Skip to main content

5th order Butterworth LPF with first-order and MFB sections

Short answer

First-order section: R=1.592 kΩ, C=0.1 μF. Two MFB biquads with R1=R2=R3, C1=3Q, C2=1/(3Q) scaled to ω0=6283.2 rad/s, largest C1=0.1 μF. Section 1 (Q=1.618): R=7.726 kΩ, C1=0.1 μF, C2=4.244 nF. Section 2 (Q=0.618): R=2.951 kΩ, C1=0.1 μF, C2=29.09 nF. Overall DC gain magnitude 1.

Design a 5th order Butterworth LPF using cascade of 1st order active section and MFB biquads with DC gain equal to unity and half power frequency at 1 kHz. Make the largest capacitance 0.1 μF.

Butterworth poles (n = 5) lie on the unit circle at 0°, ±36° and ±72° from the negative real axis, so

TN(s)=1(s+1)(s2+0.618s+1)(s2+1.618s+1)T_N(s) = \frac{1}{(s+1)(s^2 + 0.618s + 1)(s^2 + 1.618s + 1)}

Each quadratic s2+(1/Q)s+1s^2 + (1/Q)s + 1 gives Q=1/0.618=1.618Q = 1/0.618 = 1.618 and Q=1/1.618=0.618Q = 1/1.618 = 0.618. The filter is one first-order section followed by two MFB biquads; ω0=2π(1000)=6283.2\omega_0 = 2\pi(1000) = 6283.2 rad/s.

First-order section

An inverting lossy integrator: input R1R_1, feedback Rf∥CR_f \parallel C:

T1(s)=−1/(R1C)s+1/(RfC)T_1(s) = -\frac{1/(R_1C)}{s + 1/(R_fC)}

Normalised: R1=Rf=1 ΩR_1 = R_f = 1\ \Omega, C=1C = 1 F (pole at 1, gain 1). Scaling with CC = 0.1 μF: R=1/(ω0C)=1/(6283.2×10−7)R = 1/(\omega_0 C) = 1/(6283.2 \times 10^{-7}) = 1.592 kΩ for both R1R_1 and RfR_f.

          +---[Rf]---+
          +---| C |--+
 Vi-[R1]--+--(-)     |
              A -----+--o
     GND --(+)

MFB biquads

              +----------[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 = 6283.2 rad/s. For each section choose kzk_z so that its largest capacitor C1C_1 becomes 0.1 μF: kz=C1n/(ω0×10−7)k_z = C_{1n}/(\omega_0 \times 10^{-7}). Then all three resistors are kzk_z and C2=C2n/(kzω0)C_2 = C_{2n}/(k_z\omega_0). (Each section is driven by an op-amp output, so sections may be scaled separately.)

SectionQC1nC_{1n}C2nC_{2n}R1=R2=R3R_1 = R_2 = R_3C1C_1C2C_2
s2+0.618s+1s^2 + 0.618s + 11.6184.8541 F0.2060 F7.726 kΩ100 nF4.244 nF
s2+1.618s+1s^2 + 1.618s + 10.6181.8541 F0.5393 F2.951 kΩ100 nF29.09 nF

Final circuit

 Vi -->[1st order]-->[MFB, Q=1.618]-->[MFB, Q=0.618]--> Vo
       R=1.592k        R=7.726k          R=2.951k
       C=0.1uF         C1=0.1uF          C1=0.1uF
                       C2=4.244nF        C2=29.09nF

Each stage has DC gain −1, so the overall DC gain magnitude is 1 (sign −1; add a unity inverter if a positive output is needed). Half-power frequency 1 kHz.

Answer: first-order: R = 1.592 kΩ, C = 0.1 μF; MFB 1 (Q = 1.618): R = 7.726 kΩ, C1 = 0.1 μF, C2 = 4.244 nF; MFB 2 (Q = 0.618): R = 2.951 kΩ, C1 = 0.1 μF, C2 = 29.09 nF.

✓ Answer checked by Claude Sonnet 5.5

All Filter Design chapter 8 questions →