26.5.3 Magnetic permeability

Products: Abaqus/Standard  Abaqus/CAE  

References

Overview

A material's magnetic permeability:

Linear magnetic behavior

Linear magnetic behavior is defined by direct specification of magnetic permeability.

Directional dependence of magnetic permeability

Isotropic, orthotropic, or fully anisotropic magnetic permeability can be defined. For non-isotropic magnetic permeability a local orientation for the material directions must be specified (Orientations, Section 2.2.5).

Isotropic magnetic permeability

For isotropic magnetic permeability only one value of magnetic permeability is needed at each temperature and field variable value. Isotropic magnetic permeability is the default.

Input File Usage:          
*MAGNETIC PERMEABILITY, TYPE=ISOTROPIC

Abaqus/CAE Usage:   

Property module: material editor: Electrical/MagneticMagnetic Permeability: Type: Isotropic


Orthotropic magnetic permeability

For orthotropic magnetic permeability three values of magnetic permeability (, , ) are needed at each temperature and field variable value.

Input File Usage:          
*MAGNETIC PERMEABILITY, TYPE=ORTHOTROPIC

Abaqus/CAE Usage:   

Property module: material editor: Electrical/MagneticMagnetic Permeability: Type: Orthotropic


Anisotropic magnetic permeability

For fully anisotropic magnetic permeability six values (, , , , , ) are needed at each temperature and field variable value.

Input File Usage:          
*MAGNETIC PERMEABILITY, TYPE=ANISOTROPIC

Abaqus/CAE Usage:   

Property module: material editor: Electrical/MagneticMagnetic Permeability: Type: Anisotropic


Frequency-dependent magnetic permeability

Magnetic permeability can be defined as a function of frequency in a time-harmonic eddy current analysis.

Input File Usage:          
*MAGNETIC PERMEABILITY, FREQUENCY

Abaqus/CAE Usage:   

Property module: material editor: Electrical/MagneticMagnetic Permeability: Toggle on Use frequency-dependent data


Nonlinear magnetic behavior

Nonlinear magnetic behavior is characterized by magnetic permeability that depends on the strength of the magnetic field. The nonlinear magnetic material model in Abaqus is suitable for ideally soft magnetic materials (without any hysteresis effects) characterized by a monotonically increasing response in B–H space, where B and H refer to the strengths of the magnetic flux density vector and the magnetic field vector, respectively. Nonlinear magnetic behavior is defined through direct specification of one or more B–H curves that provide B as a function of H and, optionally, temperature and/or predefined field variables, in one or more directions. Nonlinear magnetic behavior can be isotropic, orthotropic, or transversely isotropic (which is a special case of the more general orthotropic behavior). More than one B–H curve is needed to define the nonlinear magnetic behavior if it is not isotropic.

Directional dependence of nonlinear magnetic behavior

Isotropic, orthotropic, or transversely isotropic nonlinear magnetic behavior can be defined. For non-isotropic nonlinear magnetic behavior a local orientation for the material directions must be specified (Orientations, Section 2.2.5).

Isotropic nonlinear magnetic behavior

For isotropic nonlinear magnetic response only one B–H curve is needed at each temperature and field variable value. Isotropic magnetic permeability is the default. Abaqus assumes that the nonlinear magnetic behavior is governed by

Input File Usage:          You define through a B–H curve:
*MAGNETIC PERMEABILITY, NONLINEAR, TYPE=ISOTROPIC
*NONLINEAR BH, DIR=direction

The B–H curve in any direction (i.e., the nonlinear behavior in global direction 1, 2, or 3) will suffice as the nonlinear magnetic behavior is assumed to be the same in all directions.


Abaqus/CAE Usage:   Nonlinear magnetic behavior is not supported in Abaqus/CAE.

Orthotropic nonlinear magnetic behavior

For orthotropic nonlinear magnetic response three B–H curves (one curve to define the behavior in each of the local directions 1, 2, and 3) are needed at each temperature and field variable value. Abaqus assumes that the nonlinear magnetic behavior in the local material directions is governed by

where refers to a diagonal matrix.

Transversely isotropic nonlinear magnetic behavior is a special case of orthotropic behavior, in which the behavior in any two directions is the same and is different from that in the third direction.

Input File Usage:          You define , , and , respectively, through three independent B–H curves, one in each of the directions 1, 2, and 3:
*MAGNETIC PERMEABILITY, NONLINEAR, TYPE=ORTHOTROPIC
*NONLINEAR BH, DIR=1
…
*NONLINEAR BH, DIR=2
…
*NONLINEAR BH, DIR=3
…

Abaqus/CAE Usage:   Nonlinear magnetic behavior is not supported in Abaqus/CAE.

Elements

Magnetic material behavior is active only in electromagnetic elements (see Choosing the appropriate element for an analysis type, Section 27.1.3).