Since version 2026, Flux 3D and Flux PEEC are no longer available.
Please use SimLab to create a new 3D project or to import an existing Flux 3D project.
Please use SimLab to create a new PEEC project (not possible to import an existing Flux PEEC project).
/!\ Documentation updates are in progress – some mentions of 3D may still appear.
About orientation of magnets
Definition
Before discussing the magnet orientation, the concept of magnet in Flux must be defined specifying the point of view it is related to.
- for magnet manufacturers:
- a material for an isotropic magnet is a material with identical magnetic characteristics in all directions; the magnetization process of the magnet will lead to the same result in any direction
- a material for an anisotropic magnet has a preferred direction of magnetization; it will be magnetized in this direction
- in the Flux software:
a material of the magnet type is a magnetized magnet ; it has a preferred direction - its direction of magnetization
Consequence
A magnet must be oriented in the region it is affected in.
Various models
The various types (models) provided for the magnets are presented in chapter Materials: principles (§B(H) law: models for hard materials).
The distinction between the unidirectional model and the vector model is explained in the two tables below:
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In a model of the “unidirectional” type the mathematical model and the direction of magnetization are dissociated |
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| Definition | Use | |
| Module of Br |
Direction (in a plane XOY)
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A single material can be used for definition of several regions (with different directions of magnetization) |
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In a model of the “vector” type (linear approximation only) the mathematical model and the direction of magnetization are associated |
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| Definition | Use |
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It is necessary to create the same number of materials and/or coordinate systems as the regions |
Orientation of unidirectional magnets: principle
For a unidirectional magnet, there is no information (at the level of the definition of the material) on the direction of magnetization.
To “orient a unidirectional magnet in a region”, one must:
- choose the type of orientation
- define the characteristics of this type
The principle of orientation for a unidirectional magnet in a region is presented in the figure below. (The basic plane is a XOY plane)
| Type of orientation | Scheme | Description characteristics | |
|---|---|---|---|
| Unidirectional |
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Radial positive / negative |
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Orthoradial positive / negative |
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Orientation of vector magnets: principle
For a vector magnet, the direction of magnetization is defined in a virtual coordinate system.
To “orient a (cartesian, cylindrical, spherical) vector magnet in a region”, one must choose a coordinate system for orientation (real coordinate system).
The principle of orientation for a vector magnet (cartesian) in a region is presented in the figure below:
!!! Magnets and thin or filiform region
Everything that was previously stated concerns the massive regions (volume regions in 3D / face regions in 2D).
Generally speaking, the models for magnets cannot be used in thin or filiform regions (3D exception: see next block).
3D exception
In 3D, it is possible to use the magnet models in thin regions (face regions).
| During … | the user chooses … |
|---|---|
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the creation of thin region |
the direction of magnetic flux:
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the orientation of magnet |
the direction of magnetization: see previous block |
In order to avoid any problem of coherence on the direction of the magnetic flux, it is advised to use the option “no restriction on the direction of the magnetic flux”.