Ti40Zr25Ni8Cu9Be18非晶合金的晶化行为研究

采用吸铸法制备出直径3mm的Ti40Zr25Ni8Cu9Be18块体非晶合金，并采用X射线衍射（XRD）、差示扫描量热（DSC）和透射电镜（TEM）研究了非晶合金试样的结构，同时，分别采用连续升温晶化方法和等温退火方法研究了该非晶合金的晶化动力学行为和晶化过程中的相转变。结果表明：该非晶合金的结构弛豫和晶化行为均具有显著的动力学特征，且具有较好的热稳定性，其过冷液相区宽度△Tx为54K，一级晶化激活能Ep1为213．04kJ／mol；晶化过程为二级晶化反应，第1阶段晶化对应I相从非晶基体中析出，第2阶段的晶化反应则包括：I相转变为Laves相和Laves相从残余非晶基体中直接析出。     

Zr41.2Ti13.8Cu12.5Ni10Be22.5合金凝固过程热力学

利用真空冷壁坩埚感应熔炼及铜模离心铸造的方法制备了大尺寸非晶态Zr41．2Til3．8Cul2．5Ni10Be22．5材料，采用DTA和DSC分别研究了该合金的凝固特性及非晶态晶化行为。结果表明：Zr41．2Til3．8Cul2．5Ni10Be22．5合金具有较低的熔点，表现出良好的深共晶特性，在较低的冷却速度下即可制备出大块部分非晶及全部非晶材料。Zr41．2Til3．8Cul2．5Ni10Be22．5大块非晶材料在339．5℃发生玻璃转变，晶化温度为420℃。     

Zr52.5Ni14.6Al10Cu17.9Ti5块体玻璃合金等温晶化与结构转变

对采用射流成形方法制备了Ｚｒ５２．５Ｎｉ１４．６Ａｌ１０Ｃｕ１７．９Ｔｉ５块体玻璃合金进行等温退火,利用Ｘ射线衍射和ＳＥＭ及ＴＥＭ分析了块状玻璃态合金等温晶化时相转变及组织转变。     

氧含量对Ni47Ti44Nb9合金组织和相变行为的影响

研究了氧含量对Ni47Ti44Nb9合金显微组织和相变行为的影响.结果表明,当氧含量超过固溶度后,氧存在于(Ti,Nb)4Ni2O氧化物中.随着氧含量的增加相变温度降低,应力诱发马氏体相变的临界应力提高,相变热滞变宽.氧含量(质量分数)在0.04%-0.07%范围内,Ni47Ti44Nb9合金具有最大的形状记忆应变和延伸率.     

（Ni0.75Fe0.25）78Si10B12非晶合金非等温晶化动力学效应

采用旋铸急冷工艺在大气环境中制备出了（Ni0.75Fe0.25）78Si10B12非晶合金带材。X射线衍射（XRD）分析表明样品为完全非晶。用Diamond TG／DTA差热分析仪在高纯氩气保护下测量了非晶薄带的热稳定性参数Tg，Txi，Tpi并分析其晶化行为，加热速度分别为10K／min，20K／min，30K／min，40K／min。（Ni0.75Fe0.25）78Si10B12非晶合金的Tg，Txi，Tpi均随加热速率的增加而增加，说明其玻璃转变和晶化行为均有动力学效应。分别用Kissinger法和Ozawa法计算该非晶合金的晶化激活能，2种方法的计算结果是一致的。对试样在通高纯氩气保护下，进行等温（695K，715K，745K，765K，保温60min）退火处理，利用XRD分析了非晶合金等温晶化时相转变及组织转变。合金在715K和745K温度退火时，在非晶基体上析出了单一的γ-（Fe，Ni）固溶体，平均晶粒尺寸分别约为10.3nm和18．5nm，765K退火处理后的结晶相为γ-（Fe，Ni），Fe2Si，Ni2Si和Fe3B，平均晶粒尺寸约29．6nm。     

