Applying DC voltage across an inductor primarily results in a voltage drop across the series internal resistance of the coil, as the reactance term becomes negligible at DC. The impedance of an inductor combines both resistance and reactance, expressed as Z = R + jωL, but at DC, the reactance (jωL) is zero. Consequently, the current through the inductor can be described by the equation i = V/R, assuming R is the only factor affecting the current. If R is zero, as in superconducting conditions, the current would theoretically be infinite, represented as i = Vt/L. In contrast, applying AC voltage introduces frequency-dependent reactance, increasing the perceived resistance as frequency rises.