（Ti，Zr，Hf）一（Cu，Ni，Ag）—Al多组元合金体系的机械驱动非晶化

研究了由前过渡族金属和后过渡族金属按照等原子比替代的(Ti0.33Zr0.33Hf0.33)50(Ni0.33Cu0.33Ag0.33)40Al10多组元合金在机械研磨作用下的非晶化转变，并与由熔体急冷制备的同一成分玻璃态合金进行了对比．两种途径获得的玻璃态相似．在机械研磨的稳态产物中，仍残留有少量尺寸小于30nm的晶体相颗粒，即非晶化转变未能完全实现．机械研磨形成的非晶相表现有明确的玻璃转变和约80K宽的过冷液态温度区间，晶化过程分两步进行，第一步晶化转变完成后，剩余的非晶相亦具有玻璃态行为，呈现另一玻璃转变及约100K宽的过冷液态温度区间．     

Formation of W Particles /La55Al25Cu10Ni5Co5 Glassy Alloy Matrix Composites By Mechanical Milling

利用X射线衍射、透射电子显微镜和差示扫描量热计分析表征了La55Al25Cu10Ni5Co5合金及其添加W颗粒后高能球磨产物的结构与相转变. 由数个金属间化合物构成的La55Al25Cu10Ni5Co5合金经过机械研磨可转变为与熔体过冷形成的金属玻璃相类似的 玻璃态合金, 过冷液态温度区间的宽度可达到76 K. 合金与W颗粒(体积分数10%---30%)的混和物机械研磨后, 形成W纳米颗粒弥散分布于La基玻璃态合金基体上的复合材料. 随着W含量的增加, 基体合金的玻璃转变温度和晶化起始温度均提高.     

机械研磨形成W颗粒/La55Al25Cu10Ni5Co5 金属玻璃基复合材料

利用X射线衍射、透射电子显微镜和差示扫描量热计分析表征了La55Al25Cu10Ni5Co5合金及其添加W颗粒后高能球磨产物的结构与相转变.由数个金属间化合物构成的La55Al25Cu10Ni5Co5合金经过机械研磨可转变为与熔体过冷形成的金属玻璃相类似的玻璃态合金,过冷液态温度区间的宽度△Tx可达到76 K.合金与W颗粒(体积分数10%-30%)的混和物机械研磨后,形成W纳米颗粒弥散分布于La基玻璃态合金基体上的复合材料.随着W含量的增加,基体合金的玻璃转变温度Tg和晶化起始温度Tx1均提高,同时△Tx增大,含30%W的复合材料,基体玻璃态合金的△Tx可达到92 K.     

机械研磨形成W颗粒／La55A125Cu10Ni5Co5金属玻璃基复合材料

摘要利用X射线衍射，透射电子显微镜和差示扫描量热计分析表征了La55A125Cu10Ni5Co5合金及其添加W颗粒后高能球磨产物的结构与相转变,由数个金属间化合物构成的La55A125Cu10Ni5Co5合金经过机械研磨可转变为与熔体过冷形成的金属玻璃相类似的玻璃态合金，过冷液态温度区间的宽度△Tx可达到76K．合金与W颗粒(体积分数10％—30％)的混和物机械研磨后，形成W纳米颗粒弥散分布于La基玻璃态合金基体上的复合材料,随着W含量的增加，基体合金的玻璃转变温度Tg和晶化起始温度Tx1均提高，同时△Tx增大，含30％W的复合材料，基体玻璃态合金的△Tx可达到92K。     

Sn替代Si和B对Ti50Ni22Cu18Al4Si4B2合金机械研磨非晶化的促进作用

采用Xn替代Ti50Ni22Cu18Al4Si4B2合金中的Si和B1形成Ti50Ni22Cu18Al4Snx(Si0．67B0．33)6-x(x=0，3，6)系列合金．所有的预制合金碎屑经过机械研磨均发生非晶化转变．随着合金中Sn含量的增加，球磨产物中转变未尽的晶体相α-Ti含量减少．由Sn完全替代Si和B的Ti50Ni22Cu18Al4Sn6合金，机械研磨可形成与熔体急冷几乎相同的单一均匀非晶相，过冷液态温度区间可达到66K．     

Mg_(80)Cu_(15)Y_5合金的非晶形成能力及晶化行为

采用单辊快速凝同法制备出厚约40μm的Mg_(80)Cu_(15)Y_5非品合金薄带,利用XRD、DSC、TEM和HRTEM研究了非品合金的非品形成能力和晶化行为,分析了品化对合金组织结构与性能的影响.结果表明:Mg_(80)Cu_(15)Y_5合金的过冷液态温度区间△T_x和约化玻璃转变温度T_(rg)分别为55K和0.58,表明其具有较强的非晶形成能力;该合金在退火温度高于473 K后发牛明显晶化,从非品基体中析出 Mg_2Cu、Cu_2Y和Mg晶体相;随着退火温度的升高,合金的硬度呈现出先升高后降低的变化趋势,这与纳米品体相颗粒的弥散析出、重溶及粗化有关.     

