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How is microstrip impedance calculated?

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Microstrip is a conductor strip of width W on a dielectric of thickness h above a ground plane. Because the field lies partly in air, it supports a quasi-TEM mode with effective permittivity between 1 and εr. Widely used closed-form approximations (Hammerstad–Jensen) give, for W/h ≥ 1, Z0 = 120π / [√εeff·(W/h + 1.393 + 0.667·ln(W/h + 1.444))].[1][2]

How is effective permittivity estimated?

εeff ≈ (εr + 1)/2 + ((εr − 1)/2)·(1 + 12h/W)−1/2. For W/h ≤ 1: Z0 = (60/√εeff)·ln(8h/W + W/(4h)).[2] These ignore conductor thickness, which slightly lowers Z0; field solvers and simulator line calculators include it.

What width gives 50 ohms?

Roughly W/h ≈ 1.9 on FR-4 (εr ≈ 4.3) and ≈ 2.2 on εr = 3.5 material; on a 0.508 mm RO4350B core, about 1.1 mm. Always confirm with the fabricator’s stackup and a field solver, since the design Dk and copper thickness shift the result.[3]

What are the limitations of microstrip?

How lossy is microstrip?

Total loss = conductor loss (∝ √f, increased by roughness) + dielectric loss αd = k0εr(εeff − 1)tan δ / (2√εeff(εr − 1)) Np/m.[2] On FR-4 at a few GHz, dielectric loss dominates.

Frequently asked questions

Is microstrip TEM?

No, quasi-TEM, because the field is in two different media.

Does solder mask change impedance?

Yes, typically lowering Z0 by a few ohms; include it in the stackup model.

When should I use CPW instead?

At high frequencies or when tight ground control and easy shunt connections are needed.

References

Online sources accessed October 21, 2026; printed works cited by edition. See all sources.

  1. “Accurate Models for Microstrip Computer-Aided Design”. E. Hammerstad and Ø. Jensen, IEEE MTT-S International Microwave Symposium Digest, pp. 407-409. 1980.
  2. “Microwave Engineering, 4th ed.”. D. M. Pozar, Wiley. 2012.
  3. “RO4000 Series High Frequency Circuit Materials data sheet (RO4350B)”. Rogers Corporation. data sheet.