Crystallization kinetics of bulk Cu58.1Zr35.9Al6 alloy

The crystallization kinetics of the bulk amorphous Cu_58.1Zr_35.9Al₆ alloy was examined by differential scanning calorimetry under continuous heating and isothermal annealing. During continuous heating, the activation energy of crystallization was determined to be 383 kJ/mol by Kissinger method. However, on the isothermal annealing, the activation energy was determined to be 459.2 kJ/mol by the Arrhenius method, which was much larger than that obtained from the Kissinger method. The different temperatures at which crystallization occurs are responsible for the discrepancy in the activation energy. The average Avrami exponent of about 3.5 implies that the crystallization process of the bulk amorphous Cu_58.1Zr_35.9Al₆ alloy is diffusion-controlled with a nucleation rate decreasing with time.     

Crystallization behavior of amorphous Zr70Cu20Ni10 alloy annealed at 380℃

Crystallization behavior of amorphous Zr70Cu20Ni10 alloy isothermally annealed at 3800℃ was first investigated by employing the differential scanning calorimetry (DSC) and transmission electron microscopy(TEM). It has been found that an exothermic peak appears in the DSC trace when the annealing time is about 17-18min,in dicating a certain phase transformation occurs in the matrix of amorphous Zr70 Cu20 Ni10 alloy.Meanwhile,isothermal annealing experiments for amorphous Zr70Cu20Ni10 alloy ranging from 370℃ to 400℃with a temperature interval of 10℃ were also carried out,from which no exothermic reaction can be observed except for the case of 380℃.This behavior indicates that the phase transformation during isothermal annealing of amorphous Zr70Cu20Ni10 alloy is strongly temperature-and time-dependent.Further investigations are required to reveal the nature of such phenome non.     

Mg60Cu30Y10块体非晶合金的变温晶化行为

采用示差扫描量热仪(DSC)得到Mg60Cu30Y10块体非晶合金在不同加热速率下的DSC曲线。利用Losocka、Kissinger以及Doyle方法研究了Mg60Cu30Y10块体非晶合金的非等温晶化动力学。结果表明:Mg60Cu30Y10块体非晶合金具有良好的热稳定性。通过Kissinger方法计算得到的其玻璃转变激活能(Eg)、晶化激活能(Ex)以及晶化峰值激活能(Ep)分别为160.07 kJ/mol、136.11和145.19 kJ/mol。随着加热速率的提高,各特征温度值向高温端移动。局域晶化激活能随着复合材料晶化体积分数的增加先增大后减小。     

Zr65Al10Ni10Cu15非晶合金电阻率的研究

在不同加热速率下利用恒流四电极法研究了非晶合金Zr65Al10Ni10Cu15的电阻率随温度的变化情况,根据电阻率随温度的变化情况可以把晶化前的温度区间分为3个阶段,第一和第二阶段分别对应于低温结构弛豫和高温度结构弛豫发生的温度区间,而第三阶段的变化情况与前二个阶段明显不同,并在晶化前出现电阻率极大值峰。研究表明,利用电阻率随温度的变化情况,可以反映出非晶更多的结构转变的信息。     

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.     

Zr65Al7.5Cu17.5Ni10大块非晶态合金的制备及晶化过程

采用直接水淬法成功制备直径５ｍｍ球状Ｚｒ６５Ａｌ７．５Ｃｕ１７．５Ｎｉ１０大块非晶态合金。Ｘ射线衍射、透射电镜检验证明样品完全为非晶态。采用Ｘ射线衍射、差示扫描热分析仪（ＤＳＣ）分析了Ｚｒ６５Ａｌ７．５Ｃｕ１７．５Ｎｉ１０非晶态合金的晶化过程,利用Ｋｉｓｓｉｎｇｅｒ方程求得Ｚｒ６５Ａｌ７．５Ｃｕ１７．５Ｎｉ１０非晶合金的晶化表观激活能。Ｘ射线衍射实验结果表明,Ｚｒ６５Ａｌ７．５Ｃｕ１７．５Ｎｉ１０非晶态合金的晶化是按下面的次序进行的,非晶态合金→体心立方晶相Ｚｒ２（Ｎｉ,Ａｌ）＋非晶相→体心立方相Ｚｒ２（Ｎｉ,Ａｌ）＋体心立方相Ｚｒ２（Ｃｕ,Ａｌ）。     

