保温时间对瞬时液相扩散连接的Ti3Al /Ti2AlNb接头微观结构及力学性能的影响

采用Ni-Ti复合箔片作为中间层,在990 ℃、低连接压力（0.1 MPa）下,通过瞬时液相（TLP）扩散连接制备了Ti₃Al/Ti₂AlNb异种合金接头。分析了保温时间（10~90 min）对Ti₃Al/Ti₂AlNb接头微观结构及力学性能的影响,并研究了TLP扩散连接接头的界面演变和形成机制。结果表明,Ti₃Al/Ti₂AlNb接头具有典型的“Ti₃Al | Al_0.5Nb_0.5Ti₃ | 残余 Ni | NiTi | NiTi₂ | 残余 Ti | Al_0.5Nb_0.5Ti₃ | Ti₂AlNb”多层梯度结构。随着保温时间的延长,接头的抗剪切强度先增大后减小,当保温时间达到60 min时,Ti₃Al/Ti₂AlNb接头的抗剪切强度最大,达到167±12 MPa。另外,接头的断裂主要发生在Ti₂AlNb/Ti附近的NiTi₂层,并向Ti层延伸,呈现出脆性断裂的特征。     

空气气氛下碳热还原筛分法制备Magnéli相Ti n O2 n -1

介绍了一种在空气气氛中通过碳热还原筛分法制备Magnéli相（Ti_nO_2n-1，4＜n＜10）低价钛氧化物的方法，研究了还原温度和还原时间对还原产物的物相、电阻率的影响。结果表明，提高还原温度和延长还原时间有利于将TiO₂还原为Magnéli相Ti_nO_2n-1。将Magnéli相Ti_nO_2n-1 (n=4，5) 粉末在1350 ℃下干燥20 min，通过扫描电子显微镜观察，其粒径为0.5~8 μm。在还原温度为1350 ℃时，还原产物的电阻率随还原时间的延长而显著降低。在1350 ℃下还原50 min的产物的电阻率最小，为79.3 Ω?cm，其物相组成几乎全部为Ti₃O₅。     

TiZrNiCu钎焊Si3N4-MoSi2复合陶瓷与Nb接头组织与力学性能

采用高温活性钎料TiZrNiCu对Si₃N₄-MoSi₂复合陶瓷和金属Nb进行真空钎焊试验,研究了其典型界面组织组成及形成机理,分析了钎焊温度和保温时间对钎焊接头界面组织及力学性能的影响规律。结果表明,接头典型界面结构为Nb/β-Ti/(Ti. Zr)₂(Cu, Ni)+β-Ti+(Ti, Zr)₅Si₃/TiN+(Ti, Zr)₅Si₃+MoSi₂/Si₃N₄-MoSi₂。钎焊温度和保温时间主要通过控制Si₃N₄-MoSi₂复合陶瓷母材中Si原子向钎料中扩散程度,来影响钎缝中(Ti, Zr)₅Si₃化合物的数量及分布,进而影响钎焊接头的抗剪强度。在920 ℃/10 min的工艺参数下,Si₃N₄-MoSi₂/Nb接头的室温抗剪强度最高达到112 MPa,选择最优参数条件下的Nb/Si₃N₄-MoSi₂钎焊接头在500 ℃和600 ℃条件下进行高温剪切实验,其高温抗剪强度分别达到123 MPa和131 MPa。     

Al2O3陶瓷/AgCuTi/GH99高温合金的钎焊接头力学性能

采用AgCuTi钎料对Al₂O₃陶瓷与GH99高温合金进行了钎焊连接,研究了工艺参数(连接温度、保温时间)的变化对接头力学性能的影响,并分析了不同参数下接头的断裂位置,结果表明：保温5min时,在不同的连接温度下进行钎焊,随着连接温度的升高,接头的抗剪强度先增后减,在900℃时取得最大值,为127.24MPa,连接温度较低时,主要断裂于Al₂O₃/钎料侧,随着温度的升高,接头TiNi₃反应层增厚,因此还有部分断裂于TiNi₃反应层/钎料界面;在连接温度为900℃时,随着保温时间的延长,接头的抗剪强度逐渐降低,保温时间较短时,主要要断裂于Al₂O₃/钎料界面,保温时间过长,TiNi₃反应层延伸入钎料中部且厚度大大增加,在该反应层中产生微裂纹,造成接头强度大大降低,此时部分断裂于钎料中部及TiNi₃反应层中。     

