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02 Barkhausen Effect (2)

Updated: 09 Jul 2026

Aim

To show the ferromagnetic behaviour of a cubic lattice.

Subjects

Diagram

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Figure 1:.

Equipment

Presentation

The model is placed on the overhead projector and projected. The individual compass-needles are aligned in groups, but in total there is no net direction. Slowly the bar magnet approaches the model. Every now and then a group of needles suddenly change their orientation and align themselves with the external magnetic field. When the bar magnet is close near the model, all needles are aligned in the same direction.

Slowly the bar magnet is moved away. Some of the needles change their direction with a step of 90 , but most of the needles keep their orientation. Only when you approach the model with the other pole of the bar magnet, then they redirect themselves.

Observing the number of needles aligned with the external field gives a good impression of the hysteresis loop. (Counting the number of individual compass needles enables you to draw a hysteresis loop.)

Explanation

The model behaves like ferromagnetic material. It has a cubic (better: flat square) structure with magnetic domains.

When the material (model) is magnetized to saturation and the external magnetic field is reduced to zero, a substantial magnetization remains. This behavior is characteristic of permanent magnets. Reducing the magnetization to zero requires the application of a magnetic field in the opposite direction.

Remarks

Sources