I. Introduction
Magnetic components are an integral part of almost every power electronic circuit [1, p. 25]. They fulfill various tasks such as storing energy temporarily (e.g., a choke in a switch mode power supply (SMPS) or a flyback transformer), transforming voltages (e.g., 50/60 Hz transformers or high frequency transformer in SMPSs) or operating as a filter choke due to electromagnetic compatibility (EMC) reasons. A material of high permeability (e.g., ferrite or electrical steel) is required as a core to increase the inductance or to improve the coupling between two or more windings. An external magnetic field strength magnetizes this material, which results in an increased flux density. However, the magnetization has limits, since it is a rotation of dipoles in the material [2, p. 5]. If all dipoles are aligned almost in the same direction, the material saturates. The first theories in physics were developed in the early 20th century to describe this process in magnetic material [3]. Today numerous models including the well-known of Jiles and Atherton [4], Hodgdon [5], or Preisach [6] exist to describe the nonlinear, hysteresis afflicted behavior.