Si3N4/AgCu/TiAl钎焊接头界面结构及性能

采用AgCu非活性钎料实现了Si3N4陶瓷与TiAl基合金的钎焊,确定接头的典型界面组织结构为:TiAl/Ti3Al+Ti(s,s)/AlCuTi/Ag(s,s)+AlCu2Ti/Ti5Si3+TiN/Si3N4陶瓷。钎焊过程中,活性元素Ti从TiAl母材溶解到钎料中与Si3N4陶瓷发生反应润湿,实现了TiAl与Si3N4陶瓷的连接。随着钎焊温度的升高及保温时间的延长,靠近Si3N4陶瓷的TiN反应层厚度增加,Ag基固溶体中弥散分布的AlCu2Ti化合物聚集长大成块状,导致接头性能下降。当钎焊温度T=860℃,保温时间为5min时接头抗剪强度达到最大值124.6MPa。基于反应热力学及动力学计算TiN层反应激活能Q约为528.7kJ/mol,860℃时该层的成长系数KP=2.7×10-7m/s1/2。     

颗粒增强复合钎料钎焊TiAl合金接头界面结构及性能

采用纳米Si3N4颗粒增强的AgCuTi复合钎料(AgCuTiC)实现了TiAl合金的钎焊连接.利用SEM,EDS及XRD等分析方法确定了TiAl/AgCuTiC/TiAl接头的典型界面结构为TiAl/AlCu2Ti/Ag(s,s)+TiN+ Al4Cu9+Ti5Si3.结果表明,钎焊过程中从TiAl母材溶入液相钎料的活性钛与复合钎料中纳米Si3N4颗粒发生反应,在钎缝中形成了细小的颗粒状TiN,Ti5Si3及Al4Cu9化合物增强的银基复合材料组织.银基复合材料的形成不仅提高了钎缝自身的强度,而且通过降低钎缝的线膨胀系数缓解了接头残余应力,并最终改善了钎焊接头的性能.当采用增强相含量为3％的AgCuTiC钎料在880℃保温5min条件下钎焊时,接头室温平均抗剪强度最高为278 MPa,比采用AgCuTi钎料提高40％.     

TiAl合金与镍基高温合金的扩散连接

采用钛为中间层,对TiAl合金与镍基高温合金（GH99）进了扩散连接.研究了扩散连接接头的界面结构和连接温度对界面结构及连接性能的影响,并对连接界面反应层的形成机制进行探讨.结果表明,GH99/Ti/TiAl的界面结构为：GH99/（Ni,Cr）ss/富Ti-（Ni,Cr）ss/TiNi/Ti2Ni/α-Ti＋Ti2Ni/Ti（Al）ss/TiAl＋Ti3Al/TiAl;随着连接温度的升高,各反应层厚度增加,接头的抗剪强度先增加后减小;在连接温度1 173 K,连接时间30 min,连接压力20 MPa时,抗剪强度最高为260.7 MPa.     

TiAl/Ti/Nb/GH99扩散连接接头的界面组织结构及接头强度

采用Ti/Nb复合中间层对TiAl与镍基高温合金(GH99)进行扩散连接.采用扫描电镜、电子探针和X射线衍射等手段对连接接头的生成相及界面组织结构进行分析,采用抗剪强度测试对接头的连接强度进行评价.结果表明,GH99/Nb/Ti/TiAl的典型界面结构为GH99/(Ni,Cr)ss/Ni3Nb/Ni6Nb7/Nb/(Ti,Nb)ss/α-Ti+(Ti,Nb)ss/Ti3Al/TiAl.当连接温度为900℃,连接时间为30 min,连接压力为20 MPa时,所得接头抗剪强度最高为273.8 MPa.随着连接温度的升高,界面组织结构及反应层厚度发生变化.当连接温度T>900℃时,界面处生成对接头强度有不利影响的Ni6Nb7反应层;根据试验结果,进一步分析了各反应层的形成过程,揭示了GH99/Nb和Nb/Ti/TiAl的界面扩散反应机制.     

TiAl/40Cr高频感应钎焊接头的界面组织及力学性能

以Ag-Cu-Ni-Li为钎料对TiAl与40Cr进行了高频感应钎焊,研究了TiAl/40Cr钎焊接头的界面组织和力学性能.采用扫描电镜、电子探针、X射线能谱分析仪等分析了界面组织及生成相,测试了接头的抗拉强度及界面生成相的显微硬度.结果表明:钎料与2种母材发生界面生反应成Al3Ti、Ag[s,s]、Ti(CuAl) 2、Ti2Ni和TiC等多种反应相,接头界面结构Al/A为Til3Ti/Al3Ti十Ag[s,s]/Ti(CuAl)2 Ti2Ni Ag[s,s]/TiC/40Cr.在实验所选的工艺参数范围内,当连接温度θ=850℃,保温时间t=180 s时,接头的抗拉强度达到265 MPa.     