非晶合金Mg_(65)Y_(10)Cu_(25)在3.5%NaCl溶液中的腐蚀行为

利用电化学极化曲线方法、交流阻抗 (EIS)技术和扫描电子显微镜 (SEM )研究了Mg65Y10 Cu2 5非晶及相应的晶化合金在 3 5 %NaCl溶液中的腐蚀行为。极化曲线测试结果表明 ,非晶合金Mg65Y10 Cu2 5在NaCl溶液中为活性溶解 ,腐蚀反应由阴极反应和阳极反应共同控制。EIS测试表明 ,随着浸泡时间延长 ,非晶合金耐蚀性下降 ,EIS由 3个时间常数变为 2个时间常数。SEM测试表明 ,非晶合金经过 2 4h浸泡后 ,表面发生了极为不均匀的腐蚀 ;EDAX能谱表明 ,非晶合金经过浸泡后 ,表面成分发生了较大变化 ,含镁量减少 ,表面出现了浓度分布不均匀的氧元素。晶化后Mg65Y10 Cu2 5合金的耐蚀性略有提高。探讨了非晶合金在 3 5 %NaCl溶液中的腐蚀机理     

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

1　ＩＮＴＲＯＤＵＣＴＩＯＮＴｈｅｍｅｔａｌｌｉｃｇｌａｓｓｅｓｈａｖｅｔｈｅｓｔｒｕｃｔｕｒｅｏｆｌｏｎｇ ｒａｎｇｅｒａｎｄｏｍａｎｄｓｈｏｒｔ ｒａｎｇｅｏｒｄｅｒ .Ｃｏｍｐａｒｅｄｗｉｔｈｃｒｙｓｔａｌｌｉｎｅａｌｌｏｙ ,ｔｈｅｙｈａｖｅａｌｏｔｏｆ     

不同直径的Zr60.3Ni16.2Cu13.5Al10块体非晶合金的力学性能

采用铜模吸铸法制备了阶梯型的Zr60.3Ni16.2Cu13.5Al10非晶合金,利用X射线衍射(XRD)分别对直径为3 mm、4 mm、6 mm的合金试样进行结构分析,利用万能试验机及扫描电镜对试样进行压缩试验和断口形貌分析.研究表明,由于冷却速度的影响,直径为3 mm时是非晶结构,直径为4 mm和6 mm时是中心晶体和表面非晶体混合结构;对于Zr60.3 Ni16.2Cu13.5Al10合金,直径为3 mm时断裂强度可达到1 775 MPa,塑性变形可达到2.02%,而直径为4 mm的非晶复合材料的塑性变形可达2.93%,适当体积的晶体相的加入可以有效地提高非晶材料的塑性.     

Mg65Cu25Y10非晶态合金的形成及其晶化行为

采用水淬法制备出厚度为2mm的片状Mg65Cu25Y10非晶态合金,衡量其非晶成形能力的参数过冷液态区域宽度△Tx（△Tx=58.3K）、约化玻璃转变温度Trg（Trg=0.56）均较高,表明此合金具有很强的非晶形成能力;并测出了它的硬度为263.2HV.通过恒速升温和等温晶化试验,采用差热分析、X射线衍射等研究了它的热行为,结果表明,此合金在433K以下还是稳定的,如进一步升高温度,材料将由非晶态结构逐步向晶态结构转变,当退火温度达到623K时,则完全转变为晶态结构.     

Mg65Cu25Gd10非晶合金的腐蚀行为

采用电化学方法研究了块体Mg65Cu25Gd10非晶合金在0.01 mol/L,pH=13的NaCl溶液及0.1 mol/L,pH=13的NaOH溶液中的腐蚀行为.在2种电解质溶液中,非晶合金样品的极化曲线具有明显的钝化区和较低的钝化电流密度.浸蚀样品的表面形貌和腐蚀产物采用SEM和EDS来表征.恒电位钝化后样品表面层化学信息运用DP-XPS来考察.结果表明,样品在NaOH溶液中形成致密少孔的钝化膜,而在含Cl离子的溶液中,样品表面钝化膜疏松且多孔,导致合金在含Cl离子的溶液中具有较低的耐蚀性.     

非晶态Zr65Cu17.5Ni10Al7.5合金氧化和晶化过程研究

利用X射线衍射（XRD）和差示扫描量热法（DSC）研究了在连续加热条件下非晶态Zr65Cu17.5Ni10Al7.5合金在空气中的氧化和晶化过程。结果表明，在450℃以下，非晶态Zr65Cu17.5Ni10Al7.5合金表面的ZrO2晶粒长大过程服从抛物线规律；当温度超过450℃时，由于非晶基体内部发生晶化过程，阻碍了表面氧化过程的发展，此时ZrO2晶粒大小满足线性规律，并给出了ZrO2晶粒尺寸与温度的函数表达式。非晶态Zr65Cu17.5Ni10Al7.5合金的晶化过程是先形成二十面体相，然后转变为稳定的晶化相。     

Zr55Al10Ni5Cu30块体金属玻璃的摩擦焊焊接

采用摩擦焊对Zr55Al10Ni5Cu30块体金属玻璃进行了焊接,当焊机主轴转速为4.0×103-5.0×103 r/min,摩擦压力为80-100 MPa,摩擦时间为0.2-0.4 s,顶锻压力和保压时间分别为200 MPa和2 s时,能够成功实施Zr55Al10Ni5Cu30金属玻璃的焊接.用SEM,XRD和TEM观察分析未检测到晶化相,焊缝处金属仍保持非晶状态.金属玻璃的塑性在玻璃转变点Tg附近随温度变化很大,在Tg以上具有良好的塑性变形能力,这是实施摩擦焊焊接的重要基础.     

