This effectively limits the cross-sectional conductor area available to carry alternating electron flow, increasing the resistance of that conductor above what it would normally be for direct current:
Skin effect: skin depth decreases with increasing frequency.
The electrical resistance of the conductor with all its cross-sectional area in use is known as the “DC resistance.” The “AC resistance” of the same conductor refers to a higher figure resulting from the skin effect.
As you can see, at high frequencies the AC current avoids traveling through most of the conductor’s cross-sectional area. For the purpose of conducting current, the wire might as well be hollow!
In some radio applications (antennas, most notably) this effect is exploited. Since radio-frequency (“RF”) AC currents wouldn’t travel through the middle of a conductor anyway, why not just use hollow metal rods instead of solid metal wires and save both weight and cost? (See figure below.)
Most antenna structures and RF power conductors are made of hollow metal tubes for this reason.
In the following photograph, you can see some large inductors used in a 50 kW radio transmitting circuit. The inductors are hollow copper tubes coated with silver, for excellent conductivity at the “skin” of the tube:
High power inductors formed from hollow tubes.
The degree to which frequency affects the effective resistance of a solid wire conductor is impacted by the gauge of that wire. As a rule, large-gauge wires exhibit a more pronounced skin effect (change in resistance from DC) than small-gauge wires at any given frequency.
The equation for approximating skin effect at high frequencies (greater than 1 MHz) is as follows:
The table below gives approximate values of “k” factor for various round wire sizes. “k” factor for various AWG wire sizes.
|gauge size||k factor||gauge size||k factor|
For example, a length of number 10-gauge wire with a DC end-to-end resistance of 25 Ω would have an AC (effective) resistance of 2.182 kΩ at a frequency of 10 MHz:
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