SNOA930C March 2015 – May 2021 LDC0851 , LDC1001 , LDC1001-Q1 , LDC1041 , LDC1051 , LDC1101 , LDC1312 , LDC1312-Q1 , LDC1314 , LDC1314-Q1 , LDC1612 , LDC1612-Q1 , LDC1614 , LDC1614-Q1 , LDC2112 , LDC2114 , LDC3114 , LDC3114-Q1
A DC current can take advantage of the entire cross section of a conductor. However, at higher frequencies electrical current prefers to simply travel along the surface of the conductor. This tendency is called Skin Effect, and is primarily a function of the conductivity and the frequency. With a copper conductor, more than 95% of a 1 MHz current flows in at the surface in a shell only 0.2 mm thick. At 10 MHz, the 95% of the current flows in a shell only 0.06 mm from the surface of the conductor.
The skin effect is the primary source of the increase in the AC RS at higher frequencies. This effect also affects the eddy currents on the target surface - the generated eddy currents flow on the surface of the conductive target closest to the inductor.