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The current density, that is, the amount of current being conducted by a material per unit of cross sectional area (usually circular mil), will vary as the voltage that is applied, and, if it is AC, on the frequency of the applied voltage. More voltage will drive more current. For DC, the total current being conducted in a material (which is part of a circuit) will be divided by the cross sectional area to get the number of amperes per unit of cross sectional area. It's a direct relationship with the conductivity of the material under inspection not an issue because the totalcircuit resistance and the applied voltage will determine current. With the current through the material of interest known, its geometry can be used with the magnitude of the current to determine current density. In an AC circuit, the same as above, exceptthat the frequency, as it increases, will drive current toward the outside of the conducting medium - the so-called skin effect. Other calculation methods will have to be employed to determine current density which incude the effects of the frequency of the AC. At low frequencies, the effect will be almost negligible. Given these things about current and current density, it is not possible to calculate current density in 316L stainless (the low carbon version of 316 stainless) or of anything else we wish to consider without more information.

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