FeNiAlGaPBSiC非晶合金的晶化动力学

采用单辊急冷法制备了Fe68Ni1Al5Ga2P9.65B4.6Si3C6.75非晶薄带.用XRD、DSC研究合金的晶化动力学过程.结果表明:合金的玻璃转变和晶化行为均具有动力学效应,其晶化类型为初晶型和随后的共晶型反应.用Kissinger法计算得到的Eg、Ex、Ep1、Ep2分别为703、373、446、723 kJ/mol,Eg远大于Ex,表明该合金具有较高的热稳定性.     

块体非晶合金Cu58 Zr30 Ti10 Sn2的形成与晶化行为研究

采用铜模吸铸法制备了直径为2～3mm的圆柱状Cu60-xZr30Ti10Snx（x=0、1、2）块体非晶合金。用X射线衍射（XRD）和差式扫描量热仪（DSC）研究了非晶合金的结构、热稳定性和晶化特征，非晶合金Cu60-xZr30Ti10Snx的特征温度Tg、Tx、△Tx=（Tx-Tg）均与Sn含量相关。块体非晶合金Cu58Zr30Ti10Sn2的Tg为703．9K、Tx为755．5K、△Tx约为51．6K。这些特征温度随DSC升温速率的增大，不断向高温区偏移，其中晶化行为的这种动力学效应比其玻璃转变的更为显著。由Kissinger法获得的块体非晶合金Cu58Zr30Ti10Sn2的玻璃转变激活能Eg为3．30eV、晶化激活能Ex为3．17eV、第一晶化峰激活能Ep1为2．82eV、第二晶化峰激活能Ep2为3．13eV。由Ozawa法获得的各激活能比Kissinger法的相应数值稍偏低，但趋势是一致的。     

Fe73.5Cu1Nb3Si13.5B9非晶合金的晶化动力学

用差热分析（ＤＴＡ）结合Ｘ射线衍射（ＸＲＤ）,研究了Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９非晶合金的晶化动力学。结果表明：温度在０～７００℃范围内,该合金的晶化相为α－Ｆｅ和Ｆｅ２Ｂ;α－Ｆｅ相晶化表观激活能为４５２．３９ＫＪ／ｍｏｌ,Ｆｅ２Ｂ相的晶化表观激活能３９５．２３ＫＪ／ｍｏｌ;两相在晶化初期激活能最小,随晶化量Ｘｃ的增加而迅速境大,在α－Ｆｅ的体积分类为３０％～８０％,Ｆｅ２Ｂ的体积分     

Cu48Zr4l7块体非晶合金的晶化行为及热力学性能研究

采用水冷铜模吸铸工艺制备出了片状Cu48Zr45Al7,块体非晶合金.X射线衍射(XRD)表明,样品为完全非晶.利用差示扫描量热分析仪(DSC)在不同的升温速率下连续加热测得该片状非晶合金的热稳定性参数值,均随着升温速率的增加而增加,表明其玻璃转变和晶化行为均存在显著的动力学效应.运用Kissinger法计算出其玻璃转变温度激活能(Eg)、晶化温度激活能(Ex)和峰值温度激活能(Ep)分别为424.7 kJ·mol-1,326.3 kJ·mol-1和297.1kJ·mol-1.从热力学模型角度出发,对该合金的非晶形成能力进行了分析,计算出其混合焓ΔHchem=-25.55 kJ.mol-1和归一化错配熵So/kB=0.78.结果表明,该块体非晶合金具有较强的非晶形成能力(AFA)NI良好的热稳定性.     

Zr57Nb5Cu15.4Ni12.6Al10大块非晶合金的晶化动力学及显微硬度

采用铜模铸造法制备直径10 mm的圆柱状Zr57Nb5Cu15.4Ni12.6Al10大块非晶合金,并用X射线衍射(XRD)证明其为完全非晶态.应用示差扫描量热(DSC)分析方法测定该合金的玻璃转变的热学参量并分析其晶化过程.利用Kissinger法和Ozawa法计算了大块非晶合金表观晶化激活能.同时研究了退火温度对非晶合金显微硬度的影响.     

