Weiss domains are small magnetic domains within a ferromagnetic material in which the magnetic moments of the atoms are aligned in parallel. These domains were named after the French physicist Pierre-Ernest Weiss, who first described them theoretically. The magnetic moments in a Weiss district are homogeneously aligned, while the alignment of the domains to each other varies in order to minimise the total energy of the material.
Ferromagnetic materials consist of many Weiss districts. Within a single district, the magnetic moments of the atoms are fully aligned, resulting in a high local magnetisation. Between neighbouring districts, however, the magnetic moments often show different directions, which means that the material as a whole initially shows no external magnetisation. This behaviour minimises the overall energy of the material.
When a ferromagnetic material is placed in an external magnetic field, the structure of the Weiss domains changes:
The transition regions between two Weiss districts are called Bloch walls. In these areas, the magnetic moments gradually change from the orientation of one neighbourhood to the orientation of the other. Bloch walls play an important role in the movement and restructuring of Weiss domains during magnetisation.
Understanding Weiss domains is crucial for the development and optimisation of magnetic materials and technologies:
Did you know that the movement of Weiss domains during magnetisation is not uniform? Instead, it occurs in small steps, a phenomenon known as the Barkhausen effect. This effect provides valuable information about the microstructure of ferromagnetic materials and is used in material diagnostics.