Skin Depth Calculator (Skin Effect)
How deep alternating current really flows in a conductor at a given frequency, the largest strand worth using, and an estimate of the extra AC resistance.
Results
The dashed line marks the value you entered.
What this tool does
Alternating current does not use the whole wire: the eddy currents it induces push it towards the surface, and the current density drops by a factor of e for every skin depth. In copper that depth is about 9 mm at 50 Hz but only about 0.2 mm at 100 kHz and 6.5 µm at 100 MHz, which is why switch-mode transformers use litz wire and radio conductors are often silver-plated tubes. A magnetic material shrinks it much further, so steel has a far smaller skin depth than copper despite its higher resistivity. The resistance ratio treats the current as filling a ring one skin depth thick — a good estimate once the wire is several skin depths across.
Formula
δ = √(ρ ÷ (π f μ₀ μᵣ))
Variables
| Symbol | Meaning | Unit |
|---|---|---|
f | Frequency | kHz |
ro | Resistivity | nΩ·m |
mr | Relative permeability µr | — |
dw | Conductor diameter | mm |
D | Skin depth | mm |
MS | Largest strand worth using (2δ) | mm |
RR | AC to DC resistance (estimate) | × |
Worked example
- Frequency100 kHz
- Resistivity16.8 nΩ·m
- Relative permeability µr1
- Conductor diameter1 mm
- Skin depth0.206288 mm
- Largest strand worth using (2δ)0.412577 mm
- AC to DC resistance (estimate)1.53 ×
Limitations
- The result is an estimate based only on the values you type. Real situations often include factors this calculator does not know about.
- The default values are typical reference figures, not measurements of your situation. Replace them with your own data whenever you have it.