Question

In the circuit shown in Figure P6.12, if $$ \begin{array}{ll} L=190 \mathrm{mH} & R_1=2.3 \mathrm{k} \Omega \\ C=55 \mathrm{nF} & R_2=1.1 \mathrm{k} \Omega \end{array} $$ a. Determine how the driving point or input impedance behaves at extremely high or low frequencies. h. Find an expression for the driving point impedance in the form: $$ \begin{aligned} Z(j \omega) & =Z_\theta\left[\frac{1+j f_1[\omega]}{1+j f_2[\omega]}\right] \\ Z_p & =R_1+\frac{L}{R_2 C} \\ f_1(\omega) & =\frac{\omega^2 R_1 L C-R_1-R_2}{\omega\left[R_1 R_2 C+L\right]} \\ f_2(\omega) & =\frac{\omega^2 L C-1}{\omega C R_2} \end{aligned} $$ c. Determine the four cutoff frequencies at which $f_1(\omega)=+1$ or -1 and $f_2(\omega)=+1$ or -1 . d. Determine the resomant frequency of the circuit. e. Plot the magnitude of the impedance (in dB ) as a function of the $\log$ of the frequency, i.e., a Bode plot.

   In the circuit shown in Figure P6.12, if

$$
\begin{array}{ll}
L=190 \mathrm{mH} & R_1=2.3 \mathrm{k} \Omega \\
C=55 \mathrm{nF} & R_2=1.1 \mathrm{k} \Omega
\end{array}
$$

a. Determine how the driving point or input impedance behaves at extremely high or low frequencies.
h. Find an expression for the driving point impedance in the form:

$$
\begin{aligned}
Z(j \omega) & =Z_\theta\left[\frac{1+j f_1[\omega]}{1+j f_2[\omega]}\right] \\
Z_p & =R_1+\frac{L}{R_2 C} \\
f_1(\omega) & =\frac{\omega^2 R_1 L C-R_1-R_2}{\omega\left[R_1 R_2 C+L\right]} \\
f_2(\omega) & =\frac{\omega^2 L C-1}{\omega C R_2}
\end{aligned}
$$

c. Determine the four cutoff frequencies at which $f_1(\omega)=+1$ or -1 and $f_2(\omega)=+1$ or -1 .
d. Determine the resomant frequency of the circuit.
e. Plot the magnitude of the impedance (in dB ) as a function of the $\log$ of the frequency, i.e., a Bode plot.
Show more…
Principles and Applications of Electrical Engineering
Principles and Applications of Electrical Engineering
Giorgio Rizzoni 4th Edition
Chapter 6, Problem 12 ↓

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Step 1

Step 2: Determine behavior at extreme frequencies (part a) For extremely low frequencies (ω → 0): - The inductor L behaves like a short circuit (ZL = jωL → 0) - The capacitor C behaves like an open circuit (ZC = 1/jωC → ∞) - Therefore, Z(jω) ≈ R1 (as ω → 0) For  Show more…

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In the circuit shown in Figure P6.12, if $$ \begin{array}{ll} L=190 \mathrm{mH} & R_1=2.3 \mathrm{k} \Omega \\ C=55 \mathrm{nF} & R_2=1.1 \mathrm{k} \Omega \end{array} $$ a. Determine how the driving point or input impedance behaves at extremely high or low frequencies. h. Find an expression for the driving point impedance in the form: $$ \begin{aligned} Z(j \omega) & =Z_\theta\left[\frac{1+j f_1[\omega]}{1+j f_2[\omega]}\right] \\ Z_p & =R_1+\frac{L}{R_2 C} \\ f_1(\omega) & =\frac{\omega^2 R_1 L C-R_1-R_2}{\omega\left[R_1 R_2 C+L\right]} \\ f_2(\omega) & =\frac{\omega^2 L C-1}{\omega C R_2} \end{aligned} $$ c. Determine the four cutoff frequencies at which $f_1(\omega)=+1$ or -1 and $f_2(\omega)=+1$ or -1 . d. Determine the resomant frequency of the circuit. e. Plot the magnitude of the impedance (in dB ) as a function of the $\log$ of the frequency, i.e., a Bode plot.
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