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Justify insertion loss method for filter design

Short answer

Insertion loss method synthesises from power loss ratio PLR=1/(1−|Γ|²), giving exact specified response and real terminations, unlike image method. Choose Butterworth/Chebyshev PLR, find order N, use g tables, scale/transform, implement with transmission lines.

Justify and describe how a microwave filter is designed using insertion loss method.

In the insertion loss method, the filter is synthesised directly from a chosen power loss ratio PLR(ω), so the complete frequency response is controlled from the start.

Justification

Image parameter methodInsertion loss method
Cascades constant-k and m-derived sectionsSynthesises the whole network
Response is not exactly specifiedResponse specified exactly
Needs iteration to meet specsSystematic, table based
Termination mismatch ignoredReal terminations included
No direct trade-offTrades order vs roll-off vs ripple

Hence it gives optimum, repeatable designs, and it is the standard method for microwave filters.

Description of the method

  1. Specify fc (or band edges), R0, passband ripple and stopband attenuation.
  2. Choose the response:
PLR = 1/(1 − |Γ(ω)|²),  IL = 10 log PLR
Butterworth:   PLR = 1 + k²(ω/ωc)^(2N)
Chebyshev:     PLR = 1 + k²·TN²(ω/ωc)
Linear phase:  flat group delay
  1. Find the order N from the stopband specification. Example: Butterworth, 15 dB at 2fc: N ≥ log(10^1.5 − 1)/(2 log 2) = 2.47 → N = 3.
  2. Low-pass prototype values gk from tables (R0 = 1, ωc = 1): for N = 3 Butterworth, 1, 2, 1.
  3. Scaling and transformation: L = gR0/ωc, C = g/(R0ωc); LP → HP, BP, BS by frequency substitution. For fc = 2 GHz, R0 = 50 Ω: C = 1.59 pF, L = 7.96 nH.
  4. Implementation: lumped elements become transmission-line sections using Richards' transformation, Kuroda identities, stepped-impedance lines or coupled lines.
  5. Simulate and tune, including junction and step discontinuities, then fabricate.

✓ Answer checked by Claude Opus 5.5 (high effort)

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