Si3N4／Cu68Ti20Ni12的界面结构及连接强度

采用Cu68Ti20Ni12钎料进行了Si3N4／Si3N4的活性钎焊连接。结果表明：钎焊温度和时间对连接强度有重要影响；在1373K，10min的连接条件下，Si3N4/Si3N4连接强度达到最大值289MPa。通过对Si3N4／Cu68Ti20Ni12界面区的微观分析：发现Ti，Ni明显向Si3N4方向富集，相对Ni而言，Ti的富集区更靠近Si3N4陶瓷，而Si则向钎料方向扩散，Cu在接头中心富集：界面区存在2层反应层，反应层Ⅰ为TiN层，而反应层Ⅱ则由TiN，Ti5Si4，Ti5Si3，Ni3Si及NiTi化合物组成。     

连接温度对TiAl/Ti3AlC2扩散焊接头界面结构及性能的影响

采用Ti/Ni复合中间层实现了TiAl合金和Ti₃AlC₂陶瓷的扩散连接,利用SEM,XRD等分析方法对接头界面结构进行了分析.结果表明,TiAl/Ti₃AlC₂接头典型界面结构为TiAl/Ti₃Al+Al₃NiTi₂/Ti₃Al/α-Ti+Ti₂Ni/Ti₂Ni/TiNi/Ni₃Ti/Ni/Ni₃(Ti,Al)/Ni₃Al+TiC_x+Ti₃AlC₂/Ti₃AlC₂.随着连接温度的升高,TiAl/Ti界面处的Ti_ss层逐渐减小,Ti₃Al化合物层逐渐变厚;TiNi化合物层厚度显著增加,Ti₂Ni和Ni₃Ti层厚度基本保持不变.接头抗剪强度随连接温度升高先增加后减小,当连接温度为850℃时,接头的抗剪强度最高可达到85.3 MPa.接头主要在Ni/Ti₃AlC₂界面及Ti₃AlC₂基体处发生断裂.     

保温时间对TiAl合金与镍基合金扩散连接界面组织结构及连接强度的影响

采用纯钛箔做中间层扩散连接TiAl合金与镍基高温合金(GH99).利用扫描电镜、电子探针和X射线衍射等手段对界面产物及接头的界面结构进行分析.结果表明,GH99/Ti界面主要由四个反应层组成,分别为(Ni,Cr)ss,富Ti-(Ni,Cr)ss,TiNi和Ti2Ni.当保温时间较短时,Ti/TiAl界面反应层主要为Ti(Al)ss.延长保温时间,此界面反应层转化为Ti3Al和Al3NiTi2.随着保温时间的延长,TiNi反应层厚度持续增加,而Ti2Ni反应层厚度先增加后减小.随保温时间的延长接头的抗剪强度先增加后减小,然后又增加.由接头断口形貌可以看出,接头主要断裂于Ti2Ni反应层.     

复合阻隔法的阻隔效应原理及其在扩散连接中的应用

以TiAl金属间化合物增压涡轮与 4 0Cr钢轴的扩散连接为背景 ,提出了复合阻隔法扩散连接工艺 ,并探讨了阻隔效应原理 ,建立了从材料的扩散连接性角度出发的原子半径、原子电负性阻隔层选择原则。利用本文的扩散连接阻隔效应原理 ,确定了TiAl金属间化合物增压涡轮与 4 0Cr钢轴的扩散连接复合阻隔层为Ti/V/Cu ,由此得到的扩散连接接头在V/Cu及Cu/ 4 0Cr的连接界面处出现了对连接性能有利的无限固溶体层 ,在TiAl/Ti的接触面上生成了能够强化接头强度的Ti3 Al TiAl双相层和Ti的固溶体层 ,与TiAl/ 4 0Cr直接扩散连接相比 ,Ti/V/Cu复合阻隔层的加入 ,避免了在TiAl/4 0Cr的接触面上TiC、Ti3 Al、FeAl、FeAl2 金属间化合物脆性相的产生 ,接头强度高达4 2 0MPa ,因此利用本文的阻隔效应原理可以很好地进行复合阻隔层的选择     

活性金属部分瞬间液相连接氮化硅陶瓷的研究

采用Ti/Cu/Ti多层中间层在1273 K温度下进行氮化硅陶瓷部分瞬间液相连接,考察了保温时间对连接强度的影响,并对连接界面进行了SEM,EPMA和XRD分析.结果表明,通过Cu-Ti二元扩散促使液相与氮化硅发生界面反应,形成Si3N4/TiN/Ti5Si3+Ti5Si4+TiSi2/TiSi2+Cu3Ti2(Si)/Cu的梯度层.保温时间影响接头反应层厚度,从而影响接头的连接强度根据活性金属部分瞬间液相连接陶瓷的界面行为,建立了活性金属部分瞬间液相连接陶瓷的理论模型.该模型较好地解释了Ti/Cu/Ti和Ti/Ni/Ti连接氮化硅陶瓷的异同点和连接工艺参数的选择.     

