Tool 09 · Available

Impedance Matching Designer

Synthesize and verify L matches or a quarter-wave transformer at one design frequency.

Engineering question

Which lossless branch transforms this load to the selected real system impedance?

Single-frequency matching synthesis

The objective is zero voltage-wave Γ for a positive real system impedance. That is not a claim of arbitrary complex-source power-wave or conjugate matching.

Preferred response ordering
Selected practical branchseries L 79.5775 nH · shunt C 15.9155 pFExact values · 2 mathematically valid branches
Source
50 Ω
series
L 79.5775 nH
shunt
C 15.9155 pF
Load
100 + j0 Ω
Exact synthesis residual
0 Ω
Practical Zin
50.00000 + j0.00000 Ω
Practical Γ / VSWR
0.000000 / 1.00000
Practical return loss
∞ dB
Ideal insertion loss
0.000000 dB
includes residual mismatch; ideal reactive parts
Lossy response, Q 100
0.08664 dB
series-loss component model
Worst corner, ±1.00%
42.9672 dB RL
Design frequency
100.0000 MHz
Every valid branch is retained; the preference only changes ordering.
BranchExact componentsForward residual
1. Series L then shunt Cseries L 79.5775 nH; shunt C 15.9155 pF0 Ω
2. Series C then shunt Lseries C 31.831 pF; shunt L 159.155 nH0 Ω
Ideal-network RMS stress at 0.000 dBm available source power; use for screening only.
ComponentVoltageCurrent
1. series L 79.5775 nH223.607 mVrms4.47214 mArms
2. shunt C 15.9155 pF316.228 mVrms3.16228 mArms

Calculation path

  1. The exact network is independently solved as a circuit; preferred values, tolerance corners, and finite-Q parts are then evaluated separately.
  2. Perfect f₀ math excludes interconnect, pad/via parasitics, self-resonance, bias, temperature, and measured load movement.
  3. Verify the assembled network with a calibrated VNA at the intended reference plane.

What this calculator is doing

Ideal reactive networks are synthesized at one frequency and independently re-evaluated with the complex circuit model. L branches accept complex loads; the bounded π/T implementation states its real-load condition.

How to read the result

Choose a branch for harmonic response, bias paths, parasitics, stress, and available component Q. Verify the built network at its real reference plane.

Equations & conventions

  • Zin(f0)=Z0+j0Z_{\mathrm{in}}(f_{0}) = Z_{0} + j 0
  • Zt=R1R2for a real quarter-wave matchZ_t=\sqrt{R_1R_2}\quad\text{for a real quarter-wave match}
  • Z0 is positive real source/system resistance; ZL = R + jX is the load.
  • Q is loaded network selectivity for π/T synthesis.
  • Component Q estimates first-order reactive loss, not full parasitics.

Independently checked example

Checked example: matching 100 + j0 Ω to 50 Ω at 100 MHz yields two ideal L branches; both re-evaluate to 50 + j0 Ω within floating-point tolerance.

Common mistakes

  • Assuming a single-frequency match guarantees bandwidth.
  • Ignoring component self-resonance and layout parasitics.

Assumptions, validity & omissions

  • The source/system reference is positive and real.
  • L matches are narrowband ideal lumped models.
  • Quarter-wave synthesis requires real positive terminal resistances.

Sources & model provenance

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