高温形变对FeCoCrMoYCB块体非晶结构和热稳定性的影响

采用水冷铜模吸铸法制备直径为4 mm的Fe_(41)Co_7Cr_(15)Mo_(14)Y_2C_(15)B_6块体非晶合金,利用X射线衍射(XRD)和差式扫描量热分析仪(DSC)分别对该非晶的结构及热力学参数进行表征。利用Gleeble 3500热模拟机在过冷液相区温度620℃下,以1×10~(-2)s~(-1)的应变速率对该非晶合金进行压缩变形,研究变形量(20%、40%和75%)对该非晶合金结构和热稳定性的影响。结果表明,该条件下非晶试样能发生较好的塑性变形并未发现明显的晶化,且随着塑性变形的增加,非晶合金的热稳定性更加优异,当形变量为75%时,非晶合金的玻璃转变温度和过冷液相区宽度分别从铸态的585℃和40℃增大至658℃和59℃。变形影响非晶试样的显微硬度,宏观表现为应变量越大其显微硬度越高,当塑性形变量为20%、40%及75%时,对应最高维氏硬度分别为1258,1270和1288 HV。     

铁基块体非晶合金的制备及其晶化动力学

采用工业用原材料在铜模吸铸条件下制备了直径为2 mm的Fe50Co7Ni13Zr10B20块体非晶合金.利用X射线衍射仪(XRD)、差分扫描量热计(DSC)对铸态样品的结构、非晶合金的热稳定性、晶化动力学行为进行了研究.该合金的玻璃转变温度Tg、初始晶化温度Tx1、过冷液相区△Tx1约化玻璃转变温度Trg分别为804 K、875 K、71 K和0.59.采用连续加热方法对其晶化动力学进行了研究,得到其玻璃转变激活能和晶化峰激活能分别为339.2 kJ/mol和326.4 kJ/mol,表明合金具有强的热稳定性.由VFT方程拟合获得该非晶合金的脆性参数m为23.     

Zr基非晶合金在过冷液相区的拉伸变形行为

采用ARAMIS三维变形分析测试系统对Zr65Cu20Al10Fe5块体非晶合金在400℃和应变速率为1×10-3s-1条件下的高温拉伸变形行为进行研究,并利用X射线衍射(XRD)对合金试样的显微组织进行分析。结果表明,在变形条件下,该Zr-基非晶合金可表现出良好的塑性,其伸长率为103%,其变形模式为非牛顿流变。用三维变形分析得到的不同变形时刻的应变分布图显示,随着变形量的增加,试样变形变得不均匀,在变形后期会出现颈缩现象。XRD分析结果表明,在拉伸变形过程中,非晶合金试样会发生晶化,其晶化程度与试样不同部位的局部应变量大小有关,局部变形量较大的区域晶化程度较高,而较高含量纳米晶的存在导致了该区域具有较高的变形速率。     

高温变形对(Cu50Zr50)92Al8等温晶化行为及其力学性能的影响

研究了(Cu50Zr50)92Al8非晶合金在过冷液相区中,经过牛顿流变和非牛顿流变后的等温晶化行为及其对该合金力学性能的影响。结果表明,牛顿型流变对(Cu50Zr50)92Al8非晶合金的结构没有明显的影响;而非牛顿流变对该非晶的显微结构及其等温晶化行为有显著影响:非牛顿流变促进了(Cu50Zr50)92Al8非晶合金的晶化,其主要晶化相为体心立方结构的CuZr相(B2相)和CuZr马氏体相;经非牛顿流变及真空热处理试样,在室温压缩过程中,应力诱发了部分B2相的马氏体相变,从而使其在室温下表现出超弹性,当预塑性应变量为8%时,其总可回复应变为5%左右。     

Si对Ni基非晶合金玻璃形成能力及热稳定性的影响

研究Si对NiCuTiZrAl非晶合金的玻璃形成能力及热稳定性的影响。利用铜模铸造制备NiCuTiZrAlSi非晶合金,3.5%Si的添加显著改善非晶合金的玻璃形成能力。在DSC、DTA、XRD及TEM分析的基础上,利用SEM(EDS)技术对类金属Si提高非晶合金的玻璃形成能力及热稳定性进行深入分析。适量元素Si添加不仅可以延缓熔体中初生相Ni(TiZr)和(TiZr)(CuAl)2形成,而且可抑制元素O的有害作用,这为类金属提高非晶合金的玻璃形成能力提供有效证据。利用Kissinger方程进行不同含Si量的NiCuTiZrAl非晶合金晶化动力学研究表明,放热峰Tp处晶化激活能随着Si量增加而增大。     

