Engineering calculators

Skin Depth Calculator

Updated Sep 21, 2026 By Infinity Calculator
Rate Formulas

Inputs

Choosing a preset fills in resistivity and relative permeability. Select Custom to edit them yourself.
Most values are in the range of 0.01–10 μΩ·m. To convert Ω·m to μΩ·m, multiply by 1×10⁶.
For most non-magnetic metals (copper, aluminum, gold, silver), μᵣ = 1. Ferromagnetic materials such as nickel or carbon steel can have μᵣ values ranging from 100 to several hundred.

Output Format

Number format for all results

Results

Conductivity (σ)
Resistivity (ρ)
Skin Depth (δ)
In micrometres
In micro-inches

Step-by-Step Solution

Conductor Cross-Section

Range: 0.1 – 10 mm
Skin depth δ:
Radius R:
δ / R:

Cross-section of a round conductor. The hatched outer ring marks the skin-depth region carrying most of the alternating current, and the dotted inner circle marks the core where current is largely excluded.

Diagonal hatch — Skin depth region (outer shell, carries most of the current)
Dotted fill — Core (current largely excluded)

Skin Depth vs. Frequency

Additional Metrics

Skin Depths Across Reference Conductor Diameter
A value greater than 1 indicates significant skin effect. A value less than 1 means current penetrates the full conductor.
Effective Conducting Shell Area
Share of the circular cross-section area that lies within one skin depth of the surface, for the reference radius set above.

Introduction

When AC (alternating current) flows through a wire, it does not spread out evenly. Most of the current moves near the outside surface of the wire. This is called the skin effect. The skin depth is how deep the current goes before it drops to about 37% of its strength at the surface.

This skin depth calculator finds that depth. Enter the frequency, pick a material like copper, aluminum, brass, or steel, and press Calculate. You can also type your own resistivity and relative permeability values if your material is not on the list.

The calculator shows the skin depth, the conductivity, and the resistivity in the units you choose. It also gives you a step-by-step solution, a cross-section diagram of the wire, and a chart of skin depth versus frequency.

Skin depth matters because it changes how much of a wire really carries current. Higher frequency means a thinner skin, more resistance, and more heat. Engineers use this to pick wire sizes, design coils and transformers, plan PCB traces, and choose shielding and plating thickness.

How to use our Skin Depth Calculator

Enter the frequency, pick your metal, and set a conductor radius. The calculator shows the skin depth, the conductivity, the resistivity, and a picture of how deep the current flows in the wire.

Frequency (f): Type the AC frequency of your signal, then pick the unit: Hz, kHz, MHz, or GHz. Higher frequency means a smaller skin depth.

Material Preset: Pick the metal you are using, like copper, aluminum, brass, or steel. The preset fills in the resistivity and permeability for you. Pick "Custom" if you want to type your own numbers.

Resistivity (ρ): This is how much the material fights current flow. It fills in on its own from the preset. With "Custom" picked, type your value and choose the unit, such as μΩ·m or Ω·cm.

Relative Permeability (μᵣ): This tells how magnetic the material is. Use 1 for copper, aluminum, gold, and silver. Use a bigger number, like 100, for steel or nickel. It also fills in on its own unless you pick "Custom".

Output Format: Choose how the numbers look. Pick Scientific, Engineering, or Fixed. This changes every result on the page.

Display Units: Under each result you can change the unit. Show conductivity in S/m or S/cm, resistivity in Ω·m or μΩ·cm, and skin depth in mm, μm, mils, and more.

Reference Conductor Radius: Type the radius of your wire and pick mm, cm, or in. You can also drag the slider. This draws the cross-section diagram and gives you the skin depth count across the wire and the shell area percent.

Click Calculate to see your results and the step-by-step math. Click Reset to Defaults to start over with copper at 100 kHz.

What Is Skin Depth?

When alternating current (AC) flows through a wire, it does not spread out evenly. Instead, it crowds near the outside surface of the wire. This is called the skin effect. Skin depth (the Greek letter δ, "delta") is the distance from the surface where the current drops to about 37% of its surface value. Most of the current flows inside this thin outer layer.

