纳米ZrO2与微米Al2O3复合陶瓷的断裂模式

研究了两种微米Al2O3与纳米ZrO2复合陶瓷的裂纹扩展过程与显微结构的关系.结果表明,Al2O3晶粒内部形成纳米级或亚微米级ZrO2颗粒,是复合陶瓷的断裂模式从沿晶断裂向穿晶断裂转化的主因.ZrO2含量较低有利于Al2O3晶界迁移包裹纳米ZrO2形成内晶结构;而ZrO2含量较高使主晶相长大受到抑止,不利于形成内晶结构,趋向于沿晶断裂.裂纹穿晶扩展需要的驱动力比沿晶断裂大,故裂纹扩展阻力曲线的上升趋势更加显著.裂纹穿晶扩展路径主要取决于内晶颗粒产生的弹性应力场的性质.     

SHS纳米组织Al2O3-ZrO2共晶复相陶瓷断裂力学研究

通过对纳米组织Al2O3-ZrO2共晶复相陶瓷的Vickers压痕测试、SEM观察与XRD分析,发现诱发该复相陶瓷中位裂纹扩展的压痕压制载荷临界值为30kg,复相陶瓷的裂纹扩展主要受晶内型纳米相微观结构所控制,分布于纳米组织Al2O3-ZrO2共晶复相陶瓷中的ZrO2纳米相的结构、含量与分布及ZrO2纳米相与基体相之间的残余应力场决定着该复相陶瓷的断裂力学.     

超重力下燃烧合成大体积凝固态Al2O3/ZrO2（4Y）研究

通过在铝热剂中引入ZrO2(4Y)混合粉末,以超重力下燃烧合成方式,制备出Al2O3/ZrO2(4Y)自生复合陶瓷板材,并研究了复合陶瓷微观结构、生长机理与力学性能.XRD、SEM与EDS结果显示,Al2O3/32%ZrO2(4Y)复合陶瓷基体为亚微米t-ZrO2纤维成三角对称分布其上、取向各异的棒状共晶团,而Al2O3/37%ZrO2(4Y)复合陶瓷则以分布均匀的微米级t-ZrO2球晶为基体.Al2O3/32%ZrO2(4Y)复合陶瓷的强化归因于小尺寸共晶团边界及残余压应力增韧、相变增韧机制引发的高断裂韧性所致;同时,细小t-ZrO2球晶所具有的小尺寸缺陷及相变增韧与微裂纹增韧机制所引发的高断裂韧性也使Al2O3/37%ZrO2(4Y)复合陶瓷得以强化.     

SHS纳米/微米块体复相陶瓷微观结构与断裂

通过在(CrO3 Al)燃烧体系中添加一定量的ZrO2(2Y)粉末,利用SHS冶金技术直接制备出Al2O3-35vol%ZrO2纳米/微米结构块体复相陶瓷,研究该复相陶瓷的微观结构与断裂行为.研究发现:该复相陶瓷基体主要由纳米/微米相晶内型结构共晶体组织构成;Vickers压痕试验显示引发陶瓷裂纹扩展的压痕压制临界载荷为30 kg;ZrO2相所具有的应力诱发相变增韧机制和微裂纹增韧机制均很微弱;裂纹扩展主要受纳米/微米相晶内型结构共晶体控制,使该复相陶瓷在断裂过程中呈现出强烈的裂纹偏转绕过机制.     

烧结温度对20%ZrO_2(3Y)/Al_2O_3复相陶瓷力学性能和微观结构的影响

20%纳米ZrO2(3Y)粉末加入到高纯亚微米Al2O3粉中,采用高压干压成型方法和恒速升温多阶段短保温烧结方法制备出不同烧结温度下的复相陶瓷。研究烧结温度对复相陶瓷力学性能的影响,通过XRD,EDS和SEM对复相陶瓷进行元素组成和微观结构分析。结果表明:烧结温度在很大程度上影响着复相陶瓷的力学性能和微观结构,常压烧结1600℃保温8h时,相对密度、维氏硬度和断裂韧性达到最大,分别为98.6%,18.54GPa和9.3MPa·m1/2,而基体晶粒尺寸为1.4~8.1μm,ZrO2相变量为34.6%。1600℃下复相陶瓷具有优质的微观结构,断裂方式为沿晶-穿晶混合断裂模式。ZrO2(3Y)粉体的加入,从相变增韧、内晶型颗粒增韧和裂纹偏转等多个方面提高了复相陶瓷的断裂韧性。     

Al2O3/SiC纳米复相陶瓷材料的研究进展

Al2O3/SiC纳米复相陶瓷由于具有优异的室温及高温机械性能而成为结构陶瓷领域研究的热点.本文就Al2O3/SiC纳米复相陶瓷的不同制备加工方式及增强增韧机理进行了详细的阐述.其中粉体的均匀混合是制备过程的关键因素,残余应力及裂纹偏转导致的穿晶断裂以及裂纹尖端SiC颗粒的桥联作用是复相陶瓷强度和韧性增加的主导因素.     