加压退火对 (La0.6Ce0.4)65Al10Cu25块体非晶合金晶化行为和热稳定性的影响

利用铜模铸造法制备了(La0.6Ce0.4)65Al10Cu25块体非晶合金,并在其过冷液相区内不同温度下,采用不同压力对该非晶合金进行加压退火处理,通过X射线衍射仪和差示扫描量热法研究了加压退火处理对该非晶合金晶化行为及热稳定性的影响。结果表明,加压退火促进了(La0.6Ce0.4)65Al10Cu25非晶合金的晶化过程,使得晶化初始温度Tx降低(dTx/dP=-5.17K/GPa),晶化激活能Ep随退火压力的增加而增大,并从能量和化学短程序畴的角度解释了加压退火对(La0.6Ce0.4)65Al10Cu25非晶合金晶化过程的影响机理。     

W17.9Ni65.6B13.5V3非晶合金的非等温晶化动力学研究

采用单辊急冷法制备了W17.9Ni65.6B13.5V3非晶薄带,并用X射线衍射(XRD)和示差扫描量热分析仪(DSC)研究了该非晶合金的变温晶化动力学。结果表明：玻璃转变温度Tg、晶化起始温度Tx和晶化峰值温度Tp均随着升温速率的增加而提高,具有明显的动力学效应;利用Kissinger方程和Ozawa方程求出的W17.9Ni65.6B13.5V3非晶合金的晶化激活能Ex分别达456.9kJ/mol和471.1kJ/mol,非晶合金具有较强的热稳定性;利用Kissinger方程和Ozawa方程计算得到的晶化激活能Ex均小于晶体长大激活能Ep,表明形核过程比晶粒长大过程更容易,该非晶合金在一定条件下退火容易获得超细晶粒组织。     

W_(17.9)Ni_(65.6)B_(13.5)V_3非晶合金的非等温晶化动力学

采用单辊急冷法制备了W_(17.9)Ni_(65.6)B_(13.5)V_3(at%)非晶薄带,并用X射线衍射(XRD)和示差扫描量热分析仪(DSC)研究了该非晶合金的变温晶化动力学。结果表明:玻璃转变温度Tg、晶化起始温度Tx和晶化峰值温度Tp均随着升温速率的增加而提高,具有明显的动力学效应;利用Kissinger方程和Ozawa方程求出的W_(17.9)Ni_(65.6)B_(13.5)V_3非晶合金的晶化激活能Ex分别达456.9和471.1 kJ/mol,表明非晶合金具有较强的热稳定性;该晶化激活能Ex均小于晶体长大激活能Ep,表明形核过程比晶粒长大过程更容易,该非晶合金在一定条件下退火容易获得超细晶粒组织。     

Cu_(46)Zr_(47-x)Al_7Ti_x(x=0,1.5)非晶合金晶化动力学研究

采用铜模吸铸法制备Cu46Zr47-xA l7Tix(x=0,1.5)大块非晶合金。用X射线衍射仪(XRD)确定合金的结构,采用差示扫描量热仪(DSC)对非晶合金的晶化动力学进行了研究。结果显示,随着升温速率的加快,这两种非晶合金的玻璃转变温度Tg,晶化开始温度Tx和晶化峰值温度Tp均向高温区移动,且过冷液相区逐渐加宽,表明非晶合金的玻璃化转变和晶化均具有动力学效应。利用K issinger方程计算合金的晶化激活能。通过晶化动力学研究了热稳定性和晶化反应速率常数之间的关系,以及Ti元素添加对Cu-Zr-A l大块非晶合金热稳定性的影响。     

镍基块状非晶合金的晶化动力学行为

利用铜模铸造方法制备了Ni45 Ti23Zr15Si5Pd12块状非晶合金，采用扫描差热分析(DSC)和X射线衍射(XRD)对该块状非晶合金的晶化动力学行为进行了研究．结果表明：Ni45Ti23Zr15Si5Pd12块状非晶样品的晶化过程为多阶段晶化，主要晶化过程的Avrami指数大于3．0，为三维形核长大过程；随着晶化体积分数的增加，剩余非晶的晶化激活能增大，合金热稳定性增加；原子尺寸差异以及各原子间大的负混合焓是合金具有高的热稳定性的主要原因．     