X-ray diffraction study of Ba0.985Na0.015Ti0.985Nb0.015O3, Ba0.6Na0.4Ti0.6Nb0.4O3 and Ba0.3Na0.7Ti0.3Nb0.7O3 compositions

The Ba_0.985Na_0.015Ti_0.985Nb_0.015O₃, Ba_0.6Na_0.4Ti_0.6Nb_0.4O₃ and Ba_0.3Na_0.7Ti_0.3Nb_0.7O₃ compositions of the (1 − x) BaTiO₃–xNaNbO₃ (BTNNx) system have been studied by X-ray diffraction and by measurements of dielectric properties. The specimens with composition BTNN (x = 0.015, 0.40 and 0.70) have been refined by the JANA program from X-ray powder diffraction data. Ceramic samples with composition (1 − x) BaTiO₃ + xNaNbO₃ (where x = 0.015, 0.40 and 0.70) were prepared by calcinations from appropriate mixture of BaCO₃, TiO₂, Na₂CO₃ and Nb₂O₅. The calcined powder was sintered at temperature range 1200–1400 °C. As the composition x increased from 0.015 (and 0.70), the ferroelectric ceramics (x = 0.015, FE) with tetragonal phase changed to the ferroelectric relaxors (RFE, x = 0.40). RFE ceramics showed a peculiar diffuse phase transition and dielectric relaxation at the low temperature (down to 180 K) due to a frustration between RFE and FE state. These ceramics present the classical ferroelectric character when 0 ≤ x < 0.075 and 0.55 < x ≤ 1 and relaxor character when 0.075 ≤ x ≤ 0.55.     

Magnetic, electrical and plastic properties of Fe76Nb2Si13B9, Fe75Ag1Nb2Si13B9 and Fe75Cu1Nb2Si13B9 amorphous alloys

Influence of 1 h annealing in vacuum on magnetic, electrical and plastic properties of Fe₇₆Nb₂Si₁₃B₉, Fe₇₅Ag₁Nb₂Si₁₃B₉ and Fe₇₅Cu₁Nb₂Si₁₃B₉ melt spun ribbons were carefully investigated. It was shown that in all cases soft magnetic properties can be significantly enhanced by applying 1-h annealing at characteristic temperatures T_op. This optimization annealing causes that permeability increases more than 15-times and magnetic losses (tangent of loss angle) achieves a minimum in relation to the as quenched state. Using structural examinations (X-ray and HRTEM) it was shown that for the Fe₇₅Cu₁Nb₂Si₁₃B₉ alloy the optimized microstructure corresponds to a nanocrystalline αFe(Si) phase whereas in other alloys to a relaxed amorphous phase free of iron nanograins. As a consequence of this fact the Fe₇₆Nb₂Si₁₃B₉ and Fe₇₅Ag₁Nb₂Si₁₃B₉ alloys show higher plasticity in comparison to the nanocrystalline Fe₇₅Cu₁Nb₂Si₁₃B₉ alloy. Temperatures of the first stage of crystallization, and related diffusion parameters were determined using measurements of resistivity versus temperature with different heating rates.     

Fe2+-Ni2+-NH3-NH4+-C2O42-H2O体系的沉淀配合平衡热力学

针对草酸盐配位共沉淀热分解还原法制备超细铁镍合金粉过程中Fe2+-Ni2+-NH3-NH4+-C2O42--H2O体系的溶液平衡建立热力学分析模型,并根据模型进行相关计算,揭示反应体系中各物质随pH值、氨及草酸浓度的变化关系。结果表明:溶液中的Fe主要以[Fe(C2O4)n]2 2n络合物形式存在,而铁氨络合物含量很低。当氨含量较低时,溶液中的Ni主要以[Ni(C2O4)n]2 2n存在;氨含量较高时,在酸性条件下,溶液中的Ni主要以[Ni(C2O4)n]2 2n存在,在碱性条件下,则主要以[Ni(NH3)n]2+存在。低pH值下,Ni的沉淀率较Fe的高,而高pH值下,Ni的沉淀率则较Fe的低。     

New Zr6CoAs2-type compounds: Y6CoBi2, Ho6CoBi2 and Tm6CoBi2

Results of a powder X-ray diffraction investigation of new ternary compounds are reported. The compounds Y₆CoBi₂ [a=0.8312(1) nm, c=0.4144(1) nm], Ho₆CoBi₂ [a=0.8246(2) nm, c=0.4095(1) nm], and Tm₆CoBi₂ [a=0.8155(2) nm, c=0.4066(1) nm] crystallize in the hexagonal Zr₆CoAs₂-type structure (space group P6b2m No. 189). The Zr₆CoAs₂-type structure is a superstructure of the Fe₂P-type structure.     

