45,685 research outputs found

    Computational study on microstructure evolution and magnetic property of laser additively manufactured magnetic materials

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    Additive manufacturing (AM) offers an unprecedented opportunity for the quick production of complex shaped parts directly from a powder precursor. But its application to functional materials in general and magnetic materials in particular is still at the very beginning. Here we present the first attempt to computationally study the microstructure evolution and magnetic properties of magnetic materials (e.g. Fe-Ni alloys) processed by selective laser melting (SLM). SLM process induced thermal history and thus the residual stress distribution in Fe-Ni alloys are calculated by finite element analysis (FEA). The evolution and distribution of the Ī³\gamma-Fe-Ni and FeNi3_3 phase fractions were predicted by using the temperature information from FEA and the output from CALculation of PHAse Diagrams (CALPHAD). Based on the relation between residual stress and magnetoelastic energy, magnetic properties of SLM processed Fe-Ni alloys (magnetic coercivity, remanent magnetization, and magnetic domain structure) are examined by micromagnetic simulations. The calculated coercivity is found to be in line with the experimentally measured values of SLM-processed Fe-Ni alloys. This computation study demonstrates a feasible approach for the simulation of additively manufactured magnetic materials by integrating FEA, CALPHAD, and micromagnetics.Comment: 20 pages, 15 figure

    Absence of Magnetism in Hcp Iron-Nickel at 11 K

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    Synchrotron Mƶssbauer spectroscopy (SMS) was performed on an hcp-phase alloy of composition Fe92Ni8 at a pressure of 21 GPa and a temperature of 11 K. Density functional theoretical calculations predict antiferromagnetism in both hcp Fe and hcp Fe-Ni. For hcp Fe, these calculations predict no hyperfine magnetic field, consistent with previous experiments. For hcp Fe-Ni, however, substantial hyperfine magnetic fields are predicted, but these were not observed in the SMS spectra. Two possible explanations are suggested. First, small but significant errors in the generalized gradient approximation density functional may lead to an erroneous prediction of magnetic order or of erroneous hyperfine magnetic fields in antiferromagnetic hcp Fe-Ni. Alternately, quantum fluctuations with periods much shorter than the lifetime of the nuclear excited state would prohibit the detection of moments by SMS

    Phase equilibria and phase transformations in the Ti-rich corner of the Fe-Ni-Ti system

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    While the main features of the Fe-Ni-Ti system are well known at low Ti content, literature review of the Ti-rich corner revealed inconsistencies between experimental reports. This investigation presents new experimental results, defined to remove the uncertainties concerning melting behavior and solid-state phase equilibria of the (Ni,Fe)Ti2 phase with the adjacent (Fe,Ni)Ti (B2, CsCl-type structure) and Beta-Ti (A2, W-type) phases. Six samples have been prepared and examined by differential thermal analysis performed in yttria and alumina crucibles, and by scanning electron microscopy in the as-cast state as well as equilibrated at 900Ā°C

    Sound velocity and elastic properties of Feā€“Niā€“Sā€“Si liquid: the effects of pressure and multiple light elements

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    Feā€“Niā€“Sā€“Si alloy is considered to be one of the plausible candidates of Mercury core material. Elastic properties of Feā€“Niā€“Sā€“Si liquid are important to reveal the density profile of the Mercury core. In this study, we measured the P-wave velocity (VP) of Feā€“Niā€“Sā€“Si (Fe73Ni10S10Si7, Fe72Ni10S5Si13, and Fe67Ni10S10Si13) liquids up to 17 GPa and 2000 K to study the effects of pressure, temperature, and multiple light elements (S and Si) on the VP and elastic properties. The VP of Feā€“Niā€“Sā€“Si liquids are less sensitive to temperature. The effect of pressure on the VP are close to that of liquid Fe and smaller than those of Feā€“Niā€“S and Feā€“Niā€“Si liquids. Obtained elastic properties are KS0ā€‰=ā€‰99.1(9.4) GPa, KSā€™ā€‰=ā€‰3.8(0.1) and Ļ0 =6.48 g/cm3 for S-rich Fe73Ni10S10Si7 liquid and KS0ā€‰=ā€‰112.1(1.5) GPa, KSā€™ā€‰=ā€‰4.0(0.1) and Ļ0=6.64 g/cm3 for Si-rich Fe72Ni10S5Si13 liquid. The VP of Feā€“Niā€“Sā€“Si liquids locate in between those of Feā€“Niā€“S and Feā€“Niā€“Si liquids. This suggests that the effect of multiple light element (S and Si) on the VP is suppressed and cancel out the effects of single light elements (S and Si) on the VP. The effect of composition on the EOS in the Feā€“Niā€“Sā€“Si system is indispensable to estimate the core composition combined with the geodesy data of upcoming Mercury mission
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