Zr55Al10Ni5Cu30合金熔体与金属W的润湿行为

用座滴法研究了Zr55Al10Ni5Cu30合金液滴与W基片在连续升温和不同温度下保温20min的润湿动力学。结果表明：箍着温度的升高，Zr55Al10Ni5Cu30与W基片的接触角不断减小，润湿半径不断增大，润湿过程大约在6min内完成．在连续升温过程中，润湿动力学分为孕育、准稳态和稳态三个阶段，在1173-1223K温度范围内等温润湿动力学分为准稳态和稳态两个阶段，Zr55Al10Ni5Cu30合金液滴与W之间的润湿为反应性润湿，在界面处发生了W的溶解和扩散现象，在制备Zr55Al10Ni5Cu30/W非晶复合材料时，必须合理选择制备工艺，严格控制界面反应。     

Ni元素对非晶合金Mg_(65)Cu_(25)Gd_(10)在NaCl溶液中腐蚀行为的影响

采用析氢腐蚀实验比较了非晶合金Mg65Cu25Gd10和Mg65Cu20Ni5Gd10在1%NaCl溶液中腐蚀性能。利用电化学测试技术和场发射扫描电子显微镜(FESEM)对两非晶合金在NaCl溶液中的腐蚀行为进行了研究。析氢腐蚀实验表明,Ni的加入大大提高了非晶合金Mg65Cu25Gd10抗蚀性能,极化曲线测试结果也表明Mg65Cu20Ni5Gd10非晶合金的腐蚀电流远远小于Mg65Cu25Gd10非晶合金。EIS测试表明,电化学阻抗谱测试结果显示Mg65Cu20Ni5Gd10非晶合金电荷转移电阻高于Mg65Cu25Gd10非晶合金。腐蚀产物形貌观察表明,Ni的加入使非晶合金Mg65Cu20Ni5Gd10腐蚀表面膜更为致密。结合各测试结果,探讨了Ni的加入提高镁基非晶合金耐蚀性机理。     

Applicability of Johnson-Mehl-Avrami model to crystallization kinetics of Zr60Al15Ni25 bulk amorphous alloy

The applicability of Johnson-Mehl-Avrami（JMA） model to the crystallization kinetics of Zr60Al15Ni25 bulk amorphous alloy is investigated by differential scanning calorimetry（DSC） under isochronal and isothermal conditions. A criterion Xm, at which a defined function z（x） exhibits the maximum value, is introduced to check the validity of JMA model to the kinetics analysis. The value Of Xm has a constant of 0.632 for JMA model. It is found that the values Of Xm at different isothermal annealing temperatures （743,748, 753 and 758 K） are almost near 0.632, which indicates that the isothermal crystallization kinetics can be modeled by JMA equation. However, the values Of Xm at different heating rates （10, 20, 30 and 40 K/min） are about 0.52, implying that JMA model is not valid to the isochronal crystallization kinetics. The reason why the JMA model is not valid to the isochronal crystallization kinetics is discussed.     

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。     

Mg_(65)Cu_(25)Y_(10)块体非晶合金的晶化组织(英文)

将普通铜模浇铸法制得的Mg65Cu25Y10块体非晶合金试样置于200°C进行保温处理,对处理后的试样的相组成和显微组织进行研究。XRD分析结果表明,该块体非晶的晶化随保温时间的延长趋于完全,在此过程中有Mg2Cu、Mg24Y5和HCP-Mg等晶体相析出。通过SEM观察到雪花状组织,EDS结果表明该雪花状组织的成分接近于铸态合金的成分,TEM分析表明其为层片状结构。电子衍射花样分析表明,雪花状组织由Mg24Y5晶体和非晶相组成。在保温过程中,基体中的FCC-Mg会转变为HCP-Mg。     

块体非晶合金(La0.6Ce0.4)65Al10Cu25晶化行为的研究

利用铜模铸造法制备(La0.6Ce0.4)65Al10Cu25块体非晶合金,通过X射线衍射和差示扫描量热法对该非晶合金的热稳定性和晶化行为进行研究。利用J-M-A方程对其等温晶化动力学进行分析,该合金平均Avrami指数在2.39～3.38之间。区域Avrami指数n(x)分析表明,晶化初期n(x)趋于3;晶化中期阶段,n(x)由2.5变化到3.5,在此过程中,当2.5相似文献   

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.