表面活化Al2O3陶瓷与5005铝合金真空钎焊

采用Al-Si钎料对经过Ag-Cu-Ti粉末活性金属化处理的Al₂O₃陶瓷与5005铝合金进行了真空钎焊,研究了钎焊接头的典型界面组织,分析了钎焊温度对接头界面结构特征及力学性能的影响. 结果表明,接头典型界面结构为5005铝合金/α-Al+θ-Al₂Cu+ξ-Ag₂Al/ξ-Ag₂Al+θ-Al₂Cu+Al₃Ti/Ti₃Cu₃O/Al₂O₃陶瓷. 钎焊过程中,Al-Si钎料与活性元素Ti及铝合金母材发生冶金反应,实现对两侧母材的连接. 随着钎焊温度的升高,陶瓷侧Ti₃Cu₃O活化反应层的厚度逐渐变薄,溶解进钎缝中的Ag和Cu与Al反应加剧,生成ξ-Ag₂Al+θ-Al₂Cu金属间化合物的数量增多,铝合金的晶间渗入明显;随钎焊温度的升高,接头抗剪强度先增加后降低,当钎焊温度为610 ℃时,接头强度最高达到15 MPa.     

Al_2O_3陶瓷与紫铜的间接钎焊

利用Sn0.3Ag0.7Cu-4%Ti金属化涂料,在金属化温度900℃、保温时间30 min条件下,对Al2O3陶瓷表面进行金属化处理,然后在钎焊温度600℃、保温时间5 min条件下,利用Sn0.3Ag0.7Cu钎料实现Al2O3陶瓷与紫铜的间接钎焊,通过SEM,EDS和XRD等分析测试手段对金属化层显微组织、Al2O3陶瓷/铜接头结合强度和接头断口形貌等进行了分析.结果表明,利用金属化方法得到了均匀且与Al2O3陶瓷结合良好的金属化层,并实现了Al2O3陶瓷与铜的间接连接,接头界面结构为Cu/Cu3Sn/Cu6Sn5/Sn(s,s)+Ti6Sn5/Al2O3陶瓷.钎焊接头抗剪强度为13.6 MPa,接头断裂发生于金属间化合物层.     

采用AgCuTi活性钎料真空钎焊MgAl_2O_4透明陶瓷

采用Ag Cu Ti活性钎料箔带分别在880℃/10 min和880℃/60 min两种工艺下对Mg Al2O4陶瓷进行了真空钎焊连接,接头冶金质量良好,两种工艺下接头抗剪强度分别为52.4 MPa和61.3 MPa.微观分析结果表明,靠近陶瓷母材附近生成了连续的扩散反应层结构,结合XRD结果,该层主要由Cu Al2O4和Ti O两种化合物组成;钎缝基体区由Cu(s,s),Ag(s,s)和Ti O相组成.     

采用辅助脉冲电流液相扩散连接Ti(C,N)-Al_2O_3的接头形成行为及强度

采用辅助脉冲电流液相扩散连接方法,对Ti(C,N)-Al2O3陶瓷基复合材料与40Cr钢进行了焊接试验,重点研究了在辅助脉冲电流作用下,界面及焊缝组织演变、基体材料溶解等界面行为,探讨了工艺参数对接头强度及断口形态影响规律.结果表明,通过采用辅助脉冲电流液相扩散连接Ti(C,N)-Al2O3与40Cr钢,可以在较短的焊接时间条件下获得较为稳定的接头强度,四点弯曲平均强度位于231~272 MPa之间;降低焊接件整体加热温度以缓解接头残余应力,控制界面和焊缝化学冶金反应进程以较少金属间化合物数量、提高固溶体含量,抑制活性元素Zr向陶瓷基复合材料中的扩散进程以减少陶瓷颗粒向焊缝中的溶解量,是提升焊接接头强度的关键因素.     

