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Kato, A.
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Publications (9/9 displayed)
- 2023Effect of grain size on the core loss of nanocrystalline Fe86B13Cu1 prepared by ultra-rapid annealingcitations
- 2019Nanocrystalline soft magnetic materials from binary alloy precursors with high saturation magnetizationcitations
- 2018Towards understanding of magnetization reversal in Nd-Fe-B nanocomposites: analysis by high-throughput micromagnetic simulationscitations
- 2018Low temperature texture development in Nd 2 Fe 14 B/ α -Fe nanocomposite magnets via equal channel angular pressingcitations
- 2018Low temperature texture development in Nd2Fe14B/<i>α</i>-Fe nanocomposite magnets via equal channel angular pressingcitations
- 2017Copper-free nanocrystalline soft magnetic materials with high saturation magnetization comparable to that of Si steelcitations
- 2017On the limits of coercivity in permanent magnetscitations
- 2015CRP 1846C>T Genetic Polymorphism Is Associated with Lymph Node Metastasis and/or Severe Lymphatic Invasion in Endometrial Cancer.citations
- 2009An in situ neutron diffraction study of magnetic hardening in Fe3B/Nd2Fe14B nanocomposite magnets induced by rapid thermal annealingcitations
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article
Effect of grain size on the core loss of nanocrystalline Fe86B13Cu1 prepared by ultra-rapid annealing
Abstract
<jats:p>Nanocrystalline alloy samples with the same chemistry (Fe86B13Cu1) but with a range of mean grain sizes were prepared in order to investigate the effect of the grain size (D) on the core losses in nanocrystalline alloys. The core loss was measured on an Epstein frame in a frequency range between 10 Hz and 30 kHz. The measured core loss was separated into 3 parts, i.e. the hysteresis loss, classical eddy current loss and the excess loss. The classical eddy current loss is only a minor component due to the small thickness and moderately high electrical resistivity of the samples. Both the coercivity and the cycle hysteresis loss are found to follow roughly a D3 dependence. The excess loss at the maximum polarization (Jm) between 0.6 and 1.0 T is described universally by a simple power dependence of (Jm·f)n with an exponent of about 1.4 over a wide frequency (f) range between 10 Hz to 30 kHz. The excess loss at low frequencies appears almost independent of the grain size. Thus, the grain size effect on the total loss at low frequencies is attributable to the change in the hysteresis loss which reflects the static coercivity. However, the excess loss at 30 kHz shows a clear increase with an increase in D, indicating that the excess loss also becomes influential to the grain size dependence of the total core loss at high frequencies.</jats:p>