Cu44.25Ag14.75Zr36Ti5非晶合金的晶化行为

采用铜模铸造法制备了直径为3mm的柱状Cu44.25Ag14.75Zr36Ti5块体非晶合金,X射线衍射证明试样为完全非晶态。利用差示扫描热分析仪(DSC)、X射线衍射,研究了该非晶合金的晶化行为。利用Kissinger和Ozawa方程求得Cu44.25Ag14.75Zr36Ti5第一晶化峰和第二晶化峰的晶化激活能。结果表明,该大块非晶合金具有良好的热稳定性,在10K/min的加热速率下,析出相主要是Cu8Zr3和Cu10Zr7。     

Zr50Ti5Cu18Ni17Al10块体金属玻璃的热稳定性和力学性能

采用差示扫描量热仪以连续加热的方式研究了Zr50Ti5Cu18Ni17Al10块体金属玻璃的热稳定性。其玻璃转变激活能(Eg)以及晶化激活能(Ep1和Ep2)分别为438±11,284±8和323±11kJ/mol。采用压缩试验研究了金属玻璃的室温力学性能,初始应变速率为1×10-4s-1。直径为3mm的金属玻璃棒呈现良好的力学性能,最大塑性应变达3%,杨氏模量和断裂强度的最大值分别为90GPa和1968MPa。多条剪切带的交织、分叉和滑移以及宽度为60?m的较大临界剪切台阶是Zr50Ti5Cu18Ni17Al10块体金属玻璃具有较高压缩塑性的主要原因。     

Crystallization behavior of Ti61.67Zr17.15Ni14.80Cu6.38 glass-forming alloy

Ti61.57Zr17.15Ni14.80Cu6.38(atom fraction, %) metallic glass has applications in brazing. Using the hammer-and-anvil technique, Ti61.67Zr17.15Ni14.80Cu6.38 metallic glass was prepared. The crystallization behavior for this metallic glass was investigated by differential scanning calorimetry(DSC), X-ray diffractometry (XRD) and transmission electron microscopy(TEM). There are three stages in DSC curves of crystallization. The reduced glass temperature Trg is 0.42. The kinetic parameters of crystallization were calculated by a set of equations of the maximum crystallization rate. The crystalline phase formed in the MSⅠ(Metastable stage D is Zr2Cu, in the MSII is α-Ti and in the MSⅢ is Ti2Ni. This kind of alloy has lower glass forming ability, and the Ti61.67Zr17.15Ni14.80Cu6.38 metallic glass has lower thermal stability.     

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。     

ZrCuAlSi大块非晶合金变温晶化行为

利用铜模吸铸法制备Zr46.3Cu43.3Al8.9Si1.5(at%)大块非晶合金,利用示差扫描量热(DSC)仪研究合金连续升温过程中的晶化行为,利用Kissinger方法计算其特征温度表观激活能,利用Doyle方法计算其局域激活能。结果表明,Zr46.3Cu43.3Al8.9Si1.5大块非晶合金具有良好的热稳定性。利用Kissinger方法计算得到其玻璃转变激活能Eg为395.4kJ/mol、晶化起始激活能Ex为343.2kJ/mol、晶化峰的激活能Ep为343.0kJ/mol。Doyle方法计算其局域激活能表明,其晶化过程中,激活能明显越过一能量势垒后,再呈现逐渐减小的趋势。     

Cu50 Zr42 Al8块体金属玻璃的组织和力学性能

采用悬浮熔炼-铜模吸铸法制备了Cu50Zr42Al8块体金属玻璃,研究了其楔形试样的组织演变.随着熔体凝固过程中冷却速度的变化,楔形试样中存在表面全非晶区,中心晶体区以及二者之间的过渡区域,并确定Cu50Zr42Al8块体金属玻璃临界尺寸为4.8 mm.分别考察了φ4 mm铸态完全非晶棒和φ5 mm非晶复合棒的力学性能.φ4 mm非晶棒的压缩断裂强度,弹性应变和塑性应变分别为2260 MPa,2.0%,0.4%,几乎没有塑性变形.而φ5 mm铸态非晶复合棒的屈服强度、断裂强度分别为1670MPa、1849 MPa,弹性应变和塑性应变分别为1.6%和1.9%.非晶基体中存在的马氏体相CuZr和正交晶相Cu10Zr7的竞争影响了非晶复合棒的最终力学行为.     

