AC Resistance, Skin Effect & Trace Loss
The AC resistance of a real trace, the loss it produces, and the frequency where the laminate takes over from the copper.
Inputs
Board profileFills Copper weight and Dielectric constant (Dk) from your board profile.
Results
Checked: loss over 254 mm at 5 GHz ≤ the 10.0 dB allowance, at the rough end of the band
23.4× the DC value
All results (10)
at most 2
the smooth end of the band
32.5 inches at this frequency
same model as Controlled Impedance & Delay
Trace loss alone does not decide whether a link works. Reflections, crosstalk and the receiver equaliser matter too, and none are modelled here. Confirm with a channel simulation.
Roughness puts the loss over this length between 2.87 dB (smooth) and 3.08 dB. The Hammerstad correction caps conductor loss at twice the smooth-copper value, so it cannot represent rougher foil.
Conductor and dielectric loss are equal at 4.941 GHz. Below it, widen the trace or use smoother foil; above it, the laminate matters most.
Roughness is entered as RMS. Fabs often quote Rz, Ra or a foil class instead, which are different. If yours is not RMS, use the whole band.
Accuracy
- Wheeler (1942)
- Hammerstad and Jensen (1980)
- Hammerstad and Bekkadal
Wheeler, Formulas for the Skin Effect, Proceedings of the IRE (1942) the equation
Hammerstad and Jensen, Accurate Models for Microstrip Computer-Aided Design (1980) the equation
Hammerstad and Bekkadal, A Microstrip Handbook, University of Trondheim fitted to measurements
- Dielectric constant (Dk) 1 to 20
Dielectric constant (Dk) The impedance model was fitted for ordinary laminate permittivities. Outside that range it is not reliable enough to differentiate.
For microstrip the √ε_eff form leaves out the filling factor, so it overstates dielectric loss somewhat, on the safe side. Conductor loss uses Wheeler’s rule, which reproduces the exact coaxial result. Foil roughness and the loss tangent at your frequency move the answer most, so roughness is shown as a band and the verdict uses its rough end.
Most of the uncertainty comes from Foil roughness, RMS. Tighten that first.
6 independent cases. See the working.
This is a design aid. The engineer remains responsible for the design and for checking the standard itself.
Parameter sweep
Vary one input over a range and see the answer and verdict at each step, as a table and a curve.ProWorst-case corners
Put a tolerance on each input and get the worst-case band around the answer.ProGive at least one input a tolerance above zero.
Cross-section
The principle
Trace loss has two parts. Copper loss rises with the square root of frequency as the skin depth shrinks; dielectric loss rises linearly. The frequency where they cross decides the fix: below it, a wider trace and smoother foil; above it, a better laminate.
- skin depth
- surface resistance, ohms per square
- foil roughness, RMS
- Hammerstad roughness factor, between 1 and 2
- conductor attenuation
- dielectric attenuation
- effective permittivity of the line
- characteristic impedance, from the same model as the impedance page
More detail
A simple strip formula, ρ/(δw), misses the current crowding to the edges and underside of the trace, and the loss in the return plane. Wheeler’s rule captures both.
Not included: reflections at via stubs, connectors, AC coupling capacitors and package transitions; fibre weave; crosstalk. This is a matched, uniform line.
Engine version 1.18.3