Cr_2O_3-8%TiO_2等离子喷涂层结合强度、表面状态与喷涂层厚度的关系

以往,有关等离子喷涂CrO3-8%TiO2涂层厚度与涂层性能关系的报道较少,为此,通过优化工艺参数,在45钢表面等离子喷涂不同厚度(350,450,550μm)的Cr2O3-8%TiO2涂层,研究了涂层厚度与其结合强度、硬度和孔隙率之间的关系。涂层厚度为350,450,550μm时,结合强度分别为29.2,11.5,7.2MPa,显微硬度分别为2528,2190,1930HV;孔隙率分别为3.80%,3.95%,4.45%。结果表明,随Cr2O3-8%TiO2喷涂层厚度的增加,涂层的结合强度减小,孔隙率增加,造成显微硬度降低。     

粉末粒度对等离子喷涂Al2O3-13%TiO2陶瓷涂层组织结构及性能的影响

等离子喷涂粉末的粒度影响涂层组织结构与性能。选用4种不同粒度的Al2O3-13%TiO2(AT13)粉末等离子喷涂陶瓷涂层,研究了喷涂粉末粒度对涂层组织结构、孔隙率、显微硬度和沉积效率的影响。结果表明:采用较细的喷涂粉末制备的AT13涂层致密、均匀,孔隙率低;随着喷涂粉末粒度增大,涂层的孔隙率增加,显微硬度降低,沉积效率先增后减;采用粒度为38～44μm的粉末喷涂涂层时沉积效率最高,达到51%,涂层组织也较致密,这是等离子喷涂AT13陶瓷层较理想的粒度。     

等离子喷涂纳米Al2O3-13wt% TiO2涂层组织与性能的双态分布特性研究（英文）

采用由喷雾造粒制备的纳米团聚粉末并通过等离子喷涂制备出纳米Al2O3-13wt%TiO2涂层.研究分析了涂层的相组成、显微结构、硬度及断裂韧性,结果发现,该纳米涂层呈现出由两部分不同区域组成的双态分布结构:一部分为完全熔化后凝固形成的层状结构;另一部分则为部分熔化的粒状结构,其内保留来源于喷涂喂料的纳米或亚微米粒子.涂层中与未熔纳米α-Al2O3粒子含量成比例的部分熔化区百分数可以通过调整关键喷涂工艺参数(CPSP)来控制.纳米涂层所具有的这种混合结构特性,可以被其力学性能的双态分布特征所证实.Weibull统计分析表明,涂层的显微硬度和断裂韧性均呈现出双态分布,部分熔化区的显微硬度及其分散性均比完全熔化区低,而其断裂韧性及其分散性则均比完全熔化区高.     

等离子喷涂Al_2O_3-40%TiO_2陶瓷复合层的微观结构及耐磨性能

为了探讨不同功率下6063铝合金表面等离子喷涂Al2O3-40%TiO2陶瓷复合层的形貌、组构及其耐磨性能,利用X射线衍射仪(XRD)、扫描电镜(SEM)、显微硬度计和摩擦磨损试验机进行了相关研究。结果表明:微米级Al2O3-40%TiO2粉末经过等离子喷涂可以获得弥散分布的纳米级颗粒的陶瓷复合涂层,涂层硬度在1 000 HV以上;当喷涂功率为25～33 kW时,涂层硬度和耐磨性能随喷涂功率的升高而降低。     

不同Al2O3-TiO2-Cr2O3-SiO2配比等离子喷涂层的耐磨粒磨损性能

为了探讨等离子喷涂制备Al2O3-TiO2-Cr2O3-SiO2层的可行性及其喷涂层的耐磨性,采用等离子喷涂在Q235钢表面分别制备了54%Al2O3-36%TiO2-10%Cr2O3-0.5%SiO2,42%Al2O3-28%TiO2-28.5%Cr2O3-1.5%SiO2和30%Al2O3-20%TiO2-47.5%Cr2O3-2.5%SiO23种陶瓷层,分析了陶瓷涂层的金相显微形貌、显微硬度及耐磨粒磨损性能,并分析了其耐磨粒磨损的机理。结果表明:3种涂层的显微硬度分布均具有梯度分布特性,Al2O3+Cr2O3硬质相含量越高,涂层硬度越大;30%Al2O3-20%TiO2-47.5%Cr2O3-2.5%SiO2喷涂粉制成的涂层的硬度最大,耐磨粒磨损性能最佳。     