A Dy-based bulk metallic glass with high thermal stability and excellent magnetocaloric properties

A new heavy rare-earth-based Dy₃₆Ho₂₀Al₂₄Co₂₀ bulk metallic glass (BMG) with high thermal stability and excellent magnetocaloric properties has been prepared by a copper mold casting. Compared with the other known rare-earth-based BMGs, this BMG alloy possess higher glass transition temperature and crystallization temperature, larger effective activation energy for glass transition and crystallization. Under a modest magnetic field, this BMG alloy exhibits a comparable or even larger magnetocaloric effect than that the previously reported RE-based BMGs and crystalline compounds. The high thermal stability and the excellent magnetocaloric effect together with other merits of the BMGs make this BMG alloy suitable candidate for use as magnetic refrigerant in a temperature range below 50 K.     

Preparation, thermal stability, and magnetic properties of Fe---Co---Zr---Mo---W---B bulk metallic glass

A bulk metallic glass (BMG) cylinder of Fe₆₀Co₈Zr₁₀Mo₅W₂B₁₅ with a diameter of 1.5 mm was prepared by copper mould casting of industrial raw materials. The amorphous state and the crystallization behavior were investigated by X-ray diffraction (XRD). The thermal stability parameters, such as glass transition temperature (T_g), crystallization temperature (T_x), supercooled liquid region (ΔT_x) between T_g and T_x, and reduced glass transition temperature T_rg (T_g/T_m) were measured by differential scanning calorimetry (DSC) to be 891, 950, 59 K, and 0.62, respectively. The crystallization process took place through a single stage, and involved crystallization of the phases -Fe, ZrFe₂, Fe₃B, MoB₂, Mo₂FeB₂, and an unknown phase, as determined by X-ray analysis of the sample annealed for 1.5 ks at 1023 K, 50 K above the DSC peak temperature of crystallization. Mössbauer spectroscopy was studied for this alloy. The spectra exhibit a broadened and asymmetric doublet-like structure that indicated paramagnetic behavior and a fully amorphous structure. -Fe was found in the amorphous matrix for a cylinder with a diameter of 2.5 mm. The success of synthesis of the Fe-based bulk metallic glass from industrial materials is important for the future progress in research and practical application of new bulk metallic glasses.     

High Temperature Deformation Behavior of High Strength and Toughness Ti-Ni Base Bulk Metallic Glass CompositesEI北大核心CSCD

Room-temperature brittleness and strain-softening during deformation of bulk metallic glasses, and limited processability of shape memory alloys have been stumbling blocks for their advanced functional structural applications. To solve the key scientific problems, a new shape memory bulk metallic glass based composite, through the approach using transformation-induced plasticity (TRIP) effect of shape memory alloys to enhance both ductility and work-hardening capability of metallic glasses, and superplasticity of bulk metallic glass in supercooled liquid region to realize near net forming, was developed in this work. And the Ti-Ni base bulk metallic glass composites (BMGCs) rods were prepared by the levitation suspend melting-water cooled Cu mold process. Microstructure, thermal behavior, mechanical properties and high temperature deformation behavior of the alloy were investigated. The results show that the as-cast alloy microstructure consists of amorphous matrix, undercooled austenite and thermally-induced martensite. Besides, the size of the crystal phase precipitated on the amorphous matrix in-creases from the surface to the inside. The alloy exhibits excellent comprehensive mechanical properties at room temperature. The yield strength, fracture strength and the plastic strain of alloy are up to 1286 MPa, 2256 MPa and 12.2%, respectively. Under compressive loading in the supercooled liquid region, the composite exhibits approximate Newtonian behavior at lower strain rate in higher deformation temperature, and the optimum deformation temperature is T>480 degrees C and the intersection part with supercooled liquid region (SLR). When the temperature is 560 degrees C and the strain rate is 5x10(-4) s(-1), the stress sensitivity index m and the energy dissipation rate Psi are 0.81 and 0.895, respectively. Furthermore, the volume of activation is quantified to characterize the rheological behavior.     

微量添加Fe元素对CuZrAl块体金属玻璃的结构和力学性能的影响(英文)

使用水淬法制备含微量Fe元素的CuZrAl块体金属玻璃。使用X射线衍射(XRD)检测其结构;采用DSC研究Fe元素的添加对块体金属玻璃热稳定性的影响,微量添加Fe元素显著拓宽了过冷液相区。Cu44Zr48Al7Fe块体金属玻璃的塑性应变约为1.5%。使用透射电子显微镜(TEM)观察其微观结构,结果发现,添加1%～2%Fe(摩尔分数)的CuZrAl合金中出现了相分离的富CuZr非晶相。