基于添加铜过渡层的钛钢异种金属真空扩散焊研究

研究了添加铜箔过渡层进行扩散焊接的纯钛TA2和14MnMoVN钢焊接接头的组织和性能。采用OM、扫描电镜、能谱分析和X射线衍射分析对扩散焊接界面的微观组织、元素扩散和组织结构进行分析观察,通过拉伸试验对接头力学性能进行测试。结果表明:通过添加铜过渡层进行扩散焊接可以获得有效连接的钛/钢异种金属复合接头。结合良好的界面可以划分为接头元素扩散过渡区和铜钛结合区。其中钛向铜扩散,少量铁向铜扩散,这是三种元素的综合扩散过渡区。铜钛结合区是铜向钛扩散的区域,主要产生大量的铜钛金属间化合物。接头拉伸强度可以达到299 MPa,断裂位置位于铜钢结合区。     

国内外SUPER304H钢焊接接头热影响区的组织对比

国内某钢厂生产的SUPER304H钢的焊接接头热影响区部分区域晶粒粗大,而国外同类产品的焊接接头热影响区晶粒则均匀细小。对国内外不同厂家生产的该钢种的焊接接头热影响区进行了金相、电镜及电子探针的检测分析,在国外产品的热影响区发现大量Cr23C6相析出,这种析出相阻碍了二次热循环时热影响区晶粒的长大,但同时会导致抗腐蚀性能变差。Cr23C6相的析出主要是因为钢材化学成分和焊接工艺的区别造成的。     

铝合金搅拌摩擦对接焊接头组织与性能研究

研究了5083铝合金搅拌摩擦焊(FSW)焊接接头组织与性能,采用金相显微镜观察焊接接头各区域的微观组织,并对接头显微硬度和力学性能进行了测定。结果表明,5083铝合金搅拌摩擦焊焊核组织为动态再结晶生成的细小组织,强化相均匀分布;热机影响区由于动态再结晶和焊接热循环的双重作用,组织变化较大,晶粒有一定程度的长大,强化相有所细化;热影响区仅仅受到热循环作用,使得晶粒粗化和强化相出现聚集现象。搅拌摩擦焊接接头中心硬度与母材基本相当,热机影响区和热影响区由于焊接热输入的原因,使得硬度有所降低。搅拌摩擦焊室温拉伸性能和冲击性能不低于母材的,其中拉伸试样均断裂于母材,焊核室温冲击值达到母材的1.5倍以上,热影响区冲击值与母材的相当。     

紫铜-碳钢磁脉冲焊接接头界面形貌研究

为探索紫铜-碳钢磁脉冲焊接(MPW)接头界面形貌等微观特征,本文进行了T2紫铜管和50#钢管的磁脉冲焊接试验,在电压11 k V、径向间隙2.2 mm、重叠面积比3/4的条件下,获得了T2铜管-50#钢管冶金连接接头.通过光学金相、SEM/EDS、显微硬度和纳米压痕试验,重点研究了接头界面形貌、基体元素扩散和硬度分布.结果表明:接头由未焊合区、波状界面结合区、平直界面结合区等特征区域构成,连接区长度达到5 mm;波状结合区界面波长约为60μm,波峰幅值高约20μm;平直界面结合区基体元素扩散区(过渡区)宽度约2μm,而在波状界面结合区,扩散区宽度可达6μm;接头铜侧硬度相对初始值提高50%,最高硬度值出现在靠近界面的50号钢侧,而界面硬度介于两种母材之间.     

铜/钢异种材料等离子弧焊接头显微组织分析

为实现铜/钢异种材料的优质连接,研究了铜/钢焊接接头的显微组织特点及其组成,试验采用LHM-200等离子弧焊系统对紫铜(T2)与不锈钢(304)异种材料进行焊接,然后通过光学金相显微镜及能谱分析仪,观察分析接头显微组织,研究其接头组织结构及组成.研究结果表明:铜/钢异种材料的等离子弧焊焊缝在铜一侧为平直的,而在钢一侧则为半χ型,在铜侧界面形成漩涡状;在焊接接头的形成过程中铜元素的迁移和扩散主要依靠钢液的流动所带动;焊接接头显微组织主要为奥氏体组织,弥散分布着块状和粒状的铜和钢的固溶体组织,和黑色鱼骨状的α相铁素体组织;焊缝区组织主要是以α、γ富铁相和ε富铜相固溶体组织的形式存在.通过实现发现最佳的焊接参数为:保护气流量与离子气流量分别为0.25 L/min和0.75 L/min,焊接电流为65 A,焊接速度为4 mm/s,焊接后的接头抗拉强度能达到174 MPa.     

