“…which means, that the imaginary part of the inductance resembles a core loss resistor R c = ωL ′′ depending on the frequency and the imaginary part of the relative permeability. Z 1 refers to (18) computed with ( 13) and ( 15), Z 2 is computed with the compact models (3) and ( 7), in addition the partial resistances R f (38) and R 1D (37), and Rc (19), which is the core resistor. b) R /R DC of IND 2: Z 1 is computed with ( 13) and ( 17), the compact models (3) and ( 11) are used to compute Z 2 , and the partial resistances are calculated using (41), (40), and (19).…”