Nb对非晶态Fe-Co-Nd-B合金的晶化动力学的影响

在Fe-Co-Nd-B非晶合金中添加4%的Nb(原子分数)可延迟其晶化过程, 提高晶化温度, 并使其热稳定性显著提高. Nb抑制Fe₃B晶化相的形核, 但促进Fe₂₃B₆相的形核及长大. Nb可使晶化相的平均晶粒尺寸从30-60 nm减至14-20 nm. Nb使由初始晶化温度计算的晶化激活能明显降低. Fe-Co-Nd-B合金中, α-Fe(Co), Fe₃B和Nd₂(Fe, Co)₁₄B晶化相的形核过程要难于长大过程, 而加Nb后α-Fe(Co), Fe₂₃B₆和Nd₂(Fe, Co)₁₄B晶化相的长大过程要难于形核过程, 但Nb基本未改变晶化相的形核及长大机制. 非晶合金的晶化主要是一维界面控制的形核以及形核率随时间减小的三维长大过程.     

锆基大块非晶合金的晶化动力学研究

利用差示扫描量热法(DSC)和X射线衍射法(XRD)研究了非晶合金Zr65Al10Ni10Cu15和Zr52.5Al10Ni10Cu15Be12.5的晶化动力学情况.结果表明,在恒速升温情况下,随着升温速率的加快,非晶合金的特征温度TgTxTp均向高温区移动,其过冷液相区的宽度也逐渐增加,表明非晶合金的玻璃转变和晶化均具有动力学效应;在等温晶化情况下,利用JMA方程计算出两种合金的Avrami指数和有效激活能,由此得出这两种合金的晶化同为受扩散机制控制的形核率随时间增加而下降的晶化过程;并且非晶合金Zr52.5Al10Ni10Cu15Be12.5的热稳定性要强于Zr65Al10Ni10Cu15,经过分析认为,造成这一现象的主要原因是原子半径较小的Be原子与合金中的其它原子组成紧密的堆垛结构,抑制了合金元素的长程扩散.     

Zr57Nb5Cul5．4Nil2．6Al10大块非晶合金的晶化动力学及显微硬度

采用铜模铸造法制备直径10mm的圆柱状Zr57Nb5Cu15.4Ni12.6Al10大块非晶合金，并用X射线衍射(XRD)证明其为完全非晶态。应用示差扫描量热(DSC)分析方法测定该合金的玻璃转变的热学参量并分析其晶化过程。利用Kissinger法和Ozawa法计算了大块非晶合金表观晶化激活能。同时研究了退火温度对非晶合金显微硬度的影响。     

Cu64Zr36非晶合金的晶化动力学

利用单辊急冷法制备了CH64Zr36非晶合金，使用盐浴等温退火并用DSC和XRD研究了其晶化过程、玻璃转变和晶化动力学。结果表明：CH64Zr36非晶合金的晶化过程为：非晶一非晶＋Cu10Zr7→Cu10Zr7＋CuZr2。该合金的玻璃转变和晶化激活能分别为433．7kJ／mol和603kJ／mol。     

Zr57Cu15.4Ni12.6Al10Nb5块体非晶合金晶化行为研究

用示差扫描量热仪（DSC）研究了Zr57Cu15.4Ni12.6Al10Nb5块体非晶合金的匀速升温晶化与等温晶化的晶化行为。在匀速升温晶化方式下，用Kissinger法与Ozawa法获得了块体非晶合金的激活能，对第一晶化峰分别为320．5kJ／mol和316．6kJ／mol，对第二晶化峰分别为324．5kJ／mol和320．5kJ／mol。该非晶合金的晶化表现出明显的动力学效应。在等温晶化方式下，用Johnson-Mehl-Avrami方程获得了晶化的Avrami指数为1．61，表明非晶合金的晶化受原子扩散控制。     