钼铜扩散焊接接头界面显微组织

采用扩散焊接方法对钼铜异种材料进行了焊接,研究了直接焊接和加镍作为中间层焊接对焊接接头界面显微组织的影响,通过SEM、EDS、EPMA、XRD等测试方法对其显微结构进行了表征.结果表明,直接焊接时,焊接界面结合紧密,Mo、Cu原子之间相互扩散形成扩散层,接头断裂发生在扩散层,由于柯肯达尔效应作用,在铜侧形成少量孔洞,孔洞的存在使焊接接头性能降低;加镍中间层焊接时,接头抗拉强度高于直接焊接时抗拉强度,Mo/Ni和Ni/Cu界面结合紧密,Mo/Ni界面形成固溶体层,接头断裂发生在Mo/Ni界面处,断口呈典型的脆性断裂特征.     

紫铜/Al_2O_3陶瓷/不锈钢复合结构钎焊接头残余应力研究

采用有限元数值模拟的方法研究AgCuTi钎焊紫铜/Al_2O_3陶瓷/不锈钢复合结构的形变和残余应力分布情况,并对模拟结果进行实验验证。结果表明:残余应力主要分布在接头区,并且该区形变较小。陶瓷端的残余应力对接头性能影响较大,由于线膨胀系数差异过大,不锈钢陶瓷侧易产生裂纹缺陷,接头倾向于在该区域断裂,紫铜侧陶瓷端TiO反应层的形成导致该区域裂纹的出现,降低了接头的性能。研究各应力分量对最终残余应力的贡献,结果显示环向应力和轴向应力在陶瓷端所产生的拉应力是造成接头强度降低的主要因素。接头拉剪实验表明,接头主要在靠近不锈钢侧的陶瓷端断裂,验证了模拟结果的准确性。     

扩散焊条件下Al2O3P/6061Al复合材料中氧化膜的行为

研究了Ａｌ２Ｏ３ｐ／６０６１Ａｌ铝基复合材料扩散焊接头区域氧化膜随焊接温度变化的规律,分析了氧化膜的变化机理,探讨了氧化膜对接头强度的影响。结果表明,在扩散焊时,随焊接规范的变化Ａｌ２Ｏ３ｐ／６０６１Ａｌ铝基复合材料接头区域的氧化膜含量及形态有明显的改变,这与Ｍｇ＋４／３Ａｌ２Ｏ３→Ａｌ２ＭｇＯ４＋２／３Ａｌ反应有关,氧化膜的变化直接影响着焊缝的接头强度。     

柱形光头搅拌针搅拌摩擦焊接铝锂合金接头组织及力学性能

采用柱形光头搅拌针搅拌摩擦焊接5mm厚的铝锂合金轧制板,并对接头组织和力学性能进行了分析.焊后接头形成了三个组织差异明显的区域:焊核区,热机影响区和热影响区.焊核区微观组织呈鱼鳞状;热影响区组织在焊接热循环作用下,发生回复反应,形成棒状的回复晶粒;前进侧和后退侧热机影响区内为颗粒较大的等轴晶晶粒,且后退侧晶粒尺寸大于前进侧.力学性能测试结果表明,焊接速度υ＝40mm/min时,接头获得最高拉伸强度(296MPa);焊接速度υ＝80mm/min时,接头获得最大延伸率(8.6%).硬度测试结果表明,焊缝区发生了软化,前进侧和后退侧材料的软化区间大致相同,但后退侧软化程度高于前进侧.     

采用Ag-Cu-Ti钎料真空钎焊SiO2f/SiO2复合陶瓷与C/C复合材料

分别在880℃/10min和880℃/60min规范下,采用Ag-Cu-Ti活性钎料实现了SiO2f/SiO2复合陶瓷与C/C复合材料的真空钎焊连接,通过电子探针(EPMA)、能谱仪(XEDS)和X射线衍射仪(XRD)分析了接头微观组织,室温下测试了接头的抗剪强度。结果表明:两种规范下所得接头界面结合良好,接头中靠近两侧母材均形成了一层扩散反应层,钎缝基体主要由均匀的共晶组织组成。880℃/10min规范下钎焊接头界面产物依次为:SiO2f/SiO2→Ti4O7→Ti5Si4+Cu(s,s)+Ag-Cu共晶合金→TiC→C/C;对于880℃/60min规范下的接头,界面组织结构与保温10min的接头基本类似,但是不存在Cu(s,s),并且接头反应层明显增厚。880℃/60min条件下所得钎焊接头剪切强度平均值为16.6MPa。     

