How do you design an LC filter from a prototype?
LC filter design starts from normalized low-pass prototype values gk, then applies impedance scaling (multiply L by R0, divide C by R0) and frequency scaling (divide by ωc). For a low-pass: Lk = gkR0/ωc, Ck = gk/(R0ωc). Band-pass filters replace each element with a resonator.[1]
What is a worked low-pass example?
Third-order Butterworth, 50 Ω, fc = 100 MHz, shunt-C first. g = 1, 2, 1. C1 = C3 = 1/(50·2π·108) ≈ 31.8 pF; L2 = 2·50/(2π·108) ≈ 159 nH.
How is the band-pass transformation done?
With center ω0 = √(ω1ω2) and fractional bandwidth Δ = (ω2 − ω1)/ω0, each series inductor becomes a series LC with L = g·R0/(ω0Δ), C = Δ/(ω0·g·R0); each shunt capacitor becomes a parallel LC with C = g/(ω0ΔR0), L = ΔR0/(ω0g). Narrow bandwidths give impractical value spreads, which coupled-resonator topologies avoid.[1][2]
What practical issues arise?
- Choose components with self-resonant frequency well above the passband (for low-pass, above the stopband you must reject).
- Use standard values and re-optimize; check sensitivity with Monte Carlo.
- Pad and via parasitics shift response above a few hundred MHz; include them in simulation.
- Shield or separate input and output to preserve stopband rejection.
Frequently asked questions
Shunt-first or series-first?
Both are valid duals; choose based on available values and termination needs.
What limits LC filter frequency?
Component self-resonance, Q and parasitics, practically a few GHz.
Why do narrow filters use coupled resonators?
Direct transformation yields extreme L and C ratios; coupled resonators keep values practical.
See also
References
Online sources accessed October 21, 2026; printed works cited by edition. See all sources.
- “Microwave Engineering, 4th ed.”. D. M. Pozar, Wiley. 2012.
- “Microwave Filters, Impedance-Matching Networks, and Coupling Structures”. G. Matthaei, L. Young, E. M. T. Jones, McGraw-Hill / Artech House. 1964; Artech reprint 1980.