TiN-Al2O3纳米复合材料的力学性能和导电性能

以纳米TiN和α-Al₂O₃粉体为原料,采用球磨混合法制备了纳米TiN-Al₂O₃复合粉体,通过热压烧结得到致密烧结体.研究了纳米TiN颗粒对Al₂O₃材料力学性能和导电性能的影响,实验结果表明:在Al₂O₃基体中加入15vol％TiN纳米颗粒时,Al₂O₃材料的弯曲强度和断裂韧性分别从370MPa和3.4MPa·m^1/2提高到690MPa和5.1MPa·m^1/2,随着TiN添加量的增加,复合材料的电阻率逐渐降低,在25vol％TiN时达到最低值(6.5×10^-3Ω·cm).     

Al2O3-ZrO2(3Y)-SiC纳米复合材料的制备及性能

本文研究了非均相沉淀法制备Al2O3－ZrO2（3Y）－SiC复合粉体的工艺过程,认为粉体的理烧温度是至关重要的,热压烧结得到了致密的Al2O3－ZrO2（3Y）－SiC纳米复合材料,ZrO2的加入对烧结温度的影响不大．通过TEM观察,SiC颗粒均匀分散于材料中,大的ZrO2颗粒位于Al2O3晶粒间,小的圆形ZrO2颗粒位于Al2O3晶粒内,一部分Al2O3晶粒呈非等轴状．80Wt％Al2O3－15wt％ZrO2－5Wt％SiC纳米复合材料的抗弯强度可达555MPa,韧性为3.8MPa．m1／2.     

高能球磨结合SPS技术制备Al2O3-TiC复合材料及其性能研究

以TiO2、Al、C(石墨)为原料,首先采用高能球磨引导铝热反应合成了Al2O3-TiC纳米复合粉体,然后采用放电等离子体烧结纳米复合粉体制备了Al2O3-TiC复合材料.结果表明,在氩气氛围下高能球磨3h后,原料粉末就发生了铝热反应,合成的Al2O3-TiC复合粉体粒子尺寸大约在100nm左右.采用SPS技术在1450℃保温4min烧结的试样致密度达99.6%,并且结构精细(大部分晶粒＜1μm),两相分布比较均匀,有较好的力学性能和电导性能,抗弯强度为650+21MPa,硬度为19.1±0.2GPa,断裂韧性为4.5±0.2MPa·m1/2,电导率为2.3828×105Ω-1.m-1.     

YAG-Al2O3纳米复合材料的制备和力学性能

本文介绍用化学共沉淀和在适当温度下煅烧以直接制备YAG-Al2 O3纳米复合粉体的新方法．XRD结果表明,所得粉体具纯的YAG和α-Al2 O3相,因此其化学组成符合配料的组分设计．用本方法制备的25vol％YAG-Al2 O3复合粉体经热压烧结,所得的致密体材料为晶内型纳米复合材料,其抗弯强度达612MPa,断裂韧性为4．54MPa．m-1/2,都比单相Al2 O 3陶瓷有大幅度提高．     

Al2O3颗粒形貌对注凝成型ZrO2/Al2O3陶瓷性能的影响

采用3种不同形貌的Al₂O₃原料对注凝成型制备ZrO₂/Al₂O₃（ZTA）陶瓷工艺中悬浮体的流变性能进行了研究。以低毒的单体N,N-二甲基丙烯酰胺（DMAA）制备了ZrO₂/Al₂O₃坯体和陶瓷。讨论了3种不同形貌的Al₂O₃原浆料的分散剂用量、球磨时间和固含量对浆料流变性的影响。Al₂O₃粉体呈扁平状有利于降低浆料的黏度,Al₂O₃粉体呈棒状对生坯强度的提高有利。制得的3种ZrO₂/Al₂O₃坯体颗粒间结合紧密,抗弯强度分别达到21.45,19.87,25.90 MPa。Al₂O₃粉体呈颗粒状有利于最终陶瓷力学性能的提高,陶瓷的抗弯强度及断裂韧性分别为680 MPa和7.49 MPa·m^1/2,453.1 MPa和6.8 MPa·m^1/2,549.4 MPa和6.34 MPa·m^1/2。     

水热合成KAl(OH)2CO3粉体的形貌控制

分别采用AlCl3·6H2O,Al(NO3)3·6H2O,Al2(SO4)3·12H2O为前驱体在水热条件下合成了KAl(OH)2CO3粉体.实现了KAl(OH)2CO3粉体的微观形貌从纤维状微米级颗粒到柱状两维纳米级颗粒的控制.XRD、TEM等的分析结果表明,水热体系中的铝盐种类、阴离子浓度以及反应时间等条件对所合成产物的颗粒形貌有显著的影响.其中Al(NO3)3是合成KAl(OH)2CO3的最佳前驱物,当[NO-3-]=1.2mol/L时,在120℃,反应4h条件下合成的粉体颗粒直径小于20nm,长径比约为5,且外形规整,粒度分布均匀,没有团聚.     

Al2O3/Al2O3-ZrO2（3Y）层状纳米复合材料的制备与性能优化

为优化Al2O3层状复合材料的制备工艺及力学性能,选用不同初始粉体为原料制备了系列Al2O3/Al2O3-ZrO2(3Y)层状复合材料。借助X射线衍射、冷场发射扫描电镜和万能试验机等手段,系统考察了粉体结构和形貌对层状复合材料显微结构和性能的影响。结果表明:初始粉体的颗粒尺寸及尺寸分布会显著影响层状复合材料的显微结构及力学性能,以球磨微-纳米复合粉体为原料制备的层状复合材料具有最佳的力学性能,其抗弯强度和断裂功分别可达740MPa及3892J.m-2。同时,材料具有较高的层间结合强度,平行于层方向的抗弯强度高达436MPa。     

原位氮化法制备纳米TiN-Al2O3复合粉体

以化学沉淀法的制备的纳米TiN-Al2O3复合粉体为原料，采用原位选择性氮化的方法制备了纳米TiN-Al2O3复合粉体。应用化学热力学原理分析，计算了氮化反应的条件和机理，研究了氮化条件对氮化反应的影响，实验结果表明，氮化反应在700℃时开始进行，在900℃保温5h，氮化反应进行完全，TEM照片显示纳米TiN颗粒均匀分布于Al2O3基体中，径粒为50－70nm。     

晶内/晶间复合型Al2O3/Ni纳米金属陶瓷显微结构和力学性能的研究

采用非均相沉淀法和热压工艺制备了Al2O3/Ni纳米金属陶瓷。在1450℃热压γ-Al2O3/Ni复合粉体得到相对密度＞985的金属陶瓷。结果表明，Ni颗粒均匀分布在基体中，其中＜100nm的Ni颗粒位于Al2O3晶内，100－300nm的分布在晶界，形成了晶内／晶界复合型纳米金属陶瓷。同单相Al2O3相比，Al2O3/Ni金属陶瓷的三点抗弯强度和断裂韧性分别增加了26％和795。分析了纳米金属陶瓷的增强增韧机制。     

无压烧结制备Si3N4/SiO2复合材料

以无压烧结工艺制备了Si3N4/SiO2复合材料.实验结果表明Si3N4颗粒对石英基体的析晶起到了抑制作用和增韧补强作用.Si3N4含量为5vol%的样品在1370℃烧结2h后,抗弯强度达到96.2MPa,断裂韧性为2.4MPa·m1/2,介电常数和介电损耗分别在3.63～3.68和1.29～1.75×10-3之间.     

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.     

Varistor properties of ZnO-Pr6O11-CoO-Cr2O3-Y2O3-In2O3 ceramics

The varistor properties of the ZnO-Pr₆O₁₁-CoO-Cr₂O₃-Y₂O₃-In₂O₃ ceramics were investigated for different concentrations of In₂O₃. The increase of In₂O₃ concentration slightly increased the sintered density (5.60-5.63 g/cm³) and slightly decreased the average grain size (3.4-2.9 μm). The breakdown field increased from 6023 to 14822 V/cm with increasing concentration of In₂O₃. The nonlinear coefficient increased from 17.6 to 44.6 for up to 0.005 mol%, whereas the further doping caused it to decrease to 36.8. In₂O₃ acted as an acceptor due to the donor concentration, which decreases in the range of 1.02 × 10¹⁷ to 0.24 × 10¹⁷/cm³ with increasing concentration of In₂O₃.     

Microstructures of YBa2Cu3O7/La0.7Ca0.3MnO3 and La0.7Ca0.3MnO3/YBa2Cu3O7 bi-layers grown on (001)LaAlO3

Epitaxial YBa₂Cu₃O₇/La_0.7Ca_0.3MnO₃ (YBCO/LCMO) bi-layers and La_0.7Ca_0.3MnO₃/YBa₂Cu₃O₇ (LCMO/YBCO) bi-layers were grown on (001)LaAlO₃ by pulsed laser deposition, and their microstructures were compared by transmission electron microscopy investigation. In the YBCO(100 nm)/LCMO(150 nm) bi-layers, the LCMO layer consists of columnar grains of ~ 17 nm in diameter and contains mixed orientation domains of [100]_c, [010