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首页> 外文期刊>Materials transactions >Magnetic properties and phase transformations of bulk amorphous Fe-based alloys obtained by different techniques
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Magnetic properties and phase transformations of bulk amorphous Fe-based alloys obtained by different techniques

机译:通过不同技术获得的块状非晶态铁基合金的磁性和相变

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摘要

Bulk amorphous Fe{sub}65.5Cr{sub}4Mo{sub}4Ga{sub}4P{sub}12C{sub}5B{sub}5.5 rods with diameters of 1.5-3 mm were prepared by copper mold casting. Besides casting, bulk amorphous Fe{sub}77Al{sub}2.14Ga{sub}0.86P{sub}8.4C{sub}5B{sub}4Si{sub}2.6 samples in the shape of discs (diameter of 10 mm and thickness of 3 mm) were prepared from melt-spun ribbons by high-energy ball milling and subsequent compaction of the resulting powders in the supercooled liquid region. The ascast amorphous FeCrMoGaPCB samples exhibit a low coercivity, below 10 A·m{sup}(-1). In the case of the FeAlGaPCBSi alloy, the milling-induced stress causes significant differences in coercivity between the ribbons and the powders. The relatively low coercivity of about 5-10 A·m{sup}(-1) characteristic for the melt-spun ribbons increases after 1 hour of ball milling to a value of about 2200 A·m{sup}(-1). Subsequent annealing of the ball-milled powders leads to a decrease of H{sub}c by a factor of 10 to about 220-250A·m{sup}(-1). The bulk samples prepared by hot pressing of the crushed ribbons show a coercivity of about 120-140 A·m{sup}(-1). For both alloys, thermal stability measurements show a distinct glass transition, followed by a supercooled liquid region of 60K for Fe{sub}65.5Cr{sub}4Mo{sub}4Ga{sub}4P{sub}12C{sub}5B{sub}5.5 and of 30K for Fe{sub}77Al{sub}2.14Ga{sub}0.86P{sub}8.4C{sub}5B{sub}4Si{sub}2.6. For the Fe{sub}65.5Cr{sub}4Mo{sub}4Ga{sub}4P{sub}12C{sub}5B{sub}5.5 alloy, crystallization of the amorphous phase as observed by in-situ X-ray diffraction measurements in transmission configuration occurs via the formation of a metastable intermediate phase. The phases observed in the crystalline state obtained by heating do not correspond to those occurring after slow cooling.
机译:通过铜模铸造制备了直径为1.5-3mm的块状非晶Fe {sub} 65.5Cr {sub} 4Mo {sub} 4Ga {sub} 4P {sub} 12C {sub} 5B {sub} 5.5棒。除铸造外,块状非晶态Fe {sub} 77Al {sub} 2.14Ga {sub} 0.86P {sub} 8.4C {sub} 5B {sub} 4Si {sub} 2.6样品呈圆盘状(直径为10 mm,厚度为10mm)通过高能球磨由熔融纺丝的条带制备3mm的粉末(3mm),随后将所得粉末在过冷的液体区域中压实。铸态非晶态FeCrMoGaPCB样品的矫顽力低,低于10 A·m {sup}(-1)。在FeAlGaPCBSi合金的情况下,铣削引起的应力会导致薄带和粉末之间的矫顽力产生显着差异。球磨1小时后,熔纺带的相对较低的矫顽力约为5-10 A·m {sup}(-1),此值会增加到约2200 A·m {sup}(-1)。球磨粉末的随后退火导致H {c}降低10倍至约220-250A·m {sup}(-1)。通过热压碎的条带制备的块状样品显示出约120-140A·m {sup}(-1)的矫顽力。对于这两种合金,热稳定性测量均显示出明显的玻璃化转变,随后是Fe {sub} 65.5Cr {sub} 4Mo {sub} 4Ga {sub} 4P {sub} 12C {sub} 5B {sub } 5.5和30K用于Fe {sub} 77Al {sub} 2.14Ga {sub} 0.86P {sub} 8.4C {sub} 5B {sub} 4Si {sub} 2.6。对于Fe {sub} 65.5Cr {sub} 4Mo {sub} 4Ga {sub} 4P {sub} 12C {sub} 5B {sub} 5.5合金,通过原位X射线衍射测量观察到非晶相的结晶通过形成亚稳定的中间相而发生在传输构型中的“α”。通过加热获得的结晶状态下观察到的相与缓慢冷却后发生的相不对应。

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