正交试验设计优化等离子喷涂纳米Al2O3-13%TiO2涂层工艺参数

为了深入研究等离子喷涂纳米Al2O3-13%TiO2(质量分数)工艺参数与涂层性能之间的关系,采用正交试验设计法,针对等离子喷涂过程中喷涂距离、喷涂电流、主气压力及辅气压力等4个主要参数,选用L9(34)正交表,以涂层结合强度为指标开展制备工艺参数的优化。结果表明,影响涂层结合强度的因素主次顺序是喷涂电流、喷涂距离、主气压力、辅气压力;等离子喷涂纳米Al2O3-13%TiO2最佳工艺参数为:喷涂距离110mm,喷涂电流870A,主气压力0.31MPa,辅气压力0.97MPa,优化工艺喷涂的涂层结合强度达到31.5MPa。     

纳米陶瓷等离子喷涂层硬度的Weibull分布及与涂层组构的对应特性

等离子喷涂层的硬度是反映其耐磨性、强度、使用寿命的重要指标,它与涂层的组构有对应的关系,但其测定结果分散性较大。为了精确测量陶瓷等离子喷涂层的硬度,在NiCrAl合金表面等离子喷涂制备了Al2O3-13%TiO2(AT13)纳米陶瓷涂层(ncc)和对照用微米涂层(mcc),采用显微硬度测试仪测量了其显微硬度,研究了其Weibull分布特性,通过SEM、XRD等分析了ncc涂层显微硬度与微观组织结构的关系,并通过TEM对涂层的微区结构进行了表征。结果表明:ncc涂层的平均显微硬度显著高于mcc,且呈双态分布;两者硬度的Weibull分布呈分散性,但ncc涂层的分布较均匀,微裂纹细小且粒径小,以α-Al2O3和γ-Al2O3及少量金红石型TiO2为主要物相;ncc涂层具有优异的力学性能主要归因于其组织的晶粒细化、纳米TiO2颗粒镶嵌于Al2O3孔隙中、Al2O3微晶弥散分布、微裂纹韧化等。     

常规和纳米陶瓷等离子喷涂层抗冲蚀性能的对比

纳米陶瓷具有高韧性和超塑性等独特的性能,用于制备涂层可极大地提高其耐冲蚀性能.以常规和纳米团聚体Al2O3-13%TiO2(质量分数)陶瓷粉末为原料,采用等离子喷涂工艺在TiAl合金表面制备了2种陶瓷涂层.比较了2种涂层的微观结构、结合强度和抗冲蚀性能,探讨了涂层的冲蚀破坏机理.结果表明:常规涂层呈典型的层状堆积特征,...     

等离子喷涂纳米Al_2O_3-8%TiO_2复合陶瓷涂层组织与性能研究

采用液相喷雾造粒+烧结的方法制备了适合等离子喷涂用的Al2O3-8%TiO2(质量分数)复合粉末,并利用等离子喷涂技术制备了具有纳米结构的复合陶瓷涂层。利用SEM、XRD、TEM和数字显微硬度计等对涂层的微观结构和力学性能进行了检测和分析。结果表明,所制备的涂层是完全熔化区和部分熔化区共存的双态分布结构,其显微硬度和断裂韧性都比较高;涂层的磨损体积损失量随施加载荷增大而增大。     

HEPJet等离子喷涂Al2O3性能试验研究

研究了新开发的高效能超音速等离子喷涂系统(HEPJet-High Efficiency Plasma Jet)的射流特性,及所制备的Al2O3陶瓷涂层的结合强度、显微硬度和孔隙率等性能以及显微结构,并与一种普通等离子喷涂系统进行了对比试验研究.结果表明,HEPJet系统制备Al2O3涂层的性能及显微结构明显优于普通等离子喷涂的Al2O3涂层.     

