Skin effect
The
skin effect is the tendency of a high-
frequency electric
current to distribute itself in a
conductor so that the current density near the surface of the conductor is greater than that at its core. It causes the effective
resistance of the conductor to increase with the
frequency of the current. The effect was first explained by
Lord Kelvin in
1887.
Nikola Tesla also investigated the
Skin effect.
Mathematically speaking, the current density J in the conductor decreases exponentially with depth δ, as follows:
where
d is a constant called the
skin depth. This is defined as the depth below the surface of the conductor at which the current is 1/
e (about 0.37) times the current at the surface. It can be calculated as follows:
where
- ρ = resistivity of conductor
- ω = angular frequency of current = 2π × frequency
- μ = absolute magnetic permeability of conductor
The resistance of a flat slab (much thicker than
d) to alternating current is exactly equal to the resistance of a plate of thickness
d to direct current. For long, thin conductors such as wires, the resistance is
approximately that of a hollow tube with wall thickness
d carrying direct current. For example, for a round wire, the resistance is approximately:
where
- L = length of conductor
- D = diameter of conductor
The final approximation above is accurate if
D >>
d.
Mitigation
A type of cable called litz wire (from the German Litzendraht, woven wire) is used to mitigate the skin effect. It consists of a number of insulated wire strands woven together in a carefully designed pattern, so that the overall magnetic field acts equally on all the wires and causes the total current to be distributed equally among them. Litz wire is often used in the windings of high-frequency
transformers, to increase their efficiency.
In other applications, solid conductors are replaced by tubes, which have the same resistance at high frequencies but of course are lighter.
Examples
In a copper wire, the skin depth at various frequencies is shown below.
| frequency | δ |
| 60 Hz | 8.57 mm |
| 10 kHz | 0.66 mm |
| 10 MHz | 21 μm |