Subsolidus phase equilibria and the Li5Nd4FeO10 phase in the Li2O-Nd2O3-Fe2O3 system

A survey of the subsolidus phase equilibria in the system Li₂O-Nd₂O₃-Fe₂O₃ was made at subsolidus temperatures in the range 1000-1050 °C. A ternary phase was identified. The phase is centered on Li₅Nd₄FeO₁₀, with a cubic lattice a = 11.9494 Å. The compound melts incongruently at 1105 °C. The magnetic susceptibility was measured in the temperature range 4-300 K. The compound is paramagnetic in the temperature range 150-300 K and follows the Curie-Weiss law. At about T_N = 10 K, a long-range magnetic ordering is observed.     

Nanocrystallization of SrBi2Nb2O9 from glasses in the system Li2B4O7---SrO---Bi2O3---Nb2O5

Transparent glasses in the system (100−x)Li₂B₄O₇–x(SrO---Bi₂O₃---Nb₂O₅) (10≤x≤60) (in molar ratio) were fabricated by a conventional melt-quenching technique. Amorphous and glassy characteristics of the as-quenched samples were established via X-ray powder diffraction (XRD) and differential thermal analyses (DTA) respectively. Glass–ceramics embedded with strontium bismuth niobate, SrBi₂Nb₂O₉ (SBN) nanocrystals were produced by heat-treating the as-quenched glasses at temperatures higher than 500 °C. Perovskite SBN phase formation through an intermediate fluorite phase in the glass matrix was confirmed by XRD and transmission electron microscopy (TEM). Infrared and Raman spectroscopic studies corroborate the observation of fluorite phase formation. The dielectric constant (_r) and the loss factor (D) for the lithium borate, Li₂B₄O₇ (LBO) glass comprising randomly oriented SBN nanocrystals were determined and compared with those predicted based on the various dielectric mixture rule formalism. The dielectric constant was found to increase with increasing SBN content in LBO glass matrix.     

Vapour-liquid equilibria in the ternary mixtures N2---CH4---C2H6 and N2---C2H6---C3H8

A systematic study was performed with mixtures consisting of N₂, CH₄, C₂H₆ and C₃H₈, to investigate experimentally phase equilibria and caloric properties and to test the accuracy of thermodynamic correlations. The first part of this Paper reports results of T---p---x---y measurements on ternary systems in the range 20 < p < 120 bar and 140 < T < 220 K. The results are compared with data calculated by generalized equations of state.     

PbSbBiS4-Sb2S3 and PbSbBiS4-Bi2S3 joins in the PbS-Sb2S3-Bi2S3 system

Phase equilibria along the PbSbBiS₄-Sb₂S₃ and PbSbBiS₄-Bi₂S₃ joins of the PbS-Sb₂S₃-Bi₂S₃ system have been studied for the first time using differential thermal analysis, X-ray diffraction, microstructural analysis, microhardness tests, and density measurements, and the phase diagrams of the joins have been mapped out. The joins are shown to be pseudobinary with limited series of terminal solid solutions. The solid solutions are p-type semiconductors.     

Magnetic properties of quaternary compounds on the Cu2GeSe3-Cr2Se3 join of the Cu2Se-GeSe2-Cr2Se3 system

We have synthesized two quaternary compounds, Cu₂GeCr₄Se₉ and Cu₂GeCr₆Se₁₂, with compositions on the Cu₂GeSe₃-Cr₂Se₃ join of the Cu₂Se-GeSe₂-Cr₂Se₃ system. Their composition stability limits and the lattice parameters of Cu₂GeCr₄Se₉ have been determined, and their magnetic properties (magnetic moments, temperatures and types of magnetic transitions) have been investigated. Ferromagnetic samples with Curie temperatures from 95 to 135 K have been identified in the homogeneity ranges of the two compounds. Original Russian Text ? T.G. Aminov, G.G. Shabunina, E.V. Busheva, 2009, published in Neorganicheskie Materialy, 2009, Vol. 45, No. 3, pp. 283–287.     

