Asymmetry of E-I loops for nickel-iron cores under alternating magnetizing forces is shown to be due to residual polarization, the distribution of which throughout the crosssection of the stamping is different from the distribution of the flux due to the applied alternating magnetizing force. It is also shown that such polarization may, under certain conditions, bein different directions simultaneously in the inner and outer parts of thestamping. The polarization can be removed by applying a relatively large alternating magnetizing force and reducing it slowly to zero. Curves are produced showing the amount of polarizing flux removed by different values of alternating magnetizing force, tarting with a known value of residual flux. It is shown that in the case of mumetal the curves are different when the residual flux is caused by switching off alternating and direct current respectively. Other curves show the marked increase in polarizing flux produced bydirect current when an alternating magnetizing force of suitable valueis superimposed. The reduction of apparent permeability due to residual polarization is also shown. Strong polarization is found to occur, both in nickel-iron and in silicon-steel cores, under conditions in which capacitanceloading of the secondary winding produces resonance with even harmouics, provideda small initial polarization is present. Initial polarization sufficient toallow this phenomenon to occur is found to be usually present, evenwhen thenormal loop is almost symmetrical. The presence of even harmonics in the magnetizing current, as may occur, for instance, when the source of supply iathermionic valve, is also found to cause polarization. With certain values of capacitance loading of polarized specimens, sub-harmonics are produced. The asymmetry of E-I loops or specimens with residual polarization is found to be less apparent as the frequency is raised above 50 cycles per sec. It is pointed out that these phenomena should be taken into account in the design and operation of electromagnetic apparatus, but that cores of the more usual commercial forms will not exhibit the phenomena to the same extent as the plain ring stampings used in most of the tests described.
Read full abstract