Question 15.20: Convert the parallel circuit in Figure 15-49 to a series for...

Convert the parallel circuit in Figure 15-49 to a series form.

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First, find the admittance of the parallel circuit as follows:

G=\frac{1}{R}= \frac{1}{18 \ k\Omega }= 55.6 \ \mu S

 

B_{C}=\frac{1}{X_{C}}= \frac{1}{27 \ k\Omega }= 37.0 \ \mu S

 

Y = G + jB_{C} = 55.6 \mu S + 37.0 \mu S

Converting to polar form yields

Y= \sqrt{G^{2}+ B^{2}_{C}} \angle \tan ^{-1} \left (\frac{B_{C}}{G} \right)

 

\ \ \ \ \ = \sqrt{(55.6 \ \mu S)^{2}+ (37.0 \ \mu S)^{2}} \angle \tan ^{-1} \left(\frac{37.0 \ \mu S}{55.6 \ \mu S} \right)= 66.8 \angle 33.6° \mu S

Then, the total impedance is

Z_{tot}= \frac{1}{Y}=\frac{1}{66.8 \angle 33.6° \mu S}= 15.0 \angle -33.6° \ K\Omega

Converting to rectangular form yields

Z_{tot}= Z\cos \theta – jZ\sin \theta = R_{eq}- jX_{C(eq)}

 

\ \ \ \ \ \ = 15.0 \ k\Omega \cos (-33.6°)- j15.0 \ k\Omega \sin (-33.6°)= 12.5 \ k\Omega – j8.31 \ k\Omega

The equivalent series RC circuit is a 12.5 kΩ resistor in series with a capacitive reactance of 8.31 kΩ. This is shown in Figure 15-50.

Screenshot (759)

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