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Thermal and Magnetic Properties of Bulk Fe-Based Glassy Alloys Prepared by Copper Mold Casting

机译:铜铸件制备的块状铁基玻璃态合金的热和磁性能

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Bulk glassy Fe_(73) Al_5Ga_2P_(11)C_5B_4 alloys in cylindrical form with diameters of 0.5 and 1,0 mm were found to form by a copper mold casting method. The further increase in diameter causes the formation of coexistent glassy, Fe_3(B, C), Fe_2B and Fe_3P phases for the 1.5 mm sample and coexistent Fe_3(B, C), Fe_2B and Fe_3P phases for the 2.0 mm* sample. It is to be noticed that the maximum thickness for glass formation is about 10 times larger than the largest thickness for Fe-based glassy alloys reported up to date. The glass transition temperature (T_g), crystallization temperature (T_x) and heat of crystallization of the 1.0 mm glassy alloy are 732 K, 785 K and 3.76 kJ/mol, respectively. No appreciable difference in the thermal stability and magnetic properties is seen between the bulk glassy alloys and the melt-spun ribbon. The 1.0 mm glassy alloy has ferromagnetism with a Curie temperature of 606 K and exhibits 1.26 T for saturation magnetization (B_s), 82 A/m for coercivity (Hc) and 0.38 for the ratio of residual magnetization to B_s at room temperature. The large triangle openT_X(= Tx - T%) and large glass-forming ability can be obtained for the Fe-based alloy containing simultaneously the five solute elements. The effectiveness of the multiplication is presumably due to the combination of the following three effects; (1) the suppression of crystalline nuclei due to the increase in dense random packing density for the glassy structure containing P, C and B with significantly different atomic sizes, (2) the difficulty of atomic rearrangements for the precipitation of the Fe-metalloid compounds caused by the generation of Al-metalloid pairs with strongly attractive bonding nature, and (3) the decrease in the preferential precipitation tendency of Fe-B and Fe-C compounds by the dissolution of Ga which is immiscible to B and C and soluble to Fe.
机译:发现通过铜铸模法形成直径为0.5和1.0mm的圆柱形的块状玻璃状Fe_(73)Al_5Ga_2P_(11)C_5B_4合金。直径的进一步增加导致形成1.5mm样品共存的玻璃相,Fe_3(B,C),Fe_2B和Fe_3P相,以及2.0mm *样品共存的Fe_3(B,C),Fe_2B和Fe_3P相。要注意的是,玻璃形成的最大厚度大约是迄今为止报道的Fe基玻璃态合金的最大厚度的10倍。 1.0mm玻璃态合金的玻璃化转变温度(T_g),结晶温度(T_x)和结晶热分别为732K,785K和3.76kJ / mol。在块状玻璃态合金和熔纺带材之间没有观察到热稳定性和磁性能的明显差异。 1.0毫米玻璃态合金具有居里温度为606 K的铁磁性,在室温下饱和磁化强度(B_s)为1.26 T,矫顽力(Hc)为82 A / m,剩余磁化强度与B_s的比值为0.38。对于同时包含五个溶质元素的铁基合金,可以获得大的三角形openT_X(= Tx-T%)和大的玻璃形成能力。乘法的有效性大概是由于以下三个效果的组合; (1)由于原子尺寸明显不同的含P,C和B的玻璃态结构的致密无规堆积密度增加而导致的晶核抑制,(2)Fe类金属化合物沉淀的原子重排困难(3)通过与B和C不混溶并溶于C的Ga的溶解,降低了Fe-B和Fe-C化合物优先析出趋势的产生。铁

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