Microstrip vs stripline: how to choose and how to calculate impedance
Every high-speed net on a board, from a USB pair to a DDR bus to an RF feed, lives or dies on one number: characteristic impedance. Pick the wrong trace structure or size it with the wrong formula and the line reflects its own signal back, which shows up as ringing, overshoot and, on fast links, a closed eye and intermittent failures that are miserable to debug. Almost all controlled-impedance routing uses one of two structures, the microstrip or the stripline. This guide explains how they differ, when to use each, the one input people get wrong, and why the formula behind your calculator matters more than most people realise. Where it helps, it ties back to the calculator so you can put real numbers to it.
The two structures at a glance
A microstrip is a trace on an outer layer with a single reference plane beneath it. A stripline is a trace on an inner layer, sandwiched between two planes. That one structural difference drives everything else: how the fields behave, how much the line radiates, how easy it is to route and probe, and how wide the trace has to be for a given impedance.
| Property | Microstrip | Stripline |
|---|---|---|
| Layer | Outer | Inner |
| Reference planes | One, below | Two, above and below |
| Field path | Part in air, part in board | Entirely in the dielectric |
| Effective permittivity | Between air and the laminate | The full dielectric constant |
| Radiation and EMI | Higher | Lower, shielded by planes |
| Crosstalk | Higher | Lower |
| Routing and probing | Easy, on the surface | Needs inner layers, hard to probe |
| Width for the same Z0 | Wider | Narrower |
| Best for | RF feeds, tight layer counts, surface routing | The fastest, most sensitive nets |
When a trace stops being a wire
The trigger is the signal's rise time, not its clock frequency. When the time it takes a signal to travel down a trace becomes an appreciable fraction of its rise time, the trace behaves as a transmission line and impedance matching matters. Because a square edge carries energy well above the fundamental, a modest clock with sharp edges acts like a much faster signal. In practice that means every multi-gigabit serial link, every DDR bus and most RF routing.
Characteristic impedance is fixed by the cross-section: trace width, the height to the nearest plane, the copper thickness and the dielectric constant. It does not depend on length. Length changes delay and loss, not the impedance.
Read H and B from the actual stackup
For microstrip, H is the dielectric height from the signal trace to its reference plane. For the symmetric stripline approximation in our calculator, B is the total separation between the two planes. These are different dimensions. Read both from the layer stackup instead of substituting the overall board thickness.
Why the formula behind the calculator matters
Our microstrip engine uses a piecewise thin-conductor, quasi-static approximation. It is not the complete Hammerstad–Jensen model and we do not claim a universal one-percent accuracy. The comparison below shows the implemented approximation alongside a historical IPC-2141 expression at relative permittivity 4.3. IPC currently lists IPC-2141 as “No Longer Maintained,” so the formula is presented here as a reference comparison, not a current-maintenance claim.
| W / H | Implemented approximation | IPC-2141 | Difference |
|---|---|---|---|
| 0.5 | 96.4 Ω | 98.5 Ω | +2% |
| 1.0 | 71.8 Ω | 73.2 Ω | +2% |
| 2.0 | 49.4 Ω | 48.0 Ω | -3% |
| 3.0 | 38.0 Ω | 33.2 Ω | -13% |
| 4.0 | 31.0 Ω | 22.8 Ω | -27% |
| 5.0 | 26.2 Ω | 14.6 Ω | -44% |
| 7.0 | 20.1 Ω | 2.4 Ω | -88% |
| 8.0 | 18.0 Ω | -2.5 Ω | negative |
| 10.0 | 14.9 Ω | -10.6 Ω | negative |
Stripline mode uses a separate closed-form approximation for a symmetric structure. Its validity depends on the geometry and assumptions; the calculator cannot establish the accuracy of a finished stackup.
Common impedance targets
Take the required impedance from the exact interface specification and its version. Single-ended and differential targets are not interchangeable. Enter a differential target only into a model that includes pair spacing and the intended stackup.
Differential pairs, and the limit of formulas
A differential pair needs both trace geometry and pair spacing. The calculator uses a preliminary coupling relation; validate the result against a field solver for the actual stackup rather than assuming a universal accuracy percentage.
When to reach for coplanar waveguide
At higher RF and microwave frequencies, a grounded coplanar waveguide (CPWG) is often the better choice. It places the signal trace between two coplanar ground pours, with a plane underneath, so the fields are tightly confined and the gap to the adjacent ground becomes a tuning knob alongside width and height. It also lets you route without via transitions that would otherwise break the impedance. The calculator includes a CPWG mode that uses the conductor-backed coplanar equations with exact elliptic integrals, rather than a rough approximation.
How the board house verifies it
Ask the fabricator which impedance-control process, coupon geometry, measurement method and acceptance tolerance apply to your order. Specify the target and tolerance, then agree the geometry using the actual materials. A closed-form estimate omits effects such as solder mask, copper roughness, etching shape and dispersion.
Putting it to work
Choose the structure from the routing and shielding needs, then use the correct stackup dimensions. The PCB impedance calculator provides preliminary values and a bracket-checked width solver. Confirm production geometry with the fabricator. Use the trace width calculator to examine the separate current and temperature estimates, and read the IPC comparison guide for the model limits.
References
- IPC document revision table — IPC-2141 is listed as No Longer Maintained; the 2004 IPC-2141A formula is retained here only as a historical/reference comparison.
- On the accuracy of microstrip impedance formulas: Wheeler and Hammerstad-Jensen versus IPC-2141
- Coplanar waveguide impedance by conformal mapping (Steer, Microwave and RF Design II)