Ag-Cu-In-Ti钎料钎焊SiO_(2f)/SiO_2复合材料与钼合金的接头组织及机理

设计了3种Ag-Cu-In-Ti钎料,在800℃/10 min工艺下实现了Si O2f/Si O2复合材料与钼合金的连接.室温下测试了接头的抗剪强度,通过扫描电镜、电子探针、能谱仪和X射线衍射仪分析了接头的微观组织和界面产物.结果表明,1号钎料所得接头平均抗剪强度最高,为24.1 MPa,其中Ti元素发挥了活性作用而富集在母材两侧的反应层,与Si O2发生反应为Ti+Si O2→Ti Si2+Ti O,伴随反应为Ti+Cu+O→Cu3Ti3O,并有一部分以Cu3Ti的形式块状分布在钎缝中,提高了接头的强度.1号钎料接头产物依次为Si O2→Cu3Ti3O+Ti O+Ti Si2→Ag(s,s)/Cu3Ti/Cu(s,s)→Cu3Ti+Ti O→Mo.     

Al_2O_3陶瓷与TiAl合金真空钎焊接头界面组织及性能

采用AgCuTi活性钎料实现了Al_2O_3陶瓷与TiAl合金的钎焊连接,研究了钎焊接头的界面结构及其形成机制,并且分析了不同钎焊参数对接头界面组织和接头力学性能的影响规律。结果表明:Al_2O_3陶瓷与TiAl合金钎焊接头的典型界面组织为:Al_2O_3/Ti_3(Cu,Al)_3O/Ag(s.s)+Cu(s.s)+AlCu_2Ti/AlCu_2Ti+AlCuTi/TiAl。钎焊过程中,TiAl基体向液态钎料中的溶解量决定了钎焊接头界面组织的形成及其演化。随着钎焊温度的升高和保温时间的延长,Al_2O_3陶瓷侧的Ti_3(Cu,Al)_3O反应层增厚,钎缝中弥散分布的团块状AlCu_2Ti化合物逐渐聚集长大。陶瓷侧界面反应层的厚度和钎缝中AlCu_2Ti化合物的形态及分布共同决定着接头的抗剪强度。当钎焊温度为880℃,保温10 min时,接头的抗剪强度最大,达到94 MPa,此时接头的断裂形式呈现沿Al_2O_3陶瓷基体和界面反应层的复合断裂模式。     

AgCu+nano-Al_2O_3复合钎料钎焊TC4合金与Al_2O_3陶瓷:界面结构及接头性能

通过向Ag Cu共晶钎料中添加nano-Al2O3增强相(2%,质量分数)并采用高能球磨的方法获得了Ag Cu+nano-Al2O3复合钎料(Ag Cu C钎料)。采用Ag Cu C钎料实现了TC4合金与Al2O3陶瓷的高质量钎焊连接,确定了TC4/Ag Cu C/Al2O3钎焊接头的典型界面组织结构为:TC4/α-Ti+Ti2Cu扩散层/Ti3Cu4层/Ag(s,s)+Ti3Cu4+Ti Cu/Ti3Cu4层/Ti3(Cu,Al)3O层/Al2O3。Nano-Al2O3的添加抑制了钎缝中连续的Ti-Cu化合物层的生长,同时在钎缝中形成了颗粒状Ti-Cu化合物相增强的Ag基复合材料,改善了钎焊接头的界面组织。随着钎焊温度的升高,各反应层厚度逐渐增加,颗粒状Ti-Cu化合物不断长大,Ag基复合材料组织逐渐细小。当钎焊温度T=920℃,保温时间t=10 min时接头抗剪强度达到最大为67.8 MPa,典型断口分析表明:压剪过程中,裂纹起源于钎角处并沿钎缝扩展后转入Al2O3陶瓷,最终在Al2O3陶瓷母材侧发生断裂。     

