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Figure 141 104rad/s10^{4} \mathrm{rad} / \mathrm{s} , and a Maximum Deviation in the Passband Transmission Of Low-Pass

Question 4

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     Figure 14.1.1 It is required to design a fifth-order Butterworth low-pass filter with a de gain of unity, a passband edge of  10^{4} \mathrm{rad} / \mathrm{s} , and a maximum deviation in the passband transmission of  3 \mathrm{~dB}  (i.e.,  \epsilon=1  ). (a) Find the transfer function  T(s)  and give  \omega_{0}  and  Q  of each of the two pairs of complex-conjugate poles. Also, specify the frequency of the real pole.  (b) Provide a complete circuit realization of the filter as a cascade of two second-order sections and a first-order section. For the second-order sections, use realizations based on the inductancesimulation circuit of Fig. 14.1.1. For the first-order section, use an op amp-RC circuit. Design so that all capacitors are equal to  10 \mathrm{nF}  and as many of the resistors as possible are equal. Give the complete circuit and specify the values of all resistors.  (c) What is the attenuation achieved at the stopband edge,  2 \times 10^{4} \mathrm{rad} / \mathrm{s}  ?

Figure 14.1.1
It is required to design a fifth-order Butterworth low-pass filter with a de gain of unity, a passband edge of 104rad/s10^{4} \mathrm{rad} / \mathrm{s} , and a maximum deviation in the passband transmission of 3 dB3 \mathrm{~dB} (i.e., ϵ=1\epsilon=1 ).
(a) Find the transfer function T(s)T(s) and give ω0\omega_{0} and QQ of each of the two pairs of complex-conjugate poles. Also, specify the frequency of the real pole.
(b) Provide a complete circuit realization of the filter as a cascade of two second-order sections and a first-order section. For the second-order sections, use realizations based on the inductancesimulation circuit of Fig. 14.1.1. For the first-order section, use an op amp-RC circuit. Design so that all capacitors are equal to 10nF10 \mathrm{nF} and as many of the resistors as possible are equal. Give the complete circuit and specify the values of all resistors.

(c) What is the attenuation achieved at the stopband edge, 2×104rad/s2 \times 10^{4} \mathrm{rad} / \mathrm{s} ?

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