magnetization increases in the same proportion. When the magnetizing force attains the value D, the magnetization is two-thirds of its limiting value. When the magnetizing force is further increased, the magnetization, instead of increasing indefinitely, tends towards a finite limit.
The law of magnetization is expressed in Fig. 7, where the magnetizing force is reckoned from towards the right and the magnetization is expressed by the vertical ordinates. Weber's own experiments give results in satisfactory accordance with this law. It is probable, however, that the value of D is not the same for all the molecules of the same piece of iron, so that the transition from the straight line from O to E to the curve beyond E may not be so abrupt as is here represented.
444.] The theory in this form gives no account of the residual magnetization which is found to exist after the magnetizing force is removed. I have therefore thought it desirable to examine the results of making a further assumption relating to the conditions under which the position of equilibrium of a molecule may be permanently altered.
Let us suppose that the axis of a magnetic molecule, if deflected through any angle β less than β0, will return to its original position when the deflecting force is removed, but that if the deflexion β exceeds β0, then, when the deflecting force is removed, the axis will not return to its original position, but will be permanently deflected through an angle β - β0, which may be called the permanent set of the molecule.
This assumption with respect to the law of molecular deflexion is not to be regarded as founded on any exact knowledge of the intimate structure of bodies, but is adopted, in our ignorance of the true state of the case, as an assistance to the imagination in following out the speculation suggested by Weber.
Let
| (9) |