Ti活度对Al2O3/AgCuTi/Fe-Ni-Co钎焊接头机械性能和微观组织结构的影响

采用AgCuTi钎料实现了Al₂O₃陶瓷与Fe-Co-Ni合金的钎焊连接,并调查了不同钛含量的钎料对Al₂O₃/AgCuTi/Fe-Ni-Co钎焊接头机械性能和微观组织结构的影响。扫描电子显微镜(SEM), X射线能量色散光谱仪(EDS), X射线衍射仪(XRD)及电子万能试验机用于分析钎焊接头的机械性能和微观组织结构,结果表明:钛含量的增加明显提高AgCuTi钎料与Al₂O₃陶瓷的相互作用,在Al₂O₃/Ag-Cu-Ti界面生成一层由Ti-Al 和 Ti-O化合物组成的反应层。Al₂O₃/AgCuTi/Fe-Ni-Co钎焊接头的抗拉强度随钛含量的增加而增加,当钛含量提高到8wt.%时,抗拉强度达到最大值78Mpa。通过微观组织结构分析发现,采用AgCu4Ti在890℃保温5min的条件下可以获得较好的钎焊接头,典型接头的微观组织结构为Al₂O₃/TiAl+Ti₃O₅/NiTi+Cu₃Ti+Ag(s,s)/Ag(s,s)+Cu(s,s)+(Cu,Ni)/Fe-Ni-Co。采用AgCu8Ti获得的钎焊接头的界面反应层与AgCu4Ti差异不大,但反应层稍微增厚,并伴有TiO和Ti3Al在Al₂O₃/Ag-Cu-Ti界面生成。     

空气反应钎焊ZrO2与GH3536接头组织与力学性能

采用Al₂TiO₅颗粒增强的Ag-CuO-Al₂TiO₅复合钎料,在钎焊温度为1050 ℃保温30 min工艺参数下,对ZrO₂陶瓷与GH3536合金进行了空气反应钎焊(RAB),分析了钎焊接头的界面结构及其形成机制;同时研究了接头在800 ℃氧化不同时间的组织演变规律及其对连接性能的影响。结果表明,钎焊过程中Al₂TiO₅颗粒分解产生Al₂O₃和TiO₂,TiO₂与ZrO₂陶瓷反应生成ZrTiO₄相。GH3536侧金属元素发生氧化形成尖晶石层,并分别与钎缝中的Al₂O₃、CuO反应,在钎缝中生成细密分布的NiAl₂O₄相及紧邻尖晶石层的团块状NiCuO₂相。ZrO₂/GH3536接头高温氧化1000 h后,钎缝中NiAl₂O₄呈团块状分布,Cr₂O₃薄层保持稳定;尖晶石层内部元素均匀化,厚度有明显增加。接头强度随着氧化时间的延长先降低后稳定在20 MPa。     

TiAl合金与GH3039摩擦焊接界面组织

使用GH3039合金作为γ-TiAl与碳钢摩擦焊接的过渡第三体,采用扫描电子显微镜（SEM）和透射电子显微镜（TEM）分析了TiAl/GH3039摩擦焊接接头的界面结构。结果表明,γ-TiAl和GH3039摩擦焊接接头的最大抗拉伸强度能达到400 MPa以上。GH3039一侧热力影响区的塑性变形大于TiAl一侧,并且在两侧均发生动态再结晶。接近GH3039母材相层中的Ni含量几乎不变,接近TiAl母材相层中的Ti含量也几乎不变。在GH3039侧面附近的焊接区中,富Ni和富Cr晶粒的分布是互补的。Ti和Al容易溶于富Ni的晶粒中,而Mn容易溶于富Cr的晶粒中。在结合区中形成的大量富Cr晶粒是体心立方结构的α-Cr。γ-TiAl和GH3039摩擦焊接的典型界面结构为：γ-TiAl+α₂-Ti₃Al/α₂+τ₃/τ₃-Al_1+x-yTi_1+yNi_1-x/τ₃+α-Cr/(Ni, Cr)_ss/GH3039。     