MgO-Al2O3-SiO2-TiO2-Y2O3玻璃的弹性模量

根据硬盘基板用材料的要求，制备了MgO-Al2O3-SiO2-TiO2-Y2O3高弹性模量玻璃（120GPa)，玻璃的弹性模量随组成的变化服从Makishima-Mackenzie理论，MgO,Al2O3,TiO2,Y2O3等具有较高单位体积离解能的氧化物有利于提高玻璃的弹性模量，但玻璃弹性模量的理论计算值低于测试值，这是因为Makishima-Mackenzie理论没有考虑玻璃内阳离子的具体配位，对MgO,Y2O3堆积密度因子的堆导存在误差，因此利用Makishima-Mackenzie理论发展高弹性模量玻璃时应对MgO,Y2O3等氧化物的计算进行修正。     

Les phases SrLa2Al2O7 et SrGd2Al2O7

SrLa₂Al₂O₇ and SrGd₂Al₂O₇ belong to the structural type Sr₃Ti₂O₇. In SrGd₂Al₂O₇ strontium and gadolinium occupy respectively the 12 and 9 coordinated sites, whereas in SrLa₂Al₂O₇ the homologous cations are statistically distributed. The fluorescence spectra of both phases activated by Eu³⁺ ions show that the only possible position of Eu³⁺ is the 9 coordinated site.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper and the planar oxygen 2p atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

La2O3在MgO-Al2O3-SiO2-TiO2微晶玻璃中的作用

在MgO-Al2O3-SiO2-TiO2玻璃中添加不同数量的氧化镧，采用差热分析，X射线衍射及电子显微镜等技术研究了氧化镧对玻璃析晶过程与力学性能的影响。氧化镧的加入使玻璃中析出α－堇青石相的温度降低，同时避免了高膨胀方石英相的析出。随着氧化镧加入量的增加，玻璃整体析晶能力下降，微晶玻璃中晶相含量减少，晶粒尺寸增大，微晶玻璃的弹性模量与硬度减小，断裂韧性增加，体现出大尺寸长柱状金红石晶粒的增韧作用。     

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.     

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.     

Na2O-B2O3-SiO2-SnO2系统的分相与析晶

对Na2O-B2O3-SiO2-SnO2四元系统的分相与析晶进行了探讨．通过对不同组成点在热处理、化学处理各阶段的试样进行能谱分析、XRD分析及SEM分析，确认了SnO2分布在分相结构中的富硼碱相中；在该系统中SnO2晶体的析出有赖于分相过程；分相结构尺度限制了SnO2的析晶尺寸．试验结果表明，通过控制分相结构得到了负载于多孔富硅载体的纳米尺寸的SnO2材料．该材料具有较高的CO氧化催化活性．     

Quasiparticle dispersion of Sr2CuO2Cl2

Recent angle resolved photoemission (ARPES) measurements for the insulating cuprate Sr₂CuO₂Cl₂ have provided the first experimental data which can be directly compared to the (theoretically) well-studied problem of a single hole propagating in an antiferromagnet. Some discrepancies withthe familiar 2D t— J model were observed. Here we discuss a comparison between the ARPES results and the quasiparticle dispersion of both (i) the extended t— t— J Hamiltonian and (ii) the three-band Hubbard model.     

High-pressure substitutions for Cd In Cd2Nb2O7 and Cd2Ta2O7

Substitutions into cadmium niobate of the type Cd_2?xA_xNb₂O₇ (x≤0.5) have been carried out at 58 kbars and 1100°C. The substituting A cations were Mg, Mn, Fe, Co, Ni, Cu, and Zn which are all smaller than Cd. Rhombohedral or triclinic distortions derived from cubic Cd₂Nb₂O₇ were achieved at values of x as low as 0.05. All the substituted phases appear to be centric at room temperature. Analogous substitutions into Cd₂Ta₂O₇ were also made.