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Quarter-Wave Transformer Calculator (lambda/4 Impedance Match)

Single-section quarter-wave transformer between Z1 and Z2. Returns the geometric-mean Zt, the lambda_g/4 length, and the three microstrip section widths (W1, Wt, W2) on your stackup.

Quarter-Wave Transformer Calculator

A lambda_g/4 line of impedance sqrt(Z1 Z2) matches Z2 to Z1 at a single frequency. Lay out all three sections (Z1, Zt, Z2) on your microstrip stackup in one go.

Units
Length
Frequency

Inputs

Impedances and frequency
Ω
Ω
GHz
Microstrip stackup
mm
Z₁ = 50.0 ΩZt = 100.0 ΩZ₂ = 200.0 Ωλg/4 = 18.915 mm
Quarter-wave transformer
Transformer Zt
100.00Ω
Section length
18.915mm
744.67 mil

Microstrip widths

W1 (source side)1.112 mm
Wt (transformer)0.276 mm
W2 (load side)0.021 mm

More

Pre-match Γ0.600
Pre-match return loss4.4 dB
Effective eeff (Zt section)2.616
Guided lambda_g75.66 mm

Analytical calculation

Every step the calculator runs, with the formula, your numbers plugged in, and the result.

Transformer impedance
A lambda/4 line matches via the geometric mean of source and load.
Pre-match reflection
What you would see if you skipped the transformer.
Microstrip widths
Solve Hammerstad-Jensen W(Z) on this stackup so each section is laid out, not just sized.
Effective permittivity (Zt section)
Use the Zt section's eeff so the lambda_g/4 length matches what you will fabricate.
Section length
Guided quarter-wave at f0.

References

  • PrimaryPozar, D. M. Microwave Engineering, 4th ed., Wiley 2011, Sec. 5.4 (single-section quarter-wave transformer). Section length is lambda_g/4 with eeff drawn from the Zt section's microstrip geometry.
  • Microstrip layoutHammerstad, E. & Jensen, O. 1980 (per-section width and the section eeff that drives the lambda_g/4 length).
  • ConceptQuarter-wave impedance transformer (overview)

Closed-form is just the start.

These calculators hand you the analytical starting point. RayRF takes you the rest of the way: antennas, filters, feedlines, and more, simulated on your real stackup with copper losses, dielectric loss, and finite ground. Roughly a second per iteration.

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