Interface structure and properties of a brass-reinforced Ni59Zr20Ti16Si2Sn3 bulk metallic glass composite

Interfaces between a Ni₅₉Zr₂₀Ti₁₆Si₂Sn₃ bulk metallic glass (BMG) and crystalline brass reinforcements were characterized using transmission electron microscopy and nanoindentation. An interfacial layer with a thickness of ∼50–100 nm was observed in the composite prepared by warm extrusion of gas atomized powders. Microstructural characterization and chemical analysis suggest that the formation of interfacial layer was caused by interdiffusion between the BMG and brass during the warm extrusion. Nanoindentation in the vicinity of BMG–brass interfaces does not cause interface decohesion or crack formation, suggesting a strong interface bonding. Apparently, the resultant interfacial layer not only enhances interfacial bonding but also provides a buffer zone to prevent the catastrophic shear band propagation in the BMG matrix.     

Non-isothermal nano-crystallization kinetics in amorphous Ni55Nb35Si10 alloy

The non-isothermal crystallization kinetics of Ni₅₅Nb₃₅Si₁₀ amorphous alloy, prepared by mechanical alloying, was studied using differential scanning calorimetry. The amorphous alloy showed one-stage crystallization on heating, which led to the formation of nano-intermetallic crystals in amorphous matrix. The apparent activation energy for the crystallization of the alloy, determined by the Kissinger equation, was relatively high (468 kJ/mol), indicating that this amorphous alloy has high thermal stability. Changes in the activation energy during the crystallization process, were also evaluated by iso-conversional methods. The results showed that it decreases slowly from the beginning to crystallized fraction α=0.35 and it remains almost constant to the end of the process. The nano-crystallization mechanism for the non-isothermal crystallization of the amorphous alloy was explained by determining Avrami exponents. Transmission electron microscopy studies revealed the microstructural modification of amorphous alloy via nano-crystallization during annealing. The results suggest that the nucleation rate decreases with increasing time and the crystallization mechanism is governed dominantly by a three-dimensional diffusion-controlled growth. A predictive equation was obtained based on the Sestak?Berggren autocatalytic model to describe quantitatively the non-isothermal crystallization kinetics.     

非晶合金条带Fe73.5Cu1Nb3Si13.5B9的晶化动力学研究

采用差式扫描量热方法进行热分析实验,研究不同加热速率下非晶合金条带Fe73.5Cu1Nb3Si13.5B9的晶化动力学特性.DSC曲线的晶化温度和晶化峰值温度随着加热速率的增高而向高温方向迁移,说明合金的晶化过程表现出明显的动力学特性.建立基辛格模型,拟合动力学模型函数对结晶率的实验曲线,可以获得动力学参数值,得出晶化激活能的数值为2.89 eV.研究表明:对于Fe73.5 Cu1Nb3Si13.5B9合金,采用经验的双参数Sestak-Berggre模型能更加定量描述其晶化过程,而Johnson-Mehl-Avrami模型适宜在较低加热速率下描述.     

Crystallization of amorphous Zr70Cu30—xNix alloys

X－ray diffraction (XRD)and differential scanning calorimetry(DSC) were employed to investigate the influence of Ni content on the crystallization of amorphous Zr70Cu30-xNix(atom fration in%) alloys,Experimental results show that with the Ni content increasing the activation energies for crystallization of amorphous Zr70Cu30-xNix alloys increase correspondingly,indicating that the thermal stability is greatly improved.All the DSC traces of amorphous Zr70Cu30-xNix alloys exhibit two exothermic peaks,suggesting that the crystallization process via a double-stage ticles,while the second one corresponds to the precipitaion of nano-scale Zr2Ni phase and crystallization of residual amporphous phase,The mechanism on the crystallization of amorphous Zr70Cu30-xNix alloys was discussed.     

