />

EXAMPLE 14.10 Find the average power dissipated in a network<br />

whose input current and voltage are the following:<br />

i � 5 sin(qt � 40°)<br />

v � 10 sin(qt � 40°)<br />

Solution: Since v and i are in phase, the circuit appears to be purely<br />

resistive at the input terminals. Therefore,<br />

VmIm (10 V)(5 A)<br />

P ����� �25 W<br />

2 2<br />

10 V<br />

or R �����2 �<br />

Im 5A<br />

V 2 eff<br />

[(0.707)(10 V)]<br />

and P � � �25 W<br />

2<br />

� ��<br />

R<br />

2<br />

or P � I 2 eff R � [(0.707)(5 A)] 2 (2) � 25 W<br />

I m<br />

P � � Vm � � VeffI eff<br />

2<br />

V eff<br />

� R<br />

2 eff<br />

V m<br />

For the following example, the circuit consists of a combination of<br />

resistances and reactances producing phase angles between the input<br />

current and voltage different from 0° or 90°.<br />

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