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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, rad/s) is , H, F, H, F, (T-ladder: series L first, shunt C to ground).
Write the state equations of the doubly terminated ladder (normalised, ). Every current is turned into a voltage by multiplying by a 1 Ω resistance, so each equation becomes an integrator:
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, (lossless) or (lossy, resistor across ), the signs are arranged as follows. Inverters supply the signals of opposite sign:
| Op-amp | Type | Inputs (each through ) | Output | Normalised (R = 1 Ω) |
|---|---|---|---|---|
| A1 | lossy integrator | , | 0.7654 F | |
| A2 | integrator | , | 1.848 F | |
| A3 | inverter | R / R | ||
| A4 | integrator | , | 1.848 F | |
| A5 | lossy integrator | 0.7654 F | ||
| A6 | inverter | R / R |
Check of one stage: A2 gives , which is the ladder equation for .
Denormalisation. Frequency scale by and choose all resistors = 10 kΩ (impedance scale ). Each capacitor becomes :
Final element values:
| Op-amp | Resistors | Capacitor |
|---|---|---|
| A1 | input(s) 10 kΩ, feedback 10 kΩ across C | 76.54 nF |
| A2 | input(s) 10 kΩ | 184.8 nF |
| A4 | input(s) 10 kΩ | 184.8 nF |
| A5 | input(s) 10 kΩ, feedback 10 kΩ across C | 76.54 nF |
| inverters | 10 kΩ in, 10 kΩ feedback | none |
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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