The Skin Depth Formula

Skin depth is found with this equation:

δ = √( ρ / (π · f · μ₀ · μᵣ) )

  • δ is skin depth, in meters
  • ρ is resistivity of the metal, in ohm-meters (Ω·m)
  • f is frequency of the current, in hertz (Hz)
  • μ₀ is permeability of free space, 4π × 10⁻⁷ H/m
  • μᵣ is relative permeability of the metal (1 for copper, aluminum, gold, and silver)

Conductivity (σ) is just the flip side of resistivity: σ = 1 / ρ.

What Changes Skin Depth

  • Higher frequency = smaller skin depth. If you raise the frequency 100 times, the skin depth drops 10 times.
  • Higher resistivity = larger skin depth. Current soaks deeper into poor conductors like steel or graphite.
  • Magnetic metals have tiny skin depths. Steel and nickel have a high μᵣ, so current stays in a very thin shell.

Why Skin Depth Matters

Because the middle of a thick wire carries almost no current at high frequency, the wire acts smaller than it looks. That means more resistance, more heat, and more power lost. Engineers use skin depth to:

  • Pick wire sizes for AC power lines and transformers
  • Choose Litz wire or hollow tubes instead of solid wire at radio frequencies
  • Set copper thickness on printed circuit boards
  • Plan silver or gold plating thickness on RF connectors and waveguides
  • Design induction heating, shielding, and eddy current testing

Copper Skin Depth Examples

FrequencySkin depth in copper
60 Hzabout 8.5 mm
1 kHzabout 2.1 mm
100 kHzabout 0.21 mm (209 μm)
1 MHzabout 66 μm
1 GHzabout 2.1 μm

Quick Rule of Thumb

Compare the skin depth to the radius of your conductor. If the skin depth is bigger than the radius, current fills the whole wire and skin effect barely matters. If the skin depth is much smaller than the radius, the inside metal is mostly wasted, and a thinner or stranded conductor may work just as well, though its DC resistance will be higher.


Formulas used

Skin depth
\delta = \sqrt{\frac{\rho}{\pi f \mu_0 \mu_r}}
Absolute magnetic permeability
\mu = \mu_0 \mu_r, \qquad \mu_0 = 4\pi \times 10^{-7}\ \text{H/m}
Conductivity from resistivity
\sigma = \frac{1}{\rho}
Skin depths across conductor diameter
N = \frac{2R}{\delta}
Effective conducting shell area fraction
A_{\%} = \left(1 - \frac{(R-\delta)^2}{R^2}\right) \times 100\%
Skin depth to radius ratio
\frac{\delta}{R}

Frequently asked questions

Why does AC current flow near the surface of a wire?

Changing current makes a changing magnetic field inside the wire. That field pushes back and creates small swirling currents (eddy currents) in the metal.

These eddy currents cancel out the flow in the center and add to the flow near the outside. So the current gets pushed toward the skin of the wire. The faster the current changes, the stronger this push.

Why is skin depth measured at 37 percent?

The current drops off in a smooth curve as you go deeper. At one skin depth it has fallen to 1 divided by e, which is about 0.368, or 37 percent.

It is just a marker, like a half-life. Current still flows deeper than one skin depth, it is just much weaker.

How deep does the current really go?

Use these rough numbers for a flat surface:

  • 1 skin depth: about 63% of the current
  • 2 skin depths: about 86%
  • 3 skin depths: about 95%
  • 4 skin depths: about 98%

This is why engineers often make plating or shielding about 3 to 5 skin depths thick. Going thicker adds almost nothing.

Does skin effect happen with DC?

No. Steady DC spreads out evenly across the whole wire, so the full cross-section carries current.

Skin effect only shows up when current changes. It appears during switching, in pulses, and in any AC or ripple riding on top of DC.

Is there a quick way to estimate skin depth in copper?

Yes. For copper at room temperature:

δ (mm) ≈ 66 / √f, with f in hertz.

Example: at 10,000 Hz, √10,000 = 100, so δ ≈ 0.66 mm. The pattern is easy to remember: raise frequency 100 times and skin depth drops 10 times.