Thermodynamics and phase diagrams in the binary systems Na2O-SiO2, Na2O-GeO2, Na2O-B2O3, Li2O-B2O3, CaO-B2O3, SrO-B2O3, and BaO-B2O3

We applied our model to the enthalpy of mixing data of the binary systems Na₂O-SiO₂, Na₂O-GeO₂, Na₂O-B₂O₃, Li₂O-B₂O₃, CaO-B₂O₃, SrO-B₂O₃, and BaO-B₂O₃. The most stable composition in the liquid, that is where the enthalpy of mixing is most negative, is with a metal-oxygen ratio of 4 to 3, for monovalent metals (Na and Li) and 3 to 4 for divalent metals (Ba and Ca) in liquid silicates or borates. The same applies to the CaO-SiO₂, CaO-Al₂O₃, PbO-B₂O₃, PbO-SiO₂, ZnO-B₂O₃, and ZnO-SiO₂ systems. The oxygen to metal ratio, its constant value in various types of systems, reflects and describes the structure of the liquid. Using the analyzed enthalpies of mixing data and the available phase diagrams, we calculated the enthalpies of formation of the various binary compounds. The results are in excellent agreement with data in the literature that were obtained from direct solid-solid calorimetry.     

Al2O3-Sm2O3-CeO2电解质的性能（英文）

采用溶胶-凝胶法和低温燃烧技术制备Ce1-xSmxO2（x=0,0.1,0.2,0.3）和掺杂Sm和（2%-8%）Al2O3的二氧化铈;研究其合成、结构、致密化、导电性和热膨胀等性能,并利用XRD研究其结构和相组成。结果表明,于1300°C烧结球团,获得致密的陶瓷,于1250°C在Ce0.8Sm0.2O0.2中加入2%和4%的Al2O3以促进烧结。利用扫描电子显微镜观察烧结后球团的表面形貌,使用双探针交流阻抗谱研究总离子电导率。     

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.     

Zur Kenntnis von RbBa3Ca4Cu3V7O28

Single crystals of RbBa₃Ca₄Cu₃V₇O₂₈ were prepared above the melting point of the reaction mixture. It crystallizes with hexagonal symmetry, space group C_6V⁴-P6₃mc, a 11.1751, c 12.434 Å, Z = 2. RbBa₃Ca₄Cu₃V₇O₂₈ is the second member of a new structure type of the copper-oxovanadates. Ba²⁺ shows an unusual 12-fold coordination. The two calcium positions are coordinated by trigonal prisms and octahedra respectively. The copper coordination is characterized by a stretched square pyramid. The Cu²⁺ ions are outside the centre nearly in plane of the pyramids.

Zusammenfassung

Einkristalle von RbBa₃Ca₄Cu₃V₇O₂₈ wurden oberhalb des Schmelzpunktes der Reaktionsmischung erhalten. Die Verbindung kristallisiert hexagonal, Raumgruppe C_6V⁴-P6₃mc, a 11.1751, c 12.434 Å, Z = 2. RbBa₃Ca₄Cu₃V₇O₂₈ ist das zweite Beispiel für einen neuen Strukturtyp der Kupfer-Oxovanadate, mit 12-fach koordinierten Ba²⁺ -Ionen. Die zwei Calciumpositionen sind trigonal prismatisch bzw. oktaedrisch koordiniert. Die Koordination der Cu²⁺-Ionen ist durch eine gestreckte Pyramide charakterisiert. Cu²⁺ ist auβerhalb des Polyederzentrums nahezu in der quadratischen Fläche der Pyramide angeordnet.     

电弧喷涂制备Fe65Cr20Mo7B3.5SiMn1.5W3涂层

在Q235低碳钢板上利用电弧喷涂工艺进行喷涂,以制得Fe65Cr20Mo7B3.5SiMn1.5W3涂层。喷涂材料为自行配制的丝材,按照35%的填充率将配好的粉填充到U型不锈钢外皮中,经过多道拉拔、挤压工艺制成Φ2mm的粉芯丝材。采用X射线衍射仪、扫描电镜、能谱分析仪、透射电镜对涂层的物相和组织形貌及成分进行了表征;采用差示扫描量热仪、显微硬度仪等设备对涂层的热稳定性及显微硬度进行了检测和分析。试验结果表明:涂层组织形貌呈典型的层状组织结构,由变形良好的带状粒子相互搭接堆积而成。涂层含有50.63%的非晶相,同时含有纳米级的晶相。涂层组织均匀、结构致密、孔隙率低,并且涂层硬度高达1040.5HV0.3,属硬质涂层,具有良好的热稳定性。