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Microstrip LPF implementation and prototyping
Short answer
Microstrip low-pass filters are realized by stepped-impedance lines (high-Z narrow lines as series inductors, low-Z wide patches as shunt capacitors) or by Richards transformation and Kuroda identities yielding open stubs. The prototype is a normalized LC ladder with g-values from Butterworth or Chebyshev tables, scaled to desired impedance and cutoff frequency.
How is low pass filter implemented using microstrip? How are the low pass filter prototyped?
Low-pass filter in microstrip
A microwave LPF is built in microstrip by replacing the lumped L and C of a ladder prototype with short transmission-line sections. Two common forms are used.
1. Stepped-impedance (hi-Z / low-Z) filter
A short line (βl < π/4) of high impedance Z_h behaves like a series inductor. A short line of low impedance Z_ℓ behaves like a shunt capacitor:
βl = L·R0 / Zh (inductor, L normalised)
βl = C·Zℓ / R0 (capacitor, C normalised)
Z_h is made as high as can be etched (narrow strip, about 100–150 Ω), and Z_ℓ as low as practical (wide strip, about 10–20 Ω).
Stepped-impedance microstrip LPF (top view)
___ _____ ___
=====| |______| |______| |=====
50 Ω | C1| L2 | C3 | L4 | C5| 50 Ω
|___| |_____| |___|
wide = low Z0 (shunt C)
narrow = high Z0 (series L)
2. Stub filter (Richards' transformation + Kuroda identities)
- Richards' transformation maps a shunt capacitor to an open-circuited stub and a series inductor to a short-circuited series stub, each λ/8 long at fc.
- Kuroda identities change the series stubs into shunt open stubs separated by λ/8 unit elements, so all stubs are easy to make in microstrip.
open stubs (λ/8 at fc)
| | | | | |
50 Ω ==+=+======+=+======+=+== 50 Ω
unit elements (λ/8)
Prototyping of a low-pass filter
A low-pass prototype is a normalised LC ladder with source resistance g₀ = 1 Ω and cut-off ωc = 1 rad/s.
g0 g2 (L)
--/\/--+--UUU--+-- ... --+
| | g(N+1) load
g1 (C) g3 (C)
| |
--------+-------+---------
- Choose the response: Butterworth (maximally flat), PLR = 1 + (ω/ωc)²ᴺ, or Chebyshev (equal ripple), PLR = 1 + k²T_N²(ω/ωc).
- Find the order N from the required attenuation at a given stop-band frequency, using attenuation-versus-normalised-frequency charts.
- Read the g-values from tables. For Butterworth, g_k = 2 sin[(2k − 1)π/(2N)]. For example, N = 3 gives g₁ = 1, g₂ = 2, g₃ = 1.
- Scale to the real impedance R₀ and cut-off ωc: L_k = R₀ g_k / ωc and C_k = g_k / (R₀ ωc).
- Realise the elements in microstrip as above and check the response with a simulator.
✓ Answer checked by Claude Opus 5.5 (high effort)
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