1. Specimens of steel cooled from high temperatures are, as regards their magnetic properties, in a “sensitive state.”
2. After magnetisation, reversal of the field reduces the susceptibility.
3. Cyclic reversals of the field between definite limits bring the magnetic quality to a definite lower value for fields lying between these limits.
4. So long as the field is not changed in sign, the “sensitive state” persists.
5. Cyclic reversals of the field between narrow limits reduce the susceptibility for fields beyond these limits, but not to its lowest possible value.
6. The rate of cooling from the high temperature—if not very rapid—has little influence on the magnitude of the effect.
7. The “sensitive state” does not wear off with time.
8. Mechanical vibration of the specimens considerably reduces the phenomenon.
9. The “sensitive state” is most pronounced in hard steels.
10. The effect is induced to a slight degree in some varieties of steel by temperatures as low as 100° C. It increases with increasing temperatures to about 700° C. Further increase in temperature has little influence.
11. Similar effects are noticeable in cast iron and in cobalt. The “sensitive state” is absent, or is present to only a very slight extent, in soft iron.
12. The effect has a maximum value for fields which give large values of μ, and tends to zero as the saturation point is approached.