The elements provided in the package Shapes.HysteresisAndMagnets
allow for consideration of ferromagnetic and dynamic hysteresis
during the simulation of electromagnetic networks. The
ferromagnetic hysteresis is a material property of the core
material and frequency independent. Due to eddy currents the static
ferromagnetic hysteresis is superposed by a frequency dependent
hysteresis when the ferromagnetic material is exposed to an
alternating magnetic field. Fig 1 exemplary shows the simulated
hysteresis characteristics of a simple inductor with an iron core
for three different excitation frequencies. Thereby, the 0 Hz
hysteresis loop represents the static ferromagnetic hysteresis of
the core material. The widening of the loops for higher frequencies
is due to eddy currents induced in the core material.
Several models to describe the static hysteresis behavior of
ferromagnetic materials are known. In this library two of them are
implemented. The simple but fast
Tellinen hysteresis model and the more accurate but complex
Preisach hysteresis model. Click the links for a short
description of both models.
Name / Icon |
Description |
GenericHystTellinenSoft
|
Flux tube element for modeling soft magnetic materials with
ferromagnetic and dynamic hysteresis (eddy currents). The
ferromagnetic hysteresis behavior is defined by the
Tellinen hysteresis model. The shape of the limiting hysteresis
loop is described by simple hyperbolic tangent functions with 4
parameters. Therefore, the hysteresis shape variety is limited but
the parameterization of the model is very simple and the model is
relatively fast and robust. |
GenericHystTellinenHard
|
Flux tube element for modeling the ferromagnetic (static)
hysteresis of hard magnetic materials. The ferromagnetic hysteresis
behavior is defined by the
Tellinen hysteresis model. The shape of the limiting hysteresis
loop is described by simple hyperbolic tangent functions with 4
parameters. |
GenericHystTellinenEverett
|
Flux tube element for modeling soft magnetic materials with
ferromagnetic and dynamic hysteresis (eddy currents). The
ferromagnetic hysteresis behavior is defined by the
Tellinen hysteresis model. The Shape of the limiting
ferromagnetic hysteresis loop is specified by an analytical
description of the Everett function, which is also used to
parameterize the
GenericHystPreisachEverett model. A library of predefined
parameter sets can be found in
FluxTubes.Material.HysteresisEverettParameter. |
GenericHystTellinenTable
|
Flux tube element for modeling magnetic materials with
ferromagnetic and dynamic hysteresis (eddy currents). The
ferromagnetic hysteresis behavior is defined by the
Tellinen hysteresis model. The rising and falling branch of the
limiting ferromagnetic hysteresis loop are specified by table data.
Therefore, almost any hysteresis shapes are possible. A library
with predefined tables can be found at
FluxTubes.Material.HysteresisTableData. |
GenericHystPreisachEverett
|
Flux tube element for modeling magnetic materials with
ferromagnetic and dynamic hysteresis (eddy currents). The
ferromagnetic hysteresis behavior is defined by the
Preisach hysteresis model. The Shape of the limiting
ferromagnetic hysteresis loop is specified by an analytical
description of the Everett function. A library of predefined
parameter sets can be found in
FluxTubes.Material.HysteresisEverettParameter. |
GenericHystTellinenPermanentMagnet
|
Flux tube element for modeling the hard magnetic hysteresis of
permanent magnets. The model is similar to
GenericHystTellinenHard but has an initial magnetization preset
of -100% and an adapted icon for better readability of the
diagram. |
GenericLinearPermanentMagnet
|
Simple model of a linear permanent Magnet. Typical
characteristics of common permanent magnetic materials can be found
at FluxTubes.Material.HardMagnetic. |