How much does skin effect raise AC resistance?

When the wire radius is much bigger than the skin depth, the AC resistance is about:

RAC / RDC ≈ R / (2δ)

Example: 12 AWG copper has a radius near 1 mm. At 1 MHz the skin depth is about 0.066 mm, so the AC resistance is roughly 7 to 8 times the DC value. That extra resistance turns into heat.

Does skin effect matter in 60 Hz house wiring?

Not for normal branch circuits. Copper skin depth at 60 Hz is about 8.5 mm, and a 12 AWG wire has a radius near 1 mm. Current fills the whole wire.

It starts to matter for very large conductors, like 500 kcmil cable and bus bars, where the radius gets close to or bigger than 8.5 mm. That is one reason big feeders are often split into several smaller cables.

Why is skin depth so small in steel?

Steel is magnetic. Its relative permeability can be 100 or more, and that number sits under the square root sign in the formula.

At 60 Hz, copper has a skin depth near 8.5 mm but carbon steel is only about 3 mm. At 1 kHz steel drops to under 1 mm. That is why induction heating works so well on steel, and why steel makes a poor conductor for AC.

What is Litz wire and when do you need it?

Litz wire is made of many thin strands, each one coated with its own insulation and woven so every strand takes a turn on the outside.

Use it when the wire radius is bigger than the skin depth, usually from about 10 kHz up to 1 MHz. It is common in switching transformers, inductors, and wireless charging coils. Above a few MHz, Litz gets costly and plated tubing or wide flat copper is often better.

What is proximity effect and how is it different from skin effect?

Skin effect comes from a wire's own magnetic field. Proximity effect comes from the magnetic field of nearby wires pushing current to one side of a conductor.

In tight coils and transformer windings, proximity effect can add more loss than skin effect does. Spacing turns apart, using fewer layers, and using Litz wire all help.

How thick should silver or gold plating be on an RF connector?

Aim for about 3 to 5 skin depths at your lowest working frequency. At 1 GHz, silver has a skin depth near 2 μm, so about 6 to 10 μm of plating is plenty.

The current rides in the plating, not the base metal, so plating quality and smoothness matter more than the metal underneath.

How thick does a metal shield need to be to block a field?

Each skin depth of thickness cuts the field by about 8.7 dB. So a shield 3 skin depths thick gives roughly 26 dB of loss from absorption alone, plus more from reflection at the surface.

At low frequencies the skin depth is large, so thin foil does little. That is when steel or mu-metal, with their high permeability and tiny skin depth, work better.

Does a hollow tube carry as much AC current as a solid rod?

At high frequency, almost. If the wall is a few skin depths thick, the tube carries nearly the same current as a solid bar of the same outside size.

The middle of a solid bar is mostly dead weight. This is why RF coils, large bus work, and waveguides often use copper tubing instead of solid metal.

Does temperature change skin depth?

Yes. Hot metal has higher resistivity, and higher resistivity means deeper skin depth.

Copper resistivity rises about 0.39 percent per °C. Since skin depth follows the square root, it grows about 0.2 percent per °C. Going from 20 °C to 100 °C increases copper skin depth by roughly 15 percent.

What is the skin depth of aluminum compared with copper?

Aluminum has higher resistivity, so its skin depth is about 28 percent larger than copper's at the same frequency.

  • 60 Hz: copper 8.5 mm, aluminum 10.9 mm
  • 100 kHz: copper 0.21 mm, aluminum 0.27 mm
  • 1 MHz: copper 66 μm, aluminum 85 μm

Deeper is not better here. Aluminum still has more resistance overall; the current just spreads a bit further in.

How does skin depth affect PCB trace thickness?

One ounce copper is about 35 μm thick. Copper skin depth is 66 μm at 1 MHz, so the whole trace carries current there.

At 100 MHz the skin depth drops to about 6.6 μm, and at 1 GHz to about 2 μm. Above roughly 20 MHz, adding more copper weight barely lowers resistance. Making traces wider, or smoothing the copper surface, helps more.