Fe55Ni2Cr12Mo10Y2B6C13块体非晶合金的热膨胀行为

本文采用铜模吸铸法制备直径为4mm的块体非晶合金Fe55 Ni2 Cr12 M010 Yo12 B6 C13,对非晶合金在298K-1073K温度区间的热膨胀行为进行了分析.非晶合金的膨胀系数在室温至接近玻璃转化温度区间没有发生明显的变化;当温度超过Tg后,由玻璃态进人过冷液相区,粘度急剧增加,膨胀系数增高;在T>Tg...     

Pd_(77.5)Cu_6Si_(16.5)块体非晶合金的制备与热稳定性

采用玻璃包覆净化方法和水淬法,制备出了尺寸达7mm的Pd77.5Cu6Si16.5块体非晶合金样品。热分析结果表明,与熔体旋淬甩带法制备的Pd77.5Cu6Si16.5非晶条带样品相比,所制备的Pd77.5Cu6Si16.5块体非晶合金样品具有更低的玻璃转变温Tg、更高的初始晶化温度Tx和更宽的过冷液相温度区间ΔT(ΔT=Tx-Tg)。研究结果表明,采用玻璃包覆净化法有效去除了Pd77.5Cu6Si16.5合金熔体中的异质核心,显著提高了该合金熔体的稳定性和所制备的Pd77.5Cu6Si16.5块体非晶合金的热稳定性,提高了该合金的非晶形成能力。     

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。     

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.     

Ti-(Cu,Ni)-Sn合金形成金属玻璃的成分优化及其相关联的共晶反应

采用“3D法”, 系统地研究了Ti-(Cu1-xNix)-Sn(0.20≤x≤0.30, 原子分数, 下同) 四元合金的玻璃 形成能力对成分变化的依赖性. 确定玻璃形成能力最佳的合金为Ti38Cu37.8Ni16.2Sn8,Cu模吸铸形成金属玻璃 棒材的临界直径接近1 mm.该金属玻璃的过冷液态温度区间宽度ΔTx为56 K, 约化玻璃转变温度T rg为0.57. 对电弧熔炼Ti38Cu37.8Ni16.2Sn8合金微观结构的研究表明,合金熔体的凝固主要经历伪二元共晶反应:L→ Ti5Sn3Cu+TiCuNi.     

Nanostructured bulk glassy Cu_(60)Zr_(30)Ti_(10) alloy with high strength and good ductility in cast state

1　INTRODUCTIONSinceaseriesofmetallicbulkglassyalloyswithexpectedmechanicalpropertiesandhighglassformingabilityhavebeenfound[13] ,particularattemptshavebeendonetoimprovethemechanicalpropertiesoftheglassyalloystomeetengineeringapplications .Bycrystallizingthemetallicglasses ,nanostructuredal loyscontainingnanocrystallinephasesandglassyma trixwereobtainedandthemechanicalpropertiesofthealloyswereenhancedbyhomogeneousdispersionofnanoscalemetallic particlesintheAl [4 ,5] ,Fe Ni [6 ] andMg [7]…     

Glass-forming ability and magnetic properties of mechanically solid-state reacted Co100−xTix alloy powders

A high-energy ball milling technique using the mechanical alloying method has been employed for fabrication of glassy Co_100−xTi_x (25≤x≤67) alloy powders at room temperature. The fabricated glassy alloys in the Co-rich (33≥x) side exhibit good soft magnetic properties. The binary glassy alloys for which the glass transition temperatures (T_g) have rather high temperatures (above 800 K), show large supercooled liquid regions before crystallization (ΔT_x larger than 50 K). The reduced glass transition temperature (ratio between T_g and liquidus temperatures, T_l (T_g/T_l)) was found to be larger than 0.56. We have also performed post-annealing experiments on the mechanically deformed Co/Ti multilayered composite powders. The results show that annealing of the powders at 710 K leads to the formation of a glassy phase (thermally enhanced glass formation reaction), of which the heat of formation was measured directly. The similarity in the crystallization and magnetization behaviors between the two classes of as-annealed and as-mechanically alloyed glassy powders implies the formation of the same glass state.     

Ta，b和MoTi50Ni20Cu25Sn5非晶合金玻璃形成能力的影响

利用旋转铜辊急冷法和铜模铸造法制备非晶合金薄带或圆棒，并采用X衍射仪(XRD)、差示扫描量热仪(DSC)和差示热分析仪(DTA)研究了Ta，Nb和Mo对Ti50Ni20Cu25Sn5非晶合金玻璃形成能力(GFA)的影响。结果表明，Ta的添加提高了Ti50Ni20Cu25Sn5合金的GFA，Mo的添加降低了该合金的GFA，Nb的添加剂对该合金的GFA没有明显的影响；含Ta合金具有超过60K的宽过冷液态区(△Tx)，且其约化玻璃转变温度因子(Tg／Tm)大于含Nb合金和含Mo合金；采用常规铜模铸造法制备出了直径为lmm的(Ti0.5Ni0.2Cu0.25Sn0.05)98Ta2和(Ti0.5Ni0.2Cu0.5Sn0.05)96Ta4块状非晶圆棒；(Ti0.5Ni0.2Cu0.25Sn0.05)98Ta2块状非晶圆棒的Tg，△Tx和Tg／Tm分别为678K，84K和0．60，而(Ti0.5Ni0.2Cu0.25Sn0.05)96Ta4块状非晶圆棒的Tg，△Tx和Tg／Tm分别为680K，70K和0．60。     

Deformation of Zr41Ti14 Cu12. 5Ni10Be22.5 bulk amorphous alloy under isobaric pressure in super-cooled liquid region

The curve of crystallization transition during continuous heating for the Zr41Ti14 Cu12. 5Ni10Be22.5 bulk amorphous alloy was measured by means of dilatation(Fully automatic transformation recording/measuring instrument) and X-ray diffraction(XRD) method. The deformation behavior of the alloy at various heating rates in the supercooled liquid region was studied. The results show that the glass transition temperature of the alloy increases slightly and the supercooled liquid region(SLR) increases significantly with increasing heating rate. The deformation amount under isobaric pressure of 1 N for the alloy in the SLR increases with increasing heating rate. As the heating rate of the alloy increases from 5 to 100℃/rain, the amount of deformation of the alloy increases from 8.3% to 45%     

Cu-based bulk amorphous alloy with larger glass-forming ability and supercooled liquid region

The glassy rod with a maximum sample thickness of 11 mm and larger supercooled liquid region of 108 K was successfully fabricated when substituting Cu with minor amount of Ag in the Cu–Zr–Al–Gd alloy system. The value of γ reaches a maximum of 0.418 for the Cu_45.5Zr₄₅Al₇Gd₂Ag_0.5 bulk metallic glass (BMG) alloy. The high glass-forming ability (GFA) and larger supercooled liquid region are discussed from atomic size, negative mixing heat among constituent elements and thermodynamics.     

Cu坯料纯度对Cu46Zr42Al7Gd5合金非晶形成能力与显微硬度的影响

采用铜模吸铸法制备直径为3 mm的Cu46Zr42Al7Gd5块体非晶合金;研究Cu坯料纯度对该合金非晶形成能力、热稳定性和显微硬度的影响.结果表明:采用纯度较低的Cu坯料,分别以25%和50%的比例替代纯度较高的Cu坯料后,仍可制备直径为3 mm的非晶态合金;当替代比例提高到75%或更高时,合金呈现完全晶态相;当替代比例为25%时,合金的玻璃化转变温度为669 K,晶化温度为749 K,过冷液相区为80 K;当替代比例为50%时,合金的玻璃转化温度为684 K,晶化温度为751 K,过冷液相区为67 K;两种替代比例(25%和50%)的合金经573 K保温1 h热处理后,仍然保持非晶态结构;当替代比例为25%时,合金经673和773 K热处理后,合金由基体及弥散分布于其上的第二相组成,显微硬度明显提高;当替代比例为50%时,经673 K处理后,合金由基体及不均匀弥散分布于其上的第二相组成,显微硬度有所提高,而经773 K处理后,由第二相弥散分布于白色基体的白色区域和由细小白、灰两相混合组成的灰色区域组成,显微硬度大幅度提高.     

一种新型Nd基块体非晶合金

在铜模铸造条件下制备了直径2．5mm的Nd61Fe30Zn9块状非晶合金．在普通DSC条件下，没有观察到这种合金的玻璃转变温度，晶化温度为730K，比Nd60Fe30Al10非晶合金的晶化温度低约70K，因此该合金的热稳定性较低．熔化行为分析表明，合金Nd61Fe30Zn9的熔化过程为单峰吸热过程，且熔化区间仅为54K，说明该合金的成分接近合金的共晶成分，但母合金的自然凝固组织不具有共晶凝固特点，表现为粗大的枝晶状组织．讨论了成分和组织对合金非晶形成能力的影响．     

Misch metal based metallic glasses

In this paper, a glass-forming range of metallic glasses based on Ce-rich misch metal (Mm) was pinpointed in Mm-Al-Co composition map by melt spinning. The thermal analysis indicated that the wide supercooled liquid region (above 60 K) can be found out in a large composition range in Mm-Al-Co system. The investigation of the glass-forming ability (GFA) in this system indicated a glassy composition with a larger supercooled liquid region wouldn’t be the glassy former with higher GFA. The reduced glass transition temperature is a better indicator to explore metallic glasses with high GFA. Furthermore, the mechanical properties of Mm₆₅Al₁₀Co₂₅ bulk glassy samples were evaluated in a compressive measurement. The obvious advantages of the Mm-based BMGs with high GFA, good mechanical properties and low material cost make these BMGs hopeful to be applied in the future.