Ti3Al—19Nb合金的显微组织和结构研究

用透射电镜研究了Ti_3Al-19Nb合金在不同热处理状态下的组织结构及其变化规律。从β相区冷却后,随冷却速度不同可分别得到全部或主要为B2,B2+α_2或α_2相的组织。油淬样品在时效过程中α_2相晶粒及其反相畴尺寸均逐渐变大。     

Ti45Zr35Cu5Ni15块体非晶合金动态压缩性能研究

通过铜模喷铸法制备了含有少量纳米晶的Ti45Zr35Cu5Ni15大块非晶合金.利用分离式霍普金森杆(SHPB)分别对试样进行室温(25℃)、-80℃和液氮温度(-196℃)3种不同温度环境下的高应变率加载动态压缩实验,结合带有能谱的场发射扫描电镜(SEM)观察材料压缩断口的形貌特征.对比分析发现:材料在-80℃下的动...     

纳米Ti（CN）基金属陶瓷烧结过程中的结构和相变

用分段真空烧结、X射线衍射和背散射扫描电镜研究了纳米Ti（CN）基金属陶瓷在烧结过程中的结构和相成分的演变。结果表明：纳米Ti（CN）基金属陶瓷在900℃以后，Mo2C和TaC开始由于扩散，与Ti（CN）发生固溶反应，在1200℃以前，Mo2C和TaC固溶反应结束，两相均消失。WC在1100℃以后，开始由于扩散，与Ti（CN）发生固溶反应，在1250℃以前消失。在1250℃以后，合金中只有Ti（CN）和Ni（Ni＋Co）两相存在。纳米Ti（CN）粉末与M（M=Mo，W．Ta）反应形成富M的（Ti，M）（CN）固溶体为核，贫M的（Ti，M）（CN）固溶体为环的“亮芯黑环”环形结构，在1350℃即可获得致密的合金。     

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。     

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。     

Structural transformation and rheological processes in bulk metallic glass Zr41Ti14Cu12.5 Ni10Be22.5

The temperature dependence of strain and strain rate of the Zr41Ti14Cu12.5Ni10Be22.5 (Vitl) bulk metallic glass (BMG) under constant heating condition was derived from the static extension method with a dynamic thermal mechanical analyzer (DMA). A few strain rate peaks, which corresponds to the glass transition and multistep crystallization in the differential scanning calorimeter (DSC) examination, were observed in the curves of the relation between strain rate and temperature. The onset of viscous flow and the end of glass transition are interrelated, the first and second strain rate peaks correspond with the first and second crystallization transition processes, respectively.The influence of stress on strain and strain rate was researched. It is found that the rheological behaviour of BMG Vitl changes from elasticity to anelasticity, finally to the Newtonian viscous flow along with increasing temperature.     

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

1　ＩＮＴＲＯＤＵＣＴＩＯＮＴｈｅｍｅｔａｌｌｉｃｇｌａｓｓｅｓｈａｖｅｔｈｅｓｔｒｕｃｔｕｒｅｏｆｌｏｎｇ ｒａｎｇｅｒａｎｄｏｍａｎｄｓｈｏｒｔ ｒａｎｇｅｏｒｄｅｒ .Ｃｏｍｐａｒｅｄｗｉｔｈｃｒｙｓｔａｌｌｉｎｅａｌｌｏｙ ,ｔｈｅｙｈａｖｅａｌｏｔｏｆ     

高能球磨工艺对Ti50Ni22Cu25Sn3组织演变的影响

用高能球磨法制备Ti50Ni22Cu25Sn3非晶粉末,并研究球磨工艺参数对Ti50Ni22Cu25Sn3非晶形成过程的影响。结果表明,球磨转速以及磨球直径对Ti50Ni22Cu25Sn3非晶相的形成效率具有十分重要的影响。较高的转速和合适的球径能有效促进该Ti基合金的非晶化,缩短合金非晶化的时间,当转速为400 r/min,球料比为20:1时,球磨时间约为30 h后,可得到完全的Ti50Ni22Cu25Sn3非晶粉末     

Enhanced microhardness in nanocomposite Ti60Cu14Ni12Sn4Ta10 processed by high pressure torsion

