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采用静态拉伸方法在连续升温条件下动态地测量了大块金属玻璃Zr41Ti14Cu12.5Ni10Be22.5(Vit1)的黏度随温度的变化关系.在应变速率与温度的关系曲线中,观测到了与玻璃转变和晶化过程相联系的多个应变速率峰.在玻璃转变温度Tg以上,大块金属玻璃Zr41Ti14Cu12.5Ni10Be22.5的过冷液体呈现Newton流体特征,其黏度与温度的关系符合Vogel Fulcher-Tammann (VFT)关系式,拟合得到脆度D*=36,VFT温度T0=319K,脆度参数m=30,这说明Zr41T
关键词:
大块金属玻璃
应变速率
剪切黏度
自由体积 相似文献
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Kinetics of the glass Transition of the Zr41Ti14Cu12.5Ni10Be22.5 Alloy Solidified in a Drop Tube
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Droplets of Zr41Ti14Cu12.5Ni10Be22.5 glass-forming alloy with different sizes are solidified in a drop tube containerless process.The glass transition temperature Tg of Zr41Ti14Cu12.5Ni10Be22.5 glassy spheres solidified with different cooling rates is investigated by using a differential scanning calorimeter.It was found that all the amor phous spheres show an increase of Tg with the heating rate.The glassy spheres have a unique value for the glass transition activation energy Eg=435.50kJ/mol,which is independent of cooling rate q.The insensitivity of Tg to q is interpreted by an extension of the free volume model for flow. 相似文献
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通过离子注入结合二次离子质谱分析方法,研究了高压下Co在Zr46.75Ti8.25Cu7.5Ni1oBe27.5大块金属玻璃过冷液相区中的扩散行为.在603 K时,Co在Zr46.75Ti8.25Cu7.5Ni10Be27.5大块金属玻璃中的扩散系数随压力的增大而增大,其扩散激活体积ΔV*=-1.236Ω,Ω是合金的平均原子体积.结果表明,在热平衡状态下Co在Zr46.75Ti8.25Cu7.5Ni10Be27.5大块金属玻璃中的扩散是通过间隙机理进行的. 相似文献
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Nanoscale Inhomogeneities in the Glass Transition of Zr41.2Ti13.8Cu12.5Ni10Be22.5 Bulk Metallic Glass 总被引:1,自引:0,他引:1
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《中国物理快报》2005,22(3):664-666
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通过离子注入结合二次离子质谱分析方法 ,研究了高压下Co在Zr4 6 .75Ti8.2 5Cu7.5Ni1 0 Be2 7.5大块金属玻璃过冷液相区中的扩散行为 .在 6 0 3K时 ,Co在Zr4 6 .75Ti8.2 5Cu7.5Ni1 0 Be2 7.5大块金属玻璃中的扩散系数随压力的增大而增大 ,其扩散激活体积ΔV =- 1.2 36Ω ,Ω是合金的平均原子体积 .结果表明 ,在热平衡状态下Co在Zr4 6 .75Ti8.2 5Cu7.5Ni1 0Be2 7.5大块金属玻璃中的扩散是通过间隙机理进行的 相似文献
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测量了块体金属玻璃Zr46.75Ti8.25Cu7.5Ni10Be27.5在退火前后其电阻值随温度的变化,测量的温度范围为1.5-300K.样品在退火前后都发现有超导现象.零磁场下其超导转变温度Tc分别为1.84和3.76K.在5-300K温度范围内,原始样品具有负的电阻温度系数.如果取Zr,Ti,Cu,Ni及Be分别贡献出1.5,1.5,0.5,0.5及两个传导电子,则可以用扩展的Faber-Ziman理论去解释原始样品的负电阻温度系数.还对块体金属玻璃Zr46.75Ti8.25Cu7.5Ni10Be27.5在温度范围5-300K之间的R(T)曲线用一个多项式进行了拟合. 相似文献
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以1at% Ag元素分别等量替代Zr57Cu20Al10Ni8Ti5金属玻璃的各个组元,利用差示扫描量热升温分析获得不同试样的热力学参数,并结合不同尺寸(Φ8,Φ10,Φ12)吸铸试样的X-射线衍射分析结果,考察、验证元素替代后合金的实际玻璃形成能力及热稳定性的变化规律.经比较发现,Ag替代Ti元素,其玻璃形成能力显著提高(直径实际增大4 mm),同时热稳定性也明显改善,且临界冷却速率也明显降低,而Ag替代其他组元却无明显规律.针对玻璃形成能力的相关数据比较分析表明,本文结果未显示符合其Inoue的尺寸准则,混合焓判据也未显示出明显符合的现象.通过对堆垛密度的计算发现,1 at% Ag替代Ti元素后使金属玻璃体系内部的堆垛密度增加.通过动力学分析,从晶化激活能、晶化反应速率常数两方面探讨了元素替代对玻璃形成能力和热稳定性的作用机理. 相似文献