5005铝合金与1Cr18Ni9Ti的真空钎焊分析

采用Al-Si-Mg钎料成功实现了5005铝合金与1Cr18Ni9Ti不锈钢的真空钎焊,借助扫描电镜、能谱分析仪和X射线衍射仪对焊后接头界面组织进行分析,同时对接头抗剪强度进行测试.结果表明,焊后接头界面结构从1Cr18Ni9Ti不锈钢侧到5005铝合金侧的界面组织依次为FeAl,FeAl₃,Fe_mAl_n+αAl.随着钎焊温度的升高或保温时间的延长,接头抗剪强度均呈现先升高后降低的变化趋势.当钎焊温度为580℃,保温时间为15 min时,接头抗剪强度达到最大值49 MPa.接头断裂形式受钎焊温度的影响,当钎焊温度较低时,接头断裂于铝合金侧氧化膜层及Fe_mAl_n+αAl反应层;温度升高至580℃时,接头断裂于Fe_mAl_n+αAl反应层中,接头抗剪强度最高.     

Al_2O_3陶瓷/钢钎焊工艺

陶瓷与金属的连接广泛应用于航空航天、电子、仪器仪表、燃料电池等领域.采用活性钎料Cu70Ti30,Cu75Ti25,Cu80Ti20和Cu85Ti15对Al2O3陶瓷与Q235钢进行了真空钎焊.测量了各试样的抗弯强度和界面区的显微硬度.结果表明,Cu75Ti25是最佳钎料配比,钎焊温度1 100℃,保温时间20 min是最佳的钎焊工艺,该工艺下钎料充分熔化填充接头间隙并与陶瓷和钢侧相互扩散,形成由3层不同组织所构成的界面结合区,即液态钎料填充陶瓷微孔形成的反应层、Ti-Cu合金层以及钢侧扩散层;在界面结合区生成有AlCu4,Cu3TiO4,TiC,TiFe2等新相;界面结合区组织致密、无微孔等缺陷,实现了良好的冶金结合.     

陶瓷基复合材料辅助脉冲电流液相扩散连接的界面反应及接头强化机制

采用Cu-Zr箔/Cu箔/Cu-Zr箔中间层对Ti(C,N)-Al2O3陶瓷基复合材料进行了液相扩散连接实验,研究了辅助脉冲电流对元素扩散、界面反应产物及接头强化机制的影响.结果表明,液相扩散连接过程中辅助脉冲电流条件下可以在较低的焊接温度和较短的焊接时间内实现更高的接头强度.辅助脉冲电流液相扩散连接工艺显著改变了Zr和Cu在Ti(C,N)-Al2O3陶瓷基复合材料和钎缝中的扩散行为,减少Zr的活性,抑制其与Al2O3陶瓷颗粒发生激烈的化学反应.辅助脉冲电流可以抑制陶瓷颗粒相溶解进入焊缝以及界面扩散过渡层和Zr-Cu反应层的厚度,确保焊缝强化以及界面强化,这是辅助脉冲电流液相扩散连接接头具有较高强度水平的关键所在.     

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.     

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.     

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。     

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。     

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.     

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。     

Y2O3-BaO-SiO2-B2O3-Al2O3 glass sealant for solid oxide fuel cells

A glass based on Y₂O₃-BaO-SiO₂-B₂O₃-Al₂O₃ (named YBA) has been investigated as sealant for planar solid oxide fuel cells (SOFCs). The YBA glass has been systematically characterized by differential thermal analysis, dilatometer, scanning electron microscopy, impedance analysis, and open circuit voltage to examine their suitability as sealant. The coefficient of thermal expansion of YBA is 11.64 × 10⁻⁶ K⁻¹ between 323 and 873 K. The resistivity is 9.1 × 10⁴ Ω cm at 800 °C. The glass sealant is found to be well adhered with other cell components, such as electrolytes and stainless steels, at an optimum sealing temperature of 800 °C. All measured results showed that the YBA glass appears to be a promising sealant for SOFCs.     

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.