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Leapfrog 4th order Butterworth LPF at 1000 rad/s

Short answer

Leapfrog simulation replaces LC ladder elements with op-amp integrators, preserving low sensitivity. For 4th-order Butterworth at 1000 rad/s using prototype L1=0.7654, C2=1.848, L3=1.848, C4=0.7654 and R=10kΩ, integrator capacitors are A1/A5: 76.54 nF, A2/A4: 184.8 nF; two inverters complete the circuit.

Design the fourth order Butterworth low-pass filter in resistively terminated lossless realization using a leapfrog simulation. Your final design should accommodate half power frequency of 1000 rad/sec and should have practically realizable elements in it. [Table: doubly terminated Butterworth element values normalized to 1 rad/s, 1 Ω terminations: n = 2: 1.414, 1.414; n = 3: 1, 2, 1; n = 4: 0.7654, 1.848, 1.848, 0.7654; n = 5: 0.618, 1.618, 2, 1.618, 0.618]

Leapfrog (operational) simulation realises the doubly terminated LC ladder by simulating its equations rather than its elements: each reactive element is replaced by an op-amp integrator, and the integrators are coupled exactly as the ladder voltages and currents are coupled. The result keeps the low sensitivity of the passive ladder.

From the table (n = 4), the doubly terminated Butterworth prototype (1 Ω terminations, ω0=1\omega_0 = 1 rad/s) is Rs=1R_s = 1, L1=0.7654L_1 = 0.7654 H, C2=1.848C_2 = 1.848 F, L3=1.848L_3 = 1.848 H, C4=0.7654C_4 = 0.7654 F, RL=1 ΩR_L = 1\ \Omega (T-ladder: series L first, shunt C to ground).

Write the state equations of the doubly terminated ladder (normalised, Rs=RL=1 ΩR_s = R_L = 1\ \Omega). Every current is turned into a voltage by multiplying by a 1 Ω resistance, so each equation becomes an integrator:

I1=Vin−V2sL1+1V2=I1−I3sC2I3=V2−V4sL3V4=I3sC4+1Vo=V4\begin{aligned} I_1 &= \frac{V_{in} - V_2}{sL_1 + 1} \\ V_2 &= \frac{I_1 - I_3}{sC_2} \\ I_3 &= \frac{V_2 - V_4}{sL_3} \\ V_4 &= \frac{I_3}{sC_4 + 1} \\ V_o &= V_4 \end{aligned}

The first and last equations are lossy integrators (the terminations give the "+1"); the middle ones are lossless integrators. Neighbouring integrators feed each other in alternate directions, which gives the "leapfrog" structure.

Using inverting op-amp integrators, Vo=−1sRC∑ViV_o = -\frac{1}{sRC}\sum V_i (lossless) or Vo=−∑Vi/RsC+1/RV_o = -\frac{\sum V_i/R}{sC + 1/R} (lossy, resistor RR across CC), the signs are arranged as follows. Inverters supply the signals of opposite sign:

Op-ampTypeInputs (each through RR)OutputNormalised CC (R = 1 Ω)
A1lossy integratorVinV_{in}, −V2-V_2−I1-I_10.7654 F
A2integrator−I1-I_1, I3I_3V2V_21.848 F
A3inverterV2V_2−V2-V_2R / R
A4integrator−V2-V_2, V4V_4I3I_31.848 F
A5lossy integratorI3I_3−V4-V_40.7654 F
A6inverter−V4-V_4V4=VoV_4 = V_oR / R

Check of one stage: A2 gives −(−I1)+I3sCA2=I1−I3s(1.848)-\frac{(-I_1) + I_3}{sC_{A2}} = \frac{I_1 - I_3}{s(1.848)}, which is the ladder equation for V2V_2.

Denormalisation. Frequency scale by ω0=1000 rad/s\omega_0 = 1000\ \text{rad/s} and choose all resistors RR = 10 kΩ (impedance scale kz=104k_z = 10^4). Each capacitor becomes C=g/(ω0R)C = g/(\omega_0 R):

CA1=0.76541000×104=76.54 nFCA2=1.8481000×104=184.8 nFCA4=1.8481000×104=184.8 nFCA5=0.76541000×104=76.54 nF\begin{aligned} C_{A1} &= \frac{0.7654}{1000 \times 10^4} = \text{76.54 nF} \\ C_{A2} &= \frac{1.848}{1000 \times 10^4} = \text{184.8 nF} \\ C_{A4} &= \frac{1.848}{1000 \times 10^4} = \text{184.8 nF} \\ C_{A5} &= \frac{0.7654}{1000 \times 10^4} = \text{76.54 nF} \end{aligned}

Final element values:

Op-ampResistorsCapacitor
A1input(s) 10 kΩ, feedback 10 kΩ across C76.54 nF
A2input(s) 10 kΩ184.8 nF
A4input(s) 10 kΩ184.8 nF
A5input(s) 10 kΩ, feedback 10 kΩ across C76.54 nF
inverters10 kΩ in, 10 kΩ feedbacknone
 Lossy integrator (A1 and A5)
              +-----[ C ]-----+
              |               |
              +-----[ R ]-----+
              |               |
 Va --[R]-----+---|-\         |
 Vb --[R]-----+   |  >--------+---- Vo
              GND-|+/
 Lossless integrator (A2 and A4): the same circuit
 without the feedback resistor (only C from output to (-)).

The passband gain is 1/2 (−6 dB), the same as the doubly terminated prototype; the response is that of the passive ladder but with no inductors, and the low sensitivity of the ladder is kept.

Answer: six op-amps (four integrators, two inverters), all resistors 10 kΩ, integrator capacitors 76.54 nF, 184.8 nF, 184.8 nF and 76.54 nF; half-power frequency 1000 rad/s.

✓ Answer checked by Claude Sonnet 5.5

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