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Erbium--iron (1/3) | 12400-78-1

中文名称
——
中文别名
——
英文名称
Erbium--iron (1/3)
英文别名
erbium;iron
Erbium--iron (1/3)化学式
CAS
12400-78-1
化学式
ErFe3
mdl
——
分子量
334.801
InChiKey
QKHXQWZZLQPLSW-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    -0.01
  • 重原子数:
    4
  • 可旋转键数:
    0
  • 环数:
    0.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    0
  • 氢给体数:
    0
  • 氢受体数:
    0

反应信息

  • 作为产物:
    描述:
    五羰基铁氢化铒 以 melt 为溶剂, 生成 Erbium--iron (1/3)
    参考文献:
    名称:
    基于热力学模型的Fe-Er合金玻璃形成能力分析
    摘要:
    Fe-Er相图及其所有相的热力学性质均通过自洽分析进行评估。为了完善Fe-Er系统中相平衡的数据,在10%至40%的Er浓度范围内进行了研究。熔体热力学性质的温度-浓度依赖性是使用理想的关联溶液模型来表示的。得到了各相的热力学参数,计算结果与现有实验数据相符。研究了液态Fe–Er合金的热力学性质与其非晶化趋势之间的相关性。结果表明,通过熔融淬火制备的非晶态合金的组成与Fe 3 Er和FeEr占优势的浓度范围一致。2个具有较大负熵形成的关联组。
    DOI:
    10.1134/s0036024418050035
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文献信息