Zr5Si3及Zr3Ti2Si3弹性性质与热学性质

应用基于密度泛函理论的平面波赝势方法计算16H金属硅化物Zr5Si3及Zr3Ti2Si3的基态晶格参数,得出弹性常数、体弹性模量、弹性模量、剪切模量及泊松比等弹性性质.利用弹性常数计算德拜温度、格林奈森常数,并在德拜-格林奈森模型基础上计算这两种金属硅化物的各向异性热膨胀系数,由此得出Zr5Si3的a、c方向各向异性热膨胀系数(高温时)分别为8×10-6和15×10-6,对Zr3Ti2Si3(高温时)分别为11×10-6和13×10-6,与实验基本相符.根据方向体弹性模量、方向弹性模量及重叠布居数讨论两种材料各向异性热膨胀不同的原因.     

Crystallization of amorphous Zr60Al15Ni25 alloy

The phase formation and crystallization kinetics during the thermal treatment of amorphous Zr₆₀Al₁₅Ni₂₅ alloy were investigated by differential scanning calorimetry (DSC) and X-ray diffraction (XRD). By lowering the isothermal annealing temperatures, it is revealed that the crystallization of the amorphous Zr₆₀Al₁₅Ni₂₅ alloy consists of a primary transformation followed by a polymorphic transformation, corresponding to the precipitations of hexagonal Zr₆Al₂Ni and the Zr₅AlNi₄ with a U₃Si₂-typed superstructure. The primary phase being Zr₆Al₂Ni rather than Zr₅AlNi₄ in the crystallization is because the latter has a complex structure and its formation requires the diffusion of Al and Zr atoms on a large scale.     

Ti3Zr2Sn3Mo25Nb医用钛合金相变与力学性能

研究Ti3Zr2Sn3Mo25Nb医用钛合金中相变演化过程和亚稳相对合金强度和弹性模量的影响规律.结果表明:Ti3Zr2Sn3Mo25Nb合金中相的演化过程为β→ω→α″→α,其中亚稳ω相及α″相的尺寸、数量及分布对合金强度、弹性模量及塑性的影响显著.ω相的尺寸越小,数量越多,分布越均匀,这有利于提高合金强度,降低塑性和弹性模量;通过控制亚稳ω相及α″相的尺寸、数量和分布,可以在一定范围里调整Ti3Zr2Sn3Mo25Nb合金的力学性能变化,从而得到更好的生物力学性能匹配.     

Crystallization kinetics of Zr41Ti14Cu12.5Ni10Be22.5 bulk metallic glass

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Effects of Zr on crystallization kinetics of Pr—Fe—B amorphous alloys

The effects of Zr on crystallization kinetics of Pr-Fe-B amorphous alloys have been investigated by DTA and XRD methods.It was found that for Pr8Fe86-xZrxB6(x=0,1,2)amorphous alloys,the final crystallized mixture is α-Fe and Pr2Fe14B,and the metastable Pr2Fe23B3 phase occurs during crystallization of Pr8Fe86B6 amorphous alloy,not during crystallization of Pr8Fe86-xZrxB6(x=1,2)amorphous alloys,By analyzing the activation energy of crystallization,the formation of an α-Fe/Pr2Fe14B composite microstructure with a coarse grain size in annealed Pr8Fe86B6 alloy,is attributed to a difficult nucleation and an easy growth for both the α-Fe and Pr2Fe14B in the alloy.The addition of Zr can be used to change the crystallization behavior of the α-Fe phase in Pr-Fe-B amorphous alloy,which is helpful to reduce the grain size for the α-Fe phase.     

Cu47Ti34Zr11Ni8块体非晶合金的热稳定性和力学性能

采用差压铸造法成功制备了Cu47Ti34Zr11Ni8块体非晶合金,研究了其热稳定性和力学性能.结果表明:该块体非晶合金的玻璃转变温度Tg=672 K,晶化温度Tx1=735 K,过冷液相区△Tx=63 K,约化玻璃温度Trg=0.575,弯曲断裂强度高达2 350 MPa,断裂前弹性变形量为2.1%,弯曲模量为102 GPa;淬态微米级结晶相的出现使合金的三点弯曲断裂强度下降至1 100 MPa.