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铝-铜-镓三元系合金相图的室温截面已经用X射线方法测定出来了。室温固相截面包含11个单相(即α, γ2, γ′, δ, ζ1, ζ2, η2, θ, θ′,α铝和镓)相区,14个双相(即α + ζ1, α+ γ2, α + γ′, γ2 + γ′, γ′+ ζ1, γ2+δ, γ′+δ,δ +ζ2, ζ2+η2, η2+θ,η2+ θ′, γ′ + θ′, θ′+ 镓和θ+α铝)相区和9个三相(即α + γ′+ζ1, α+ γ2+ γ′, γ2+ γ′ + δ,γ′ + δ + θ′, δ+ζ2+θ′, ζ2 + η2 + θ′, η2+ θ′ + 镓, η2 +θ + 镓和θ +镓+ α铝)相区。所有单相和三个二元系内室温存在的单相相同,没有新相出现。
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本文用X射线衍射法测定了铝-铜-镉三元系合金相图。室温等温截面包含α,γ2,δ,ζ2,η2,θ,Al,Cd,ε,δ',γ,β十二个单相区;二十一个双相区(即α+γ2,γ2+δ,δ+ζ2,ζ2+η2,η2+θ,θ+Al,Al+Cd,α+β,β+γ,γ+δ',δ'+ε,ε+Cd,α+γ,α+δ',γ2+δ',γ2+ε,δ+ε,δ+Cd,ζ2+Cd,η2+Cd,θ+Cd);以及十个三相区(即α+β+γ,α+γ+δ',γ2+α+δ',γ2+δ'+ε,δ+γ2+ε,δ+ε+Cd,ζ2+δ+Cd,η2+ζ2+Cd,θ+η2+Cd,θ+Al+Cd),所有单相与三个二元系中的单相一致,没有新相出现。 相似文献
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用X射线方法测定了银-锡-铝三元系合金相图。合金含量从30wt.%Sn到纯锡,从30wt.%Al到纯铝。同时,对此三元系的富银角(<30wt.%Sn,<30wt.%Al)相图的γ相区,ζ+δ相区和β+γ+δ相区重新做了测定。室温相截面由六个单相(即α,μ,β,γ,Sn和δ)相区,八个双相(即α+μ,α+β,β+μ,β+γ,γ+Sn,β+Sn,β+δ及Sn+δ)相区,和三个三相(即α+β+μ,β+γ+Sn及β+Sn+δ)相区所构成。所有单相与三个二元系的单相一致,没有新相出现。 相似文献
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A thorough investigation by means of X-rays has been carried out with the purpose to determine the nature of the ternary phase τ in Al-Cu-Ni alloys. In contrast with the conventional concept of alloy phase which is characterized by a definite type of crystal structure, systematic structure changes are found in the single phase field of τ which occupies quite an extensive area in the isothermal section of the phase diagram at room temperature. There are eight types of structures altogether, all derived from a basic rhombohedron with corners occupied by Al atoms and centres either occupied by the heavy atoms or remaining vacant. The basic rhombohedron is the building stone in the crystal architecture. By transforming the basic rhombohedron into a hexagonal prism in the usual way, all structures may be considered to be built up by stacking together a number of these hexagonal prisms along the triad. The transformation of one structure into another is quite systematic in the way that the number of the stacking stories in the unit cell increases according to the order 10, 11, 12, 13, 14, 15, 16, 17. The atomic arrangements in the different structures are closely related too, in the respect that they are all superstructures due to the presence of ordered vacancies in the rhombohedral centres.The principal factor controlling the formation of these structures has been fully considered. In view of the fact that the change of structure types follows closely with the content of Ni or Cu for alloys of constant Al content, the atomic size factor appears to be unimportant in the formation of these alloys. It has been shown that for alloy phases of the defect lattice type as the r-phase, the most fundamental factor is the average number of valency electrons per structural unit which is the basic rhombohedron in the present case. By assuming Hume-Rothery's valencies, the average number of valency electrons remains remarkably constant throughout the entire phase field, while the electron concentration varies with compositions. It has also been pointed out that for alloy phases where there is no unit cell change, the average number of electrons per structural unit is equivalent to the number of electrons per unit cell, and for alloy phase where there is no defect, this is in effect equivalent to the electron concentration. 相似文献
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为开发新型Bi系高温超导用银合金,使其具有良好的机械性能,我们制备了AgMg0.05V0.05和AgMg0.10V0.075合金,研究了这两种合金经过不同条件退火处理后的室温拉伸性能.实验结果表明,合金化对提高材料的强度有显著效果;由光学金相照片观察到,银合金经过空气气氛退火后,形成了氧化物析出相,使强度进一步提高.AgMg0.05V0.05合金经820℃、40h空气退火处理后,屈服强度和抗拉强度分别高达110MPa和217MPa,克服了AgMgNi合金在较高温度退火强度下降的缺点.获得在高温长时处理后保持高强度的包套合金材料.对提高超导带材的机械强度和传输性能以及工程上的应用具有重要的意义. 相似文献
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为开发新型Bi系高温超导用银合金,使其具有良好的机械性能,我们制备了AgMg0.05V0.05和AgMg0.10V0.075合金,研究了这两种合金经过不同条件退火处理后的室温拉伸性能.实验结果表明,合金化对提高材料的强度有显著效果;由光学金相照片观察到,银合金经过空气气氛退火后,形成了氧化物析出相,使强度进一步提高.AgMg0.05V0.05合金经820℃、40h空气退火处理后,屈服强度和抗拉强度分别高达110MPa和217MPa,克服了AgMgNi合金在较高温度退火强度下降的缺点.获得在高温长时处理后保持高强度的包套合金材料,对提高超导带材的机械强度和传输性能以及工程上的应用具有重要的意义. 相似文献
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本文用X射线粉末照相法和差热分析法测定了Gd-Cu二元系合金相图,发现GdCu6在735℃发生同素异构转变。此合金系中共存在着四种金属互化物,即GdCu,GdCu2,GdCu5和GdCu6,金属互化物GdCu,在932℃同成份熔化;而GdCu,GdCu2和GdCu6分别在759℃,870℃和884℃由包晶反应形成,存在两个共晶反应,分别发生在32at%Cu668℃和92at%Cu875℃,无论是Gd在Cu中或是Cu在Gd中都没有可觉察的固溶度。
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