  • The Er–{Fe,Co}–{Ti,V} systems and hydrogenation properties of the ErFe2−xMx (M=Ti, V, Cr, Mn, Co, Ni, Cu, Mo) alloys
    作者:B. Kotur、О. Мyakush、I. Zavaliy
    DOI:10.1016/j.jallcom.2007.01.126
    日期:2007.9
    phase diagrams of the Er–Fe,Co}–Ti,V} systems have been investigated by means of X-ray analysis. Existence of the Er M 12 − x M ′ x (M = Fe, Co; M′ = Ti, V) ternary compounds (ThMn 12 structure type, space group I 4/ mmm ) have been confirmed and their homogeneity ranges were determined. Formation of the ErM 2 -based solid solutions Er M 2 − x M ′ x (MgCu 2 structure type, space group Fd -3 m ) was
    摘要 已经通过 X 射线分析研究了 Er-Fe,Co}-Ti,V} 系统相图的等温截面。Er M 12 - x M ' x (M = Fe, Co; M' = Ti, V) 三元化合物(ThMn 12 结构类型,空间群I 4/ mmm )的存在已被证实,并确定了它们的均质范围。观察到基于ErM 2 的固溶体Er M 2 - x M ' x (MgCu 2 结构类型,空间群Fd -3 m )的形成。已经研究了 ErFe 2- x M x (M = Ti、V、Cr、Mn、Co、Ni、Cu、Mo) 合金的吸氢。
  • Phase equilibria at 773K and microwave absorbing properties of Er–Fe–Cr alloys
    作者:Shunkang Pan、Xing Liu、Lichun Cheng、Xiaokun Wang、Guanghui Rao、Qingrong Yao、Huaiying Zhou
    DOI:10.1016/j.jallcom.2014.03.180
    日期:2014.8
    The phase equilibria of Er-Fe-Cr system at 773 K were investigated by X-ray powder diffraction (XRD), differential thermal analysis (DTA), and scanning electron microscopy (SEM) equipped with energy dispersive spectroscopy (EDS). The isothermal section consists of 8 single-phase regions, 14 two-phase regions and 7 three-phase regions. The homogeneity range of the ternary compound ErFe12 Cr-x(x) was determined to be x = 1.6-3.0. The maximum solid solubilities of Cr in ErFe2, ErFe3, Er6Fe23, Er2Fe17, and Fe are about 8.2, 1.2, 15.6, 9.6 and 13.8 at.% Cr, respectively, and the solubility limit of Fe in Cr is about 13.3 at.% Fe. The microwave absorbing properties of the intermetallic compounds in Er-Fe-Cr system were determined. All the samples exhibited good absorbing property in the X-band (8-12 GHz). With a coating thickness of d = 2.0 mm, the minimum return loss at the absorption peak frequency of the ErFe2, ErFe3, Er6Fe23, Er2Fe17 and ErFe10Cr2 are -19.66 dB at 9.6 GHz, -29.57 dB at 8.16 GHz, -35.04 dB at 12.72 GHz, -22.72 dB at 9.76 GHz and -13.51 dB at 11.2 GHz, respectively. (C) 2014 Elsevier B. V. All rights reserved.
  • The isothermal section of the Er–Fe–Sb ternary system at 773K
    作者:Gemei Cai、Xiangzhong Wei、Lingmin Zeng
    DOI:10.1016/j.jallcom.2005.10.039
    日期:2006.8
    The phase relation of the Er-Fe-Sb ternary system at 773 K has been investigated mainly by means of X-ray powder diffraction with the aid of optical microscopy and differential thermal analysis. This section consists of 12 single-phase regions, 22 two-phase regions and I I three-phase regions. A ternary compound Er6FeSb2 has been confirmed. (c) 2005 Elsevier B.V. All rights reserved.
  • Peculiarity of component interaction in Er–Fe–Sn ternary system at 670K and 770K
    作者:L. Romaka、V.V. Romaka、P. Demchenko、R. Serkiz
    DOI:10.1016/j.jallcom.2010.07.137
    日期:2010.9
    The isothermal sections of the phase diagram of Er-Fe-Sn ternary system were constructed at 770 and 670 K in the whole concentration range using X-ray and metallographic analyses. Component interaction in the Er-Fe-Sn system at 670 K results the existence of two ternary compounds, ErFe(6)Sn(6) (YCo(6)Ge(6)-type) and Er(5)Fe(6)Sn(18) (Tb(5)Rh(6)Sn(18)-type), while at 770 K only one intermediate ErFe(6)Sn(6) phase was observed. The existence of the interstitial solid solution ErFe(x)Sn(2) (up to 5 at.% Sn) was found at both temperatures. (C) 2010 Elsevier B.V. All rights reserved.
  • Phase relationships in the Er–Fe–Mn ternary system at 773K
    作者:Jingqi Liu、Kunpeng Su、Xueqiang Li、Xina Wang、Xiaomao Yang、Mengqi Tang、Chunhui Li
    DOI:10.1016/j.jallcom.2008.06.108
    日期:2009.4
    In order to determine the existence of phases and relationships in the Er-Fe-Mn system at 773 K, we have carried out this work mainly by X-ray powder diffraction with the aid of differential thermal analysis and have obtained the conclusions below. The existence of seven binary compounds ErFe2, ErFe3, Er6Fe23, Er2Fe17, ErMn12, Er6Mn23, ErMn23 and one intermediate solid solution gamma(Fe center dot Mn) have been confirmed in this system. Er6Fe23 and Er6Mn23 form continuous solid solution Er-6 (Fe23-X Mn-X) (0 <= X <= 23). At 773 K, the maximum solid solubility of Fe in alpha Mn, ErMn12, ErMn2 phases and Mn in ErFe2, Er2Fe17, alpha Fe phases are about 31, 69, 13 at% Fe and 47, 28, 8 at% Mn, respectively. The homogeneity range of gamma(Fe center dot Mn) phase extended from about 34 at% Mn to 52 at% Mn. The maximum solid solubility of Er in gamma(Fe center dot Mn) phase is about 2 at% Er. The isothermal section consists often single-phase regions, sixteen two-phase regions and seven three-phase regions. No ternary compounds were observed at 773 K in this system. (C) 2008 Elsevier B.V. All rights reserved
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