Hysteresis

When aferromagnetic material is magnetized in one direction, it will not relax back to zero magnetization when the imposed magnetizing field is removed. It must be driven back to zero by a field in the opposite direction. If an alternating magnetic field is applied to the material, its magnetization will trace out a loop called ahysteresis loop. The lack of retraceability of the magnetization curve is the property called hysteresis and it is related to the existence of magnetic domains in the material. Once the magnetic domains are reoriented, it takes some energy to turn them back again. This property of ferrromagnetic materials is useful as a magnetic "memory". Some compositions of ferromagnetic materials will retain an imposed magnetization indefinitely and are useful as "permanent magnets". The magnetic memory aspects of iron and chromium oxides make them useful in audiotape recording and for the magnetic storage of data on computer disks.

Hysteresis Loop

It is customary to plot themagnetization M of the sample as a function of themagnetic field strength H, since H is a measure of the externally applied field which drives the magnetization .

Hysteresis in Magnetic Recording

Because ofhysteresis, an input signalat the level indicated by the dashed line could give a magnetization anywhere between C and D, depending upon the immediate previous history of the tape (i.e., the signal which preceded it). This clearly unacceptable situation is remedied by thebias signal which cycles the oxide grains around their hysteresis loops so quickly that the magnetization averages to zero when no signal is applied. The result of the bias signal is like a magnetic eddy which settles down to zero if there is no signal superimposed upon it. If there is a signal, it offsets the bias signal so that it leaves a remnantmagnetization proportional to thesignal offset.

Variations in Hysteresis Curves

There is considerable variation in thehysteresis of different magnetic materials.

The curve on the left above represents materials which are sometimes called magnetically "hard". This includes various steel alloys and special alloys such as Alnico. If magnetized near saturation, such materials may retain amagnetic field as high as B = 1 Tesla, corresponding to an internalmagnetization M = B/μ₀ of about 800,000 A/m.

The curve on the right represents magnetically "soft" materials such as soft iron which are used fortransformer andmotor cores. They minimize the energy loss and heating associated with periodically reversing the magnetic field in AC electrical applications.