Controlled Impedance
How Trace Geometry Sets Z0
A transmission line on a circuit board behaves as a distributed network of series inductance and shunt capacitance per unit length. Its characteristic impedance is the square root of that inductance-to-capacitance ratio, which means the value is governed entirely by physical geometry and the surrounding dielectric, not by the line length or the source. Widen the trace and the shunt capacitance to the reference plane rises while the loop inductance falls, so the impedance drops. Move the trace farther from the plane (thicker dielectric) and the impedance climbs. Controlled-impedance design is the discipline of pinning these geometric variables so that every impedance-critical net lands on the target value across the whole panel.
The dominant structures are microstrip, a trace on an outer layer above a single ground plane, and stripline, a trace buried between two ground planes. Microstrip is easier to route and probe but its field straddles both the substrate and the air above it, so its effective permittivity is a weighted average that shifts when solder mask is added. Stripline sits in a homogeneous dielectric, giving a cleaner, mask-immune impedance and slightly slower propagation. For RF boards the most common choice is grounded coplanar waveguide, a microstrip variant with adjacent ground pours that give the designer a second geometric knob (the gap) for hitting 50 Ω while suppressing surface-wave coupling.
Material selection matters as much as geometry. FR-4 has a relative permittivity near 4.3 that drifts with frequency and resin content, which limits its accuracy above a few gigahertz, so millimeter-wave assemblies move to PTFE-based laminates such as Rogers RO4350B or RT/duroid, where the permittivity is tightly specified. The fabricator verifies the result with a time-domain reflectometer on a dedicated impedance coupon and reports the measured value against the target on the fab drawing.
Microstrip and Stripline Impedance Equations
Z0 = √(L / C) ≈ √(L0 / C0) per unit length
Microstrip (IPC-2141 / Wheeler approximation, 0.1 < W/h < 2):
Z0 ≈ (87 / √(εr + 1.41)) × ln(5.98h / (0.8W + t)) Ω
Symmetric Stripline (thin trace):
Z0 ≈ (60 / √εr) × ln(4b / (0.67π(0.8W + t))) Ω
Where W = trace width, t = copper thickness, h = dielectric height above the plane, b = plate separation (stripline), εr = relative permittivity. Example: microstrip, εr = 3.66 (RO4350B), h = 10 mil, t = 0.6 mil → the equation gives Z0 ≈ 50 Ω at W ≈ 20 mil (W/h = 2.0).
Stackup and Geometry Comparison
| Structure | Reference | 50 Ω Width (10 mil h) | Mask Sensitive | Loss | Best Use |
|---|---|---|---|---|---|
| Microstrip (FR-4) | 1 plane | ~18 mil | Yes (1 to 3 Ω) | Moderate | Low-cost RF, sub-6 GHz |
| Microstrip (RO4350B) | 1 plane | ~20 mil | Yes | Low | mmWave front ends |
| Grounded CPW | 1 plane + side pours | Set by gap + width | Reduced | Low | Dense RF routing |
| Symmetric stripline | 2 planes | ~9 mil (b = 20 mil) | No | Higher | High-precision digital/RF |
| Differential pair | 1 to 2 planes | 100 Ω diff (gap-set) | Yes (microstrip) | Moderate | SerDes, LVDS, USB |
Frequently Asked Questions
What trace width gives 50 ohms on a typical RF board?
It depends on the stackup. On microstrip over 10 mil FR-4 (εr ≈ 4.3) a single trace needs roughly 18 to 19 mil for 50 Ω; on 10 mil RO4350B (εr 3.66) it widens to about 20 mil because the lower permittivity demands a wider conductor. Halving the dielectric height roughly halves the width. Fix the stackup first, then solve for W with a 2D field solver or the microstrip closed form. Grounded coplanar waveguide adds the ground gap as a second tuning knob.
What tolerance can a fabricator hold on controlled impedance?
Standard fabrication holds ±10%, so a 50 Ω trace lands between 45 and 55 Ω. Premium RF processes with TDR-verified coupons hold ±5% (47.5 to 52.5 Ω). The error budget comes from etch variation (±0.5 to 1 mil on width), dielectric thickness spread of ±10% on FR-4, copper roughness, and solder mask. Each panel carries an impedance coupon the fab measures and reports against the target.
Does solder mask change microstrip impedance?
Yes. A 0.5 to 1 mil mask layer (εr ≈ 3.3 to 3.9) over a microstrip trace raises the effective permittivity and lowers Z0 by roughly 1 to 3 Ω versus bare copper. Designers either model the mask in the field solver or specify exposed copper over impedance-critical traces. Buried stripline is immune, which is one reason high-precision controlled-impedance routing favors stripline despite higher loss and harder rework.