Young's modulus of elasticity and its change with magnetization, that is, the ΔE-effect in the annealed state of ferromagnetic nickel-copper alloys, have been measured in detail at ordinary temperatures by the method of magnetostrictive oscillation, which was described in a preceding paper. The measured range of magnetic field for the ΔE-effect is up to about 900 oerstcds. The general course of the change of Young's modulus accompanied by an increase of magnetic field or intentisity of magnetization, is similar for alloys of any compositions here investigated. The modulus increases quickly at weak fields, but the rate of increase diminishes gradually with growing field, finally the change of the modulus attaining a saturation. As for the relation between the change of the modulus and the intensity of magnetization, the modulus increases more and more rapidly from the low to the high magnetization range, but once the rate of its increase diminishes slightly, and afterwards the modulus shows a rapid increase in the magnetization range adjacent to its saturation. The detailed observation of the ΔE-effect reveals, however, the following two particulars. In the first place, Young's modulus in alloys of an intermediate composition range (5_??_21 weight percent copper) decreases, that is, ΔE/E (the change of the modulus, relative to that in the non-magnetized state) becomes negative, though slightly, at first at very weak fields or in the very low magnetization range, and makes a minimum before it increases rapidly with further increasing field or magnetization. Secondly, in nickel and alloys of high nickel compositions (below 15.5 percent copper), the modulus increases somewhat rapidly again in the field range just preceding the saturation. The saturation value of the relative change of Young's modulus, (ΔE/E)∞, decreases with increasing copper content, but the course of decrease is by no means monotonous, making an inflexion in the composition range of 10_??_15 percent copper. An extrapolation of the (ΔE/E)∞, vs. composition curve shows that the ΔE-effect vani-shes at the composition of about 34 percent copper, and this composition coincides with that at which the ferro-magnetism disapears at ordinary temperatures. The curve calculated on the basis of theories agrees qualitatively well with the measured one. It is also shown that a quantitative difference recognized between (ΔE/E)∞ vs. composition curves of the two sets of alloys of different origins can be explained in terms of the difference in their initial susceptibilities. The rate of a rapid increase of Young's modulus at weak fields, the intensity of magnetic field at which its increase saturates, its temporary decrease in the very weak field or magnetization range, and the intensity of magnetic field at wihch its secondary somewhat rapid increase occures, all decrease with an increase of copper content. The relation between Young's modulus at the non-magnetized state and the composition shows a considerably complicated aspect. The modulus increase at first with an addition of copper to nickel, makes a maximum at about 10, a minimum at about 15, and again a maximum at about 20 percent copper, and then it decreases with further increasing copper. The existence of the minimum at about 10 percent copper has never been found.
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