Use the following simulation settings:
- Stop time: 14 s
- Number of intervals: 5000
- Tolerance: 1e-5
This example compares the behavior of three different hysteresis
models due to the exact same input magnetic field strength. The
three different models are:
- Model=GenericHystTellinenSoft, Tellinen hysteresis model, the
upper and lower branch of the limiting hysteresis loop is roughly
approximated with simple hyperbolic tangent functions (Fig1.
c)
- Model=GenericHystTellinenTable, Tellinen hysteresis model, the
upper and lower branch of the limiting hysteresis loop can be
defined with almost arbitrary table data (Fig1. d)
- Model=GenericHystPreisachEverett,Preisach hysteresis model, the
hysteresis shape is defined by the Everett function (Fig1. e)
Compared to the complex Preisach hysteresis model the Tellinen
model is very simple and thus computationally more effective and
stable. It is sufficient for many applications. But the Tellinen
model has inherently a problem with small periodic input field
variations at locations where the outer hysteresis loop has large
slopes. In such a case, the simulated minor loops settle to the
center of the hysteresis envelope curve, whereas the minor loops of
the Preisach model stay constant ('property of equal vertical
chords', [Ma03]).
The input signal of the example (Fig. 1 a) corresponds to that case
and Fig. 1 b-e shows the behavior of the different models.
Fig. 1: Simulated magnetic
flux densities B of different hysteresis models (b) due to an
applied magnetic field strength shown in (a). Corresponding B(H)
loops of the hysteresis models GenericHystTellinenSoft (c),
GenericHystTellinenTable (d) and GenericHystPreisachEverett
(e).
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