ZrO_2增韧Al_2O_3陶瓷的力学性能和增韧机制

对通过热压烧结法制备的3种陶瓷99.5vol%Al2O3(AD995)、ZrO2(15vol%)/Al2O3和ZrO2(25vol%)/Al2O3的力学性能和增韧机制进行了实验和理论研究。基于复合材料细观力学理论并考虑ZrO2的相变特性,建立了描述ZrO2/Al2O3陶瓷力学性能的本构模型。结果表明:ZrO2的加入细化了基体Al2O3晶粒,ZrO2/Al2O3陶瓷的致密性得到提高;3种陶瓷试件的破坏呈现小变形到脆性破坏的特点,压缩加载下试件应力-应变曲线近似为线性关系;AD995陶瓷的断裂韧性为5.65 MPa·m1/2,ZrO2(25vol%)/Al2O3陶瓷的断裂韧性为8.42 MPa·m1/2,提高了近50%;随ZrO2增韧相含量的增加,ZrO2/Al2O3陶瓷的弹性模量降低而断裂韧性增加,这一变化趋势与实验结果有良好的一致性。     

Al2O3/ZrO2层状复合陶瓷的显微结构特征与强韧化的关系

利用自带能谱的扫描电镜(SEM)和透射电镜(TEM)仪,对Al2O3/ZrO2层状复合陶瓷的显微结构特征及断口形貌进行深入分析研究.研究结果表明:表面压应力的作用细化了晶粒,提高了可相变四方相的含量,增加了相变增韧的效果;沿界面两端表现出2种不同的断裂机制:界面以外靠近表面部分,其断裂主要是穿晶断裂;在基体层的断裂则表现为沿晶和穿晶混合型断裂方式.该断裂行为与ZrO2层状陶瓷的相变增韧机制密切相关.     

Al_2O_3-ZrO_2/W/Cr/Ni/Co金属陶瓷的断裂韧性

以Al2O3-ZrO2复合粉末、W、Cr、Ni、Co粉末为原料,采用热压烧结工艺制备了性能优良的Al2O3-ZrO2/W/Cr/Ni/Co金属陶瓷复合材料。通过SEM,EDS,XRD等手段分析其微观组织,单边梁开口法(SENB)测量其断裂韧性。实验结果表明在1320℃,20MPa条件下热压烧结制备的Al2O3-ZrO2/W/Cr/Ni/Co金属陶瓷的断裂韧性为7.16±0.4MPa.m1/2,硬度为83.3HRA,横向断裂强度为540MPa,相对致密度为97.4%;对维氏压痕下裂纹扩展进行了分析,其增韧机理为延性金属对裂纹的桥梁作用和氧化锆相变增韧,在裂纹通过时硬质相以沿晶断裂为主。     

ZrO2/SiC-WSi2/MoSi2纳米复相陶瓷制备及增韧机制探讨

利用扫描电镜、图像分析仪以及X射线衍射仪研究了ZrO2/SiC-WSi2/MoSi2复合粉末的分散、热压试样结构、组织以及断口形貌和断裂韧性之间的相互关系.研究表明:综合利用球磨、酒精清洗、超声波振荡能很好地实现纳米/微米颗粒的分散,团聚现象较轻.SiC,Zro2纳米颗粒的协同复合化以及W的合金化能使复相陶瓷晶粒细化,增韧效果明显,断裂韧性可达8.13 MPa·m1/2,断口呈现出以沿晶为主、穿晶为辅的混合断裂特征.复相陶瓷的增韧主要是通过晶粒细化、裂纹偏转、微裂纹形成、桥联等机制的综合作用.     

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.     

Superconductivity of barium-doped Bi2Sr2CaCu2Oy

Sintered ceramic samples of Bi₂Sr_2–x Ba _x CaCu₂O_y with nominal barium fraction 0x0.3 have been prepared by the solid-state reaction method. WDS studies verified that barium enters the superconducting phase. For slowly cooled samples, the midpointT _c of the superconducting transition is significantly increased by barium doping, whereas for quenched samplesT _c is little affected. The increase ofT _c with increasing barium fraction is consistent with a decrease in the hole concentration in the superconducting layers.     

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.     

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。     

Reactivity of the H2O2/TiO2 system

The reactivity of the H₂O₂/TiO₂ system for samples treated at atmospheric pressure is studied by means of Auger Electron Spectroscopy. The most significant changes on the TiO₂ ‘final’ state are: (i) The I(O)/I(Ti) peak-to-peak ratio is diminished by 15%. (ii) The LMV transition suffers an energy shift of +2 eV, whereas the peak-to-peak width diminishes 1.5 eV. (iii) Its structure changes with respect to that of the TiO₂ ‘initial’ state although it is not identified with any one of the known stoichiometric oxides. (iv) When the samples that represent the ‘final’ state are heated up to 650 K, the AES spectrum matches quite well that of the TiO₂ ‘initial’ state.     

Ti/SnO2+Sb2O3+MnO2/PbO2阳极的性能研究

制备了一种非贵金属阳极－Ｔi/SnO2 Sb2O3 MnO2/PbO2,并用ＸＲＤ、ＳＥＭ进行了表征,计算出了电极的分形维数,测定了该电极在硫酸中的使用寿命和动力学参数,把该电极用于处理含酚废水和Ｐb电极进行对,结果表明,节电３３％,转化率达９５％,是一种优良的电化学催化剂。     

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.     

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．     

Natural and persistent superhydrophilicity of SiO2/TiO2 and TiO2/SiO2 bi-layer films

Sol-gel SiO₂/TiO₂ and TiO₂/SiO₂ bi-layer films have been deposited from a polymeric SiO₂ solution and either a polymeric TiO₂ mother solution (MS) or a derived TiO₂ crystalline suspension (CS). The chemical and structural properties of MS and CS bi-layer films heat-treated at 500 °C have been investigated by Fourier transform infrared spectroscopy, X-ray photoelectron spectroscopy, and transmission electron microscospy. Water contact angle measurements show that MS SiO₂/TiO₂ and CS TiO₂/SiO₂ bi-layer films exhibit a natural superhydrophilicity, but cannot maintain a zero contact angle for a long time over film aging. In contrast, CS SiO₂/TiO₂ bi-layer films exhibit a natural, persistent, and regenerable superhydrophilicity without the need of UV light. Superhydrophilic properties of bi-layer films are discussed with respect to the nature of the TiO₂ single-layer component and arrangement of the bi-layer structure, i.e. TiO₂ underlayer or overlayer.     

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.