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报道一个新的Pr55Al12Fe30Cu3 大块金属玻璃.采用铜模吸铸法制备了直径为5 mm、长度达100 mm的Pr55Al12Fe30Cu3 大块金属玻璃.差示扫描量热分析结果表明在该Pr基大块金属玻璃体系具有宽达64 K左右的过冷液相区,而且该合金呈非晶态时的熔化温度要比相应晶态样品的熔化温度高约140 K.磁滞回线测量表明非晶态Pr55Al12Fe30Cu3 块体合金在室温下呈现永磁特性,而完全晶化后样品在室温下呈现软磁特性.
关键词:
大块金属玻璃
玻璃转变
晶化
永磁性 相似文献
11.
LI Gong ZHAN Zaiji LIU Jing YUN Jinku SUN Liling LIU Riping ZHANG Jun & WANG Wenkui . Key Laboratory of Metastable Materials Science Technology Yanshan University Qinhuangdao China . Center for Condensed Matter Physics Institute of Physics Chinese Academy of Sciences Beijing China . BSRF Institute of High Energy Physics Chinese Academy of Sciences Beijing China 《中国科学G辑(英文版)》2005,48(3)
With the development of multicomponent Zr-based glass bulk metallic glasses(BMGs) with a larger geometry by a conventional casting process with a low coolingrate[1—4], high pressure, which is the simplest way to vary the interatomic distance ofsubstance and thus change its physical properties, has been employed as an importantmeans to investigate structural relaxation and the crystallization of the BMGs[5]. Relativeto crystalline, metallic glasses have excess free volume, which will annihil… 相似文献
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Zr41Ti14Cu12.5Ni10Be22.5bulk metallic glass (BMG) is annealed at 573 K under 3 GPaand its structural relaxation is investigated by X-ray diffraction, ultrasonic study, compression as well as sliding wear measurements. It is found that after the ZrTiCuNiBe BMG sample was annealed under high pressure, the mechanical properties were improved. Moreover, the BMG with relaxed structure exhibits markedly different acoustic properties. These results are attributed to the fact that relaxation under high-pressure results in a microstructural transformation in the BMG. 相似文献
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In this paper, Cu52Zr37Ti8In3 bulk metallic glass has been studied by nanoindentation. Three different ways for nanoindentation tests were employed. Load-control nanoindentation was used to investigate the effect of the loading rate on the hardness and Young’s modulus. Young’s modulus of the specimen shows a loading rate dependence. The constant-load indentation creep measurement was performed. The creep data were fitted with the generalized Kelvin model, and the compliance spectrum and retardation spectrum were derived. Furthermore, the storage compliance and loss compliance were also discussed. For characterizing the change of the hardness and Young’s modulus with increasing indentation depth, depth-control nanoindentation analysis was conducted. The results show that both the hardness and Young’s modulus decrease with nanoindentation depth. 相似文献