The effect of Bi1.5Zn0.5Nb0.5Ti1.5O7 cover layer on the dielectric and tunable properties of Ba0.6Sr0.4TiO3/Bi1.5Zn0.5Nb0.5Ti1.5O7 bilayered thin films

Bi_1.5Zn_0.5Nb_0.5Ti_1.5O₇ (BZNT) thin films with different thicknesses as cover layers were deposited on the Ba_0.6Sr_0.4TiO₃ (BST) thin films on the Pt/Ti/SiO₂/Si substrates by radio frequency magnetron sputtering method. The microstructure, surface morphology, dielectric and tunable properties of BST/BZNT heterogeneous bilayered films were investigated as a function of the thickness of BZNT films and the effect of BZNT films on the asymmetric electrical properties of BST/BZNT bilayered films was discussed. It was found that BZNT cover layer significantly improved the leakage current and the dielectric loss, and the dielectric constant and tunability of BST/BZNT bilayered thin films simultaneously decreased with the increasing thickness of BZNT films. The BST/BZNT bilayered thin film with a 50 nm BZNT cover layer gave the largest figure of merit (FOM) of 33.48 with the upper tunability of 55.38%. The asymmetric electrical behavior of BST/BZNT bilayered films is probably related to an internal electric field caused by built-in voltages at Pt/BST and BZNT/Au interfaces.     

Phase relations of the Li2O-Ta2O5-B2O3 and Li2O-WO3-B2O3 systems and promising nonlinear optical compounds in K2O-Ta2O5-B2O3 system

The subsolidus phase equilibria of the Li₂O-Ta₂O₅-B₂O₃, K₂O-Ta₂O₅-B₂O₃ and Li₂O-WO₃-B₂O₃ systems have been investigated mainly by means of the powder X-ray diffraction method. Two ternary compounds, KTaB₂O₆ and K₃Ta₃B₂O₁₂ were confirmed in the system K₂O-Ta₂O₅-B₂O₃. Crystal structure of compound KTaB₂O₆ has been refined from X-ray powder diffraction data using the Rietveld method. The compound crystallizes in the orthorhombic, space group Pmn2₁ (No. 31), with lattice parameters a = 7.3253(4) Å, b = 3.8402(2) Å, c = 9.3040(5) Å, z = 2 and D_calc = 4.283 g/cm³. The powder second harmonic generation (SHG) coefficients of KTaB₂O₆ and K₃Ta₃B₂O₁₂ were five times and two times as large as that of KH₂PO₄ (KDP), respectively.     

Subsolidus phase equilibria in the Al2O3-CeO2-PbO and Al2O3-CeO2-RuO2 systems

The subsolidus phase equilibria in air for the Al₂O₃-CeO₂-PbO and Al₂O₃-CeO₂-RuO₂ systems were studied with the aim of obtaining information on possible interactions between a CeO₂-based solid electrolyte in solid-oxide fuel cells (SOFCs) and other oxides. No ternary compound was found in either of the systems. The tie line in the Al₂O₃-PbO-CeO₂ system is between Al₂Pb₂O₅ and the CeO₂.     

Radio-frequency properties of La0.6Sr0.2Mn1.2O3 and La0.65Sr0.28Mn1.07O3 ceramics near the Curie temperature

Radio-frequency magnetic and dissipative properties of La_0.6Sr_0.2Mn_1.2O₃ and La_0.65Sr_0.28Mn_1.07O₃ ceramics have been studied in the region of their Curie points. It is established that, despite relatively high conductivity in the frequency range f=1–15 MHz, the screening of samples by the skin current is negligibly small and the ceramic samples behave like strong ferromagnets. This behavior is explained by significant differences in the propagation of electromagnetic field in inhomogeneous granular ferromagnetic media and normal metals. The field dependence of the effective magnetic susceptibility of both manganites has been studied at room temperature.     

Magnetic coupling in La0.67Ca0.33MnO3/La0.67Sr0.33CoO3/La0.67Ca0.33MnO3 sandwiches

La_0.67Ca_0.33MnO₃ (LCMO)/La_0.67Sr_0.33CoO₃ (LSCO)/LCMO trilayer films are fabricated on single-crystal substrates NdGaO₃ (110) and the interlayer coupling are investigated. Compared with LCMO single layer, sandwiches showed the enhanced metal-insulator transition temperature of LCMO layers. The magnetoresistance is dependent on spacer thickness and the peak value dramatically decreases when LSCO layer is thick enough because of shorting by the LSCO layer. The magnetic coercivity H_C shows a nonmonotonic behavior with changing spacer layer thickness and the waist-like hysteresis indicates that there is an indirect exchange coupling between the top and bottom LCMO layers across the spacer layer.