Abstract. The paper presents the results of calculations, simulations, and measurements of parasitic capacitance of winding in ferrite inductor suitable for cooperating with 2 kW DC-DC boost converter built using SiC JFET transistors, operating with a switching frequency of 100 kHz. The inductor winding is made of litz wire in a two-layer configuration. The lumped model of inductor winding was adopted. The results of analytical calculations have been compared with the results obtained from experimental investigations based on the resonance effect.Key words: model of inductor circuit, interlayer capacitance, parallel resonance, litz wire, inductor winding, skin effect.
Analytical and experimental determination of the parasitic parameters in high-frequency inductor
Model of high-frequency inductorThe most common method for determining typical parameters of an inductor in a converter design process is the equivalent circuit method, which takes into account the lumped parameters of this component (Fig. 1). Essentially, the parasitic capacitance is treated as the capacitor C p , connected in parallel to the inductor. This capacitance is connected in parallel to the resistance R p , which corresponds with the power losses in the core. Also, both C p and R p are connected in parallel to the third leg, consisting of a series connection of inductance L and resistance R s , representing the total resistance of the winding. A laboratory model of the inductor has been build using a UI93 core made from N87 type ferrite, which is characterized by the effective cross section area S Fe = 840 mm 2 and volume V Fe = 220 cm 3 , as provided in the core's datasheet. Knowing these parameters, in order to achieve the assumed inductance L = 1.2 mH at nominal current I max = 8 A, the winding with the number of turns N = 40 has been prepared. In order to reduce the eddy currents and winding losses in the assumed frequency of 100 kHz, a litz wire, made up of 120 wires of 0.1 mm di-