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a c<br />

0°<br />

–30°<br />

–45°<br />

–60°<br />

–90°<br />

θL<br />

of IL θL = θs<br />

5 10 20 30 40 f (kHz)<br />

Network inductive<br />

θ L ( f )<br />

Network resistive<br />

θR ≅ θs<br />

≅ 0°<br />

FIG. 15.84<br />

The phase angle of the current I L versus frequency for the parallel R-L network<br />

of Fig. 15.79.<br />

lower-resistance path of the resistor. The magnitude of the phase angle<br />

between I L and I is approaching 90° with an increase in frequency, as<br />

shown in Fig. 15.84, leaving its initial value of zero degrees at f � 0Hz<br />

far behind.<br />

At f � 1 kHz, the phasor diagram of the network appears as shown<br />

in Fig. 15.85. First note that the magnitude and the phase angle of I L are<br />

very close to those of I. Since the voltage across a coil must lead the<br />

current through a coil by 90°, the voltage V s appears as shown. The<br />

voltage across a resistor is in phase with the current through the resistor,<br />

resulting in the direction of I R shown in Fig. 15.85. Of course, at<br />

this frequency R > X L, and the current I R is relatively small in magnitude.<br />

At f � 40 kHz, the phasor diagram changes to that appearing in Fig.<br />

15.86. Note that now I R and I are close in magnitude and phase because<br />

X L > R. The magnitude of I L has dropped to very low levels, and the<br />

phase angle associated with I L is approaching �90°. The network is<br />

now more “resistive” compared to its “inductive” characteristics at low<br />

frequencies.<br />

The analysis of a parallel R-C or R-L-C network would proceed in<br />

much the same manner, with the inductive impedance predominating at<br />

low frequencies and the capacitive reactance predominating at high frequencies.<br />

15.11 SUMMARY: PARALLEL ac NETWORKS<br />

The following is a review of important conclusions that can be derived<br />

from the discussion and examples of the previous sections. The list is<br />

not all-inclusive, but it does emphasize some of the conclusions that<br />

should be carried forward in the future analysis of ac systems.<br />

SUMMARY: PARALLEL ac NETWORKS ⏐⏐⏐ 673<br />

I R<br />

V s<br />

83.49°<br />

–6.51°<br />

FIG. 15.85<br />

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

of Fig. 15.79 at f � 1 kHz.<br />

I L<br />

I L<br />

12.35° IR Vs –77.65°<br />

I<br />

FIG. 15.86<br />

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

of Fig. 15.79 at f � 40 kHz.<br />

I

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