In the series-parallel RC circuit of Figure 15-51, determine the following:
(a) total impedance (b) total current (e) phase angle by which I_{tot} leads V_{s}
In the series-parallel RC circuit of Figure 15-51, determine the following:
(a) total impedance (b) total current (e) phase angle by which I_{tot} leads V_{s}
(a) First, calculate the magnitudes of capacitive reactance.
X_{C1}= \frac{1}{2\pi fC} = \frac{1}{2\pi (5 \ kHz)(0.1 \ \mu F)}= 318 \ \OmegaX_{C2}= \frac{1}{2\pi fC} = \frac{1}{2\pi (5 \ kHz)(0.047 \ \mu F)}= 677 \ \Omega
One approach is to find the impedance of the series portion and the impedance of the parallel portion and combine them to get the total impedance. The impedance of the series combination of R_{1} and C_{1} is
Z_{1} =R_{1} – jX_{C1} = 1.0 kΩ – j318 Ω
To determine the impedance of the parallel portion, first determine the admittance of the parallel combination of R_{2} and C_{2}
G_{2}= \frac{1}{R_{2}}= \frac{1}{680 \ \Omega}= 1.47 \ mSB_{C2}= \frac{1}{X_{C2}}= \frac{1}{677 \ \Omega}= 1.48 \ mS
Y_{2} = G_{2} + j B_{C2} = 1.47 mS + j1.48 mS
Converting to polar form yields
Y_{2}= \sqrt{G^{2}_{2} + B^{2}_{C2}} \angle \tan ^{-1}\left(\frac{B_{C2}}{G_{2}} \right)\ \ \ \ = \sqrt{(1.47 \ mS)^{2} + (1.48 \ mS)^{2}} \angle \tan ^{-1}\left(\frac{1.48 \ mS}{1.47 \ mS} \right)= 2.09 \angle 45.2°mS
Then, the impedance of the parallel portion is
Z_{2}= \frac{1}{Y_{2}}=\frac{1}{(2.09 \angle 45.2° mS)}= 478 \angle -45.2° \ \OmegaConverting to rectangular form yields
Z_{2}= Z_{2}\cos \theta – jZ_{2}\sin \theta\ \ \ \ \ \ = (478 \ \Omega) \cos (-45.2°)- j(478 \ \Omega) \sin (-45.2°)= 337 \ \Omega – j339 \ \Omega
The series portion and the parallel portion are in series with each other. Combine Z_{1} and Z_{2} to get the total impedance.
Z_{tot} = Z_{1} + Z_{2}\ \ \ \ \ \ = (1.0 \ k\Omega -j318 \ \Omega) + (337 \ \Omega – j339 \ \Omega) = 1337 \ \Omega – j657 \ \Omega
Expressing Z_{tot} in polar form yields
Z_{tot} =\sqrt{Z^{2}_{1}+ Z^{2}_{2}} \angle -\tan ^{-1}\left(\frac{Z_{2}}{Z_{1}} \right)\ \ \ \ \ \ = \sqrt{(1338 \ \Omega )^{2}+ (657 \ \Omega )^{2}} \angle -\tan ^{-1}\left(\frac{657 \ \Omega}{1337 \ \Omega} \right)= 1.49 \angle -26.2° k\Omega
(b) Use Ohm’s law to determine the total current.
I_{tot}= \frac{V_{s}}{Z_{tot}}= \frac{10 \angle 0° V}{1.49 \angle -26.2° k\Omega} = 6.71 \angle 26.2° mA(c) The total current leads the applied voltage by 26.2°.