An industrial load is modeled as a series combination of a capacitance and a resistance as shown in Fig. 9.89. Calculate the value of an inductance L across the series combination so that the net impedance is resistive at a frequency of 50 kHz.
An industrial load is modeled as a series combination of a capacitance and a resistance as shown in Fig. 9.89. Calculate the value of an inductance L across the series combination so that the net impedance is resistive at a frequency of 50 kHz.
To have a resistive impedance, \operatorname{Im}\left({Z}_{\text {in }}\right)=0. Hence,
\begin{array}{l}\omega \mathrm{L} \mathrm{R}^{2}-\left(\frac{\mathrm{L}}{\mathrm{C}}\right)\left(\omega \mathrm{L}-\frac{1}{\omega \mathrm{C}}\right)=0 \\\\\omega \mathrm{R}^{2} \mathrm{C}=\omega \mathrm{L}-\frac{1}{\omega \mathrm{C}} \\\\\omega^{2} \mathrm{R}^{2} \mathrm{C}^{2}=\omega^{2} \mathrm{LC}-1 \\\\\mathrm{L}=\frac{\omega^{2} \mathrm{R}^{2} \mathrm{C}^{2}+1}{\omega^{2} \mathrm{C}}\\\end{array}Now we can solve for L.
\mathrm{L}=\mathrm{R}^{2} \mathrm{C}+1 /\left(\omega^{2} \mathrm{C}\right)\\\\ \begin{array}{l}=\left(200^{2}\right)\left(50 \times 10^{-9}\right)+1 /\left((2 \pi \times 50,000)^{2}\left(50 \times 10^{-9}\right)\right. \\\\=2 \times 10^{-3}+0.2026 \times 10^{-3}={2.203 \mathrm{mH}}\\\end{array}Checking, converting the series resistor and capacitor into a parallel combination, gives 220.3Ω in parallel with -j691.9Ω. The value of the parallel inductance is ωL =2πx50,000×2.203x10^{–3} = 692.1Ω which we need to have if we are to cancel the effect of the capacitance. The answer checks.