Nanostructured Ti₆₀Cu₁₄Ni₁₂Sn₄Ta₁₀ alloys have been obtained by (i) arc-melting (AM) the pure elements and (ii) AM followed by severe plastic deformation induced by high pressure torsion (HPT). Scanning electron microscopy (SEM) reveals that the AM specimen consists of a dendrite–eutectic structure. After the HPT, the center of the disks exhibits a microstructure similar to the AM specimen but with strongly deformed dendrites and the lamellae become refined and intermixed as the distance from the disk center increases. At the edge of the HPT disks the dendritic/eutectic morphology is no longer observed by SEM. The Vickers microhardness is higher in the HPT disks as compared to the AM samples. This result is discussed in terms of the peculiar morphologies and nanostructures achieved after each processing route.     

含Al双相钢相变行为及退火温度对力学性能的影响

利用Formastor热膨胀仪测试了一种含Al中硅中锰双相钢的连续冷却过程的相变行为,采用连续退火热模拟试验机进行了连续退火试验,测试了力学性能,观察了微观组织。结果表明,试验钢以10℃/s的加热速率加热过程中,Ac1和Ac3分别为713 ℃和918℃,与热力学平衡状态相比,分别需要29 ℃和58 ℃的过热度;连续冷却过程中,发生铁素体相变的临界冷速为3~5 ℃/s之间,贝氏体相变的临界冷速为15~30 ℃/s;连续退火过程中,随淬火温度的提高,抗拉强度呈逐渐升高的趋势,而伸长率呈逐渐降低的趋势,应变硬化指数n值对淬火温度不敏感。     

Formation and properties of Zr48Nb8Cu14Ni12Be18 bulk metallic glass

Zr₄₈Nb₈Cu₁₄Ni₁₂Be₁₈ bulk metallic glass (BMG) with excellent glass-forming ability was prepared by water quenching method. The BMG exhibits high glass transition temperature T_g and onset crystallization temperature T_x, compared with Zr₄₁Ti₁₄Cu_12.5Ni₁₀Be_22.5 BMG. The crystallization processes, change of elastic constants, and density and hardness in the crystallization process were studied by using X-ray diffraction, differential scanning calorimetry and acoustic method. The shear modulus, Poisson ratio, density and hardness are found to be sensitive to the crystallization process. A striking softening of long-wavelength transverse acoustic phonons in the BMG relative to its crystallized state is observed. The linear expansion coefficient, determined by a dilatometer method, is α_TG=1.04×10⁻⁵ K⁻¹ (300–656 K) for the BMG and α_TC=1.11×10⁻⁵ K⁻¹ (356–890 K) for the crystalline alloy. The Mie potential function and the equation of state of the BMG are determined from the expansion coefficient and acoustic experiments.     

Transformation behaviors of Ti48.5Ni48Fe2Nb1.5 dependence of annealing and thermomechanical cycling

The effect of annealing treatments and thermomechanical cycling on the transformation behaviors and shape memory effect of Ti48.5Ni48Fe2Nb1.5 shape memory alloys were investigated using electrical resistivity measurement and tensile testing. It is found that the transformation behaviors are influenced considerably by the annealing treatments. Both Ms and As increase with increasing annealing temperature and cooling rate. Martensite stabilization occurs during thermomechanical cycles, thus resulting in lower...     

Rheological and diffusion behaviours of Zr41Ti14Cu12.5Ni10Be22.5 bulk metallic glass around glass transition

1 Introduction Since the Au-Si metallic glass were firstly prepared by rapid cooling technique in 1960 by DUWEZ et al[1], the study of structure and property of metallic glass has received much attention. The atom transportation behaviors (rheological an…     

不同熔体温度制备的Zr55Al10Ni5Cu30大块非晶结构弛豫

在不同喷铸温度下制备了Zr55Al10Ni5Cu30块体非晶试样,利用电阻率法研究熔体温度对非晶结构弛豫的影响.结果表明,缺陷散射对电阻率的影响高于电子声子散射的影响;低温结构弛豫时,在1300℃时制备的试样保温前后电阻率的差值出现负值;高温结构弛豫后,随着制备非晶时熔体温度的升高,保温前后电阻率的差值逐渐减小.