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Structures of bulk amorphous Zr_(41) Ti_(14) Ni_(10) Cu_(12.5) Be_(22.5)alloy in amorphous, crystalline, supercooled liquid and liquid states
作者姓名:田学雷  李成栋  陈熙琛  刘峰  A.G.Ilinsky
作者单位:1. Key Laboratory of Liquid Structure and Heredity of Materials,Ministry of Education,handong University,Ji′nan 250061,China; 2. Shandong Institute of Labour
基金项目:Project (Q99F16 )supportedbytheNaturalScienceFoundationofShandongProvince
摘    要:1 INTRODUCTIONThebulkamorphousalloysofMg TM Ln ,Ln Al TM ,Zr Al TM ,Hf Al TMandTi Zr TMwerepreparedbyInoueandhisco workerssince 1990 1] .Thec


Structures of bulk amorphous Zr41Ti14Ni10Cu12.5Be22.5 alloy in amorphous, crystalline, supercooled liquid and liquid states
A.G.Ilinsky.Structures of bulk amorphous Zr_(41) Ti_(14) Ni_(10) Cu_(12.5) Be_(22.5)alloy in amorphous, crystalline, supercooled liquid and liquid states[J].Transactions of Nonferrous Metals Society of China,2002,12(1).
Authors:AGIlinsky
Abstract:The amorphous and crystal structures of Zr 41 Ti 14 Ni 10 Cu 12.5 Be 22.5 alloy have been analyzed with X ray diffractometer. The structures of bulk amorphous Zr 41 Ti 14 Ni 10 Cu 12.5 B 22.5 alloy in solid, supercooled liquid and liquid states are almost of the same structure. The RDFs (Radius Distribution Function), the first coordination number, the first coordination radius, the correlation radius and atom number of the cluster were calculated for bulk amorphous Zr 41 Ti 14 Ni 10 Cu 12.5 B 22.5 alloy in different states. The first coordination sphere radii and the first coordination numbers are 0.312?nm, 11.2 in solid state, 0.301?nm, 10.932 in supercooled liquid region and 0.305?nm, 11.296 in liquid state. The crystal structure of Zr 41 Ti 14 Ni 10 Cu 12.5 B 22.5 alloy is consisted of several intermetallic compounds which are CuZr 2, Be 2Zr, etc. The reason of formation glass for this alloy is that there is a larger resistance for atoms to rearrange and form intermetallic compounds in a long range order.
Keywords:bulk amorphous  liquid structure  crystal structure
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