Al2O3/Ti2AlN复合材料在900℃,1000℃和1100℃空气中的氧化行为

利用综合热分析仪、背散射扫描电镜(BSE)和能谱分析(EDS)对Al₂O₃/Ti₂AlN复合材料在900 ℃,1 000 ℃和1 100 ℃/20 h空气中连续氧化20h后的氧化增重及氧化层截面进行了研究。结果表明：Al₂O₃/Ti₂AlN复合材料在空气中的氧化行为符合抛物线规律,在900 ℃,1 000 ℃和1 100 ℃/20 h氧化增重分别为2.78×10_-2 kg/m₂、10.4 ×10_-2 kg/m₂、21.9 ×10_-2 kg/m₂,抛物线速率常数相应为1.08×10_-8 kg₂/m₄s、1.44×10_-7 kg₂/m₄s、6.56×10_-7 kg₂/m₄s,氧化激活能为274 kJ/mol。氧化层主要由TiO₂和Al₂O₃组成的,连续的Al₂O₃次外层可以提高其抗氧化性能。氧化层结构的改变是由于氧化温度对Ti₄₊、Al₃₊由基体表面向外扩散和O_2-向内扩散的影响,以及TiO₂和Al₂O₃在不同温度下的形核生长速率导致的。对Al₂O₃/Ti₂AlN而言,控制材料与氧化气氛的界面是提高该材料抗氧化性能的关键。     

高体积分数SiCp/Al电子封装复合材料的钎焊综述

高体积分数SiC_p/Al复合材料作为电子封装材料使用日益流行,其钎焊具有重要的实际意义。近来,一些新钎料合金和工艺被开发用于高体积分数SiC_p/Al复合材料的钎焊。本文回顾了SiC_p/Al复合材料的物理力学性能和制备工艺,综述了应用于高体积分数SiC_p/Al复合材料的合金钎料、钎焊工艺及其接头微结构与性能,旨在进一步理解它们之间的关联性,以优化接头性能与可靠性。往Al?Si合金中添加Cu、Mg、Ni等合金元素有助于提高钎料合金和钎焊接头的使用性能,如可优化钎料合金的应用温度、接头界面结合和焊缝强度。而表面金属化和超声波振动两种钎焊辅助工艺可通过避免或去除复合材料表面的Al₂O₃和SiO₂氧化膜来改善合金钎料的钎焊性。最后,指出需要进一步加强对合金钎料的优化设计、表面金属化工艺以及焊料/涂层/基材体系之间的润湿性和界面行为的研究。     

稀土改性Fe-Al层表面Al2O3 薄膜的物相分布

在760 ℃下采用稀土改性包埋渗铝以及原位氧化方法制备Fe-Al/Al₂O₃复合涂层,研究了渗铝层和氧化膜的微观组织和相分布。结果表明,稀土改性渗铝层可分为3层：外层渗铝层、过渡层和内扩散层。渗铝层主要由FeAl相和Fe₃Al相组成。FeAl相主要集中在渗铝层的外层,为Al₂O₃氧化膜的选择性氧化提供了有利条件。氧化膜表面呈α-Al₂O₃脊状结构。此外,表面氧化铈的存在是由于氧化初期Ce向外扩散且与O₂的优先反应。氧化膜可分为2层,即纯α-Al₂O₃层和主要由α-Fe(Al)和Al、Fe、Ce的混合氧化物组成的过渡层。     

Effect of non-magnetic doping on multi-step magnetization behavior of Dy50−xAlxAg50

The electrical transport and magnetization measurements have been carried out on Al-doped polycrystalline intermetallic compounds Dy_50−xAl_xAg₅₀ (x = 0, 0.3, 0.6, 1.2, 1.8) in a pulsed high magnetic field, in which multi-step magnetization is observed. Partial substitute of non-magnetic Al³⁺ for Dy³⁺ ions in the compounds increases the critical magnetic fields and the relative area of the magnetic hysteresis loop, which result from the pinning effect, lattice distortion, the change of coupling strength and dilution effect related to the Al³⁺ doping.The experimental results indicate that non-magnetic Al³⁺ ions and induced amorphous phase can pin the rotation and/or growth of magnetic domains, thus, the critical magnetic field can be enhanced by doping non-magnetic ions in the magnetic materials, especially in the permanent magnet materials.     

Effects of K2O-Li2O doping on surface and catalytic properties of Fe2O3/Cr2O3 system

The effects of K₂O and Li₂O-doping (0.5, 0.75 and 1.5 mol%) of Fe₂O₃/Cr₂O₃ system on its surface and the catalytic properties were investigated. Pure and differently doped solids were calcined in air at 400-600 °C. The formula of the un-doped calcined solid was 0.85Fe₂O₃:0.15Cr₂O₃. The techniques employed were TGA, DTA, XRD, N₂ adsorption at −196 °C and catalytic oxidation of CO oxidation by O₂ at 200-300 °C. The results revealed that DTA curves of pure mixed solids consisted of one endothermic peak and two exothermic peaks. Pure and doped mixed solids calcined at 400 °C are amorphous in nature and turned to α-Fe₂O₃ upon heating at 500 and 600 °C. K₂O and Li₂O doping conducted at 500 or 600 °C modified the degree of crystallinity and crystallite size of all phases present which consisted of a mixture of nanocrystalline α- and γ-Fe₂O₃ together with K₂FeO₄ and LiFe₅O₈ phases. However, the heavily Li₂O-doped sample consisted only of LiFe₅O₈ phase. The specific surface area of the system investigated decreased to an extent proportional to the amount of K₂O and Li₂O added. On the other hand, the catalytic activity was found to increase by increasing the amount of K₂O and Li₂O added. The maximum increase in the catalytic activity, expressed as the reaction rate constant (k) measured at 200 °C, attained 30.8% and 26.5% for K₂O and Li₂O doping, respectively. The doping process did not modify the activation energy of the catalyzed reaction but rather increased the concentration of the active sites without changing their energetic nature.     

Sinterability and dielectric properties of Ba0.55Sr0.4Ca0.05TiO3-CaTiSiO5-Mg2TiO4 composite ceramics

The composite ceramics of Ba_0.55Sr_0.4Ca_0.05TiO₃-CaTiSiO₅-Mg₂TiO₄ (BSCT-CTS-MT) were prepared by the conventional solid-state route. The sintering performance, phase structures, morphologies, and dielectric properties of the composite ceramics were investigated. The BSCT-CTS-MT ceramics were sintered at 1100 °C and possessed dense microstructure. The dielectric constant was tailored from 1196 to 141 as the amount of Mg₂TiO₄ increased from 0 to 50 wt%. The dielectric constant and dielectric loss of 40 wt% Ba_0.55Sr_0.4Ca_0.05TiO₃-10 wt% CaTiSiO₅-50 wt% Mg₂TiO₄ was 141 and 0.0020, respectively, and the tunability was 8.64% under a DC electric field of 8.0 kV/cm. The Curie peaks were broadened and depressed after the addition of CaTiSiO₅. The optimistic dielectric properties made it a promising candidate for the application of tunable capacitors and phase shifters.     

Low temperature sintering and microwave dielectric properties of (Mg0.7Zn0.3)0.95Co0.05TiO3 ceramics with BaCu(B2O5) additions

The effects of BaCu(B₂O₅) additives on the sintering temperature and microwave dielectric properties of (Mg_0.7Zn_0.3)_0.95Co_0.05TiO₃ ceramics were investigated. The (Mg_0.7Zn_0.3)_0.95Co_0.05TiO₃ ceramics were not able to be sintered below 1000 °C. However, when BaCu(B₂O₅) were added, they were sintered below 1000 °C and had the good microwave dielectric properties. It was suggested that a liquid phase with the composition of BaCu(B₂O₅) was formed during the sintering and assisted the densification of the (Mg_0.7Zn_0.3)_0.95Co_0.05TiO₃ ceramics at low temperature. BaCu(B₂O₅) powders were produced and used to reduce the sintering temperature of the (Mg_0.7Zn_0.3)_0.95Co_0.05TiO₃ ceramics. Good microwave dielectric properties of Q × f = 35,000 GHz, ?_r = 18.5.0 and τ_f = −51 ppm/°C were obtained for the (Mg_0.7Zn_0.3)_0.95Co_0.05TiO₃ ceramics containing 7 wt.% mol% BaCu(B₂O₅) sintered at 950 °C for 4 h.     

Sol-gel synthesis of Bi3.25La0.75Ti3O12 nanotubes

Ferroelectric Bi_3.25La_0.75Ti₃O₁₂ (BLT) nanotubes were synthesized by sol-gel technique using nanochannel porous anodic aluminum oxide (AAO) templates, and were characterized by X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM) and high resolution transmission electron microscopy (HRTEM). BLT nanotubes with diameter of around 240 nm and the wall thickness of about 25 nm exhibited a single orthorhombic perovskite structure and highly preferential crystal growth along the [1 1 7] orientation, which have smooth wall morphologies and well-defined diameters corresponding to the diameter of the applied template. The formation mechanism of BLT nanotubes was discussed.     

Preparation and characteristic of spherical Li3V2(PO4)3

Spherical Li₃V₂(PO₄)₃ was synthesized by using N₂H₄ as reducer. The products were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). The results show that single-phase, spherical and well-dispersed Li₃V₂(PO₄)₃ has been successfully synthesized in our experimental process. Electrochemical behaviors have been characterized by charge/discharge measurements. The initial discharge capacities of Li₃V₂(PO₄)₃ were 123 mAh g⁻¹ in the voltage range of 3.0–4.3 V and 132 mAh g⁻¹ in the voltage range of 3.0–4.8 V.     

FRICTION WELDING OF Zr55Al10Ni5Cu30 BULK METALLIC GLASS

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T_g附近随温度变化很大, 在T_g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.     

废旧锂离子电池中Li, Fe和V的回收及xLiFePO4-yLi3V2(PO4)3的制备

由于LiFePO_4和Li_3V_2(PO_4)_3材料的特征相近,制备方法类似,提供了一种从废旧LiFePO_4和Li_3V_2(PO_4)_3混合电池中回收Li、Fe和V,再制备xLiFePO_4-yLi_3V_2(PO_4)_3的方法。在空气气氛中600℃热处理1h后,去除粘结剂PVDF使活性物质与集流体分离。调节Li、Fe、V和P摩尔比,球磨、锻烧,配制不同比例的xLiFePO_4-yLi_3V_2(PO_4)_3(x:y=5:1,7:1,9:1)复合电极材料。表征了其形貌、结构和电化学性能,结果表明,回收制备的复合材料将同时具备LiFePO_4和Li_3V_2(PO_4)_3两种材料的电化学性能,能显著改善LiFePO_4的倍率性能。     

二维ZnO/ Bi3.9Zn0.4V1.7O10.5纳米异质结构的制备及其可见光催化活性

表面建造是提高半导体光催化活性的一种有效方法。本文利用Zn5(CO3)2(OH)6纳米片为基底沉积了BiVO4再通过煅烧成功制备了二维ZnO/Bi3.9Zn0.4V1.7O10.5复合纳米片。通过X射线衍射,透射电镜和元素映像技术表征了所制样品。结果显示随着锌与铋的原子比的上升,ZnO多孔片状的表面逐渐变成Bi3.9Zn0.4V1.7O10.5物质。但其比例高于1:0.02时,在片状Bi3.9Zn0.4V1.7O10.5的区域表面又生长出BiVO4纳米颗粒。漫反射光谱测试显示出ZnO/Bi3.9Zn0.4V1.7O10.5复合物随着锌与铋的原子比的上升其在400~600 nm可见光区的吸收逐渐增强。所制样品在可见光（波长大于420 nm）进行了光催化降解罗丹明B的测试,结果表明在所制样品中,锌与铋的原子比为1:0.0133的ZnO/Bi3.9Zn0.4V1.7O10.5纳米片虽然其可见光的吸收并没有明显增强但却表现出最佳的光催化活性。荧光与电化学测试得出了低含量BZVO的ZnO纳米片可见光催化活性的提高主要是因为表面ZnO/Bi3.9Zn0.4V1.7O10.5异质结构提高了光生载流子的分离与传送。这种二维材料的表面建造有利于光催化的进行。因此,此法可应用于其它二维纳米材料的建造以提高光催化活性。     

固相-水热法制备LiFePO4-Li3V2（PO4）3复合材料及其电化学性能（英文）

分别采用固相-水热法和球磨法制备磷酸亚铁锂-磷酸钒锂复合正极材料(LiFePO4-Li3V2(PO4)3)。电化学性能测试表明,LiFePO4-Li3V2(PO4)3复合正极材料的电化学性能远远高于 LiFePO4和 Li3V2(PO4)3单独作为正极材料的性能,并且以固相-水热法制备的复合材料性能优于以球磨法制得的复合材料。研究发现 LiFePO4-Li3V2(PO4)3复合材料有 4 个氧化还原峰,相当于 LiFePO4 和 Li3V2(PO4)3 氧化还原峰的叠加。采用固相-水热法制备的LiFePO4-Li3V2(PO4)3 复合材料形貌较为规则,且有新相物质产生,这是导致其电化学性能较好的原因。