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4th order Butterworth LPF with two MFB biquads

Short answer

Two MFB biquads with R1=R2=R3, C1=3Q, C2=1/(3Q) scaled to ω0=1000 rad/s, C1=0.1 μF. Section 1 (Q=0.5412): R=16.24 kΩ, C1=0.1 μF, C2=37.94 nF. Section 2 (Q=1.3066): R=39.2 kΩ, C1=0.1 μF, C2=6.509 nF. DC gain +1.

Design a 4th order Butterworth LPF using cascade two MFB biquads with dc gain equal to unity and half power frequency at 1000rad/sec. Make the largest capacitance equal to 0.1 μF in your final circuit.

Butterworth poles (n = 4) lie at ±22.5° and ±67.5° from the negative real axis on the unit circle:

TN(s)=1(s2+1.8478s+1)(s2+0.7654s+1)T_N(s) = \frac{1}{(s^2 + 1.8478s + 1)(s^2 + 0.7654s + 1)}

so the two biquads have Q1=1/1.8478=0.5412Q_1 = 1/1.8478 = 0.5412 and Q2=1/0.7654=1.3066Q_2 = 1/0.7654 = 1.3066, with ω0\omega_0 = 1000 rad/s.

MFB lowpass biquad

              +----------[R2]-----------+
              |                         |
              |       +----[C2]----+    |
              |       |            |    |
 Vi o--[R1]---+--[R3]-+----(-)     |    |
              |              A ----+----+--o Vo
             [C1]     GND---(+)
              |
             GND

For this multiple-feedback (MFB) lowpass biquad:

T(s)=VoVi=−1R1R3C1C2s2+sC1(1R1+1R2+1R3)+1R2R3C1C2,T(0)=−R2R1T(s) = \frac{V_o}{V_i} = \frac{-\dfrac{1}{R_1R_3C_1C_2}}{s^2 + \dfrac{s}{C_1}\left(\dfrac{1}{R_1} + \dfrac{1}{R_2} + \dfrac{1}{R_3}\right) + \dfrac{1}{R_2R_3C_1C_2}}, \qquad T(0) = -\frac{R_2}{R_1}

Normalised design (ω0=1\omega_0 = 1, unity DC gain): take R1=R2=R3=1 ΩR_1 = R_2 = R_3 = 1\ \Omega. Then ω02=1/(C1C2)=1\omega_0^2 = 1/(C_1C_2) = 1 and ω0/Q=3/C1\omega_0/Q = 3/C_1, so

C1=3Q,C2=13QC_1 = 3Q, \qquad C_2 = \frac{1}{3Q}

Scaling

ω0\omega_0 = 1000 rad/s. In each section set C1C_1 (the larger capacitor) to 0.1 μF: kz=C1n/(ω0×10−7)k_z = C_{1n}/(\omega_0 \times 10^{-7}); then R1=R2=R3=kzR_1 = R_2 = R_3 = k_z and C2=C2n/(kzω0)C_2 = C_{2n}/(k_z\omega_0).

SectionQC1nC_{1n}C2nC_{2n}R1=R2=R3R_1 = R_2 = R_3C1C_1C2C_2
s2+1.8478s+1s^2 + 1.8478s + 10.54121.6236 F0.6159 F16.24 kΩ100 nF37.94 nF
s2+0.7654s+1s^2 + 0.7654s + 11.30663.9197 F0.2551 F39.2 kΩ100 nF6.509 nF

Check for section 2: ω0=1/R2C1C2=1/(39.2k)2(10−7)(6.509×10−9)≈1000\omega_0 = 1/\sqrt{R^2C_1C_2} = 1/\sqrt{(39.2\text{k})^2(10^{-7})(6.509 \times 10^{-9})} \approx 1000 rad/s.

Final circuit

 Vi -->[MFB 1, Q=0.5412]-->[MFB 2, Q=1.3066]--> Vo
         R = 16.24k             R = 39.2k
         C1 = 0.1uF             C1 = 0.1uF
         C2 = 37.94nF           C2 = 6.509nF

Each section has DC gain −1, so the cascade has DC gain +1 (unity) and half-power frequency 1000 rad/s.

Answer: section 1: R1=R2=R3R_1 = R_2 = R_3 = 16.24 kΩ, C1C_1 = 0.1 μF, C2C_2 = 37.94 nF; section 2: R1=R2=R3R_1 = R_2 = R_3 = 39.2 kΩ, C1C_1 = 0.1 μF, C2C_2 = 6.509 nF.

✓ Answer checked by Claude Sonnet 5.5

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