Skin effect is a phenomenon that occurs in conductors carrying alternating current (AC) at high frequencies. It describes the tendency of AC currents to distribute themselves unevenly across the cross-sectional area of a conductor, with the current density being highest near the surface and gradually decreasing as you move toward the center of the conductor. In other words, at high frequencies, the current tends to "skin" the surface of the conductor.
This effect is a result of electromagnetic induction. As AC current flows through a conductor, it generates a magnetic field around the conductor. This magnetic field, in turn, induces an opposing electric field within the conductor itself, which counteracts the flow of current toward the center. Consequently, most of the current flows near the surface where the opposing electric field is weaker, leading to higher current density on the surface and lower current density toward the core of the conductor.
The impact of skin effect on conductor resistance at high frequencies is an increase in effective resistance. Since resistance is inversely proportional to the cross-sectional area available for current flow, the reduction in usable cross-sectional area due to the concentration of current near the surface leads to an apparent increase in resistance. This, in turn, results in increased power losses in the form of heat, reducing the overall efficiency of the system.
To mitigate the effects of skin effect, conductors used in high-frequency applications are often designed with larger diameters or multiple smaller strands bundled together. This increases the overall surface area available for current flow, effectively reducing the resistance and minimizing power losses. In some cases, hollow conductors or conductors with special geometries can also be employed to manage skin effect and maintain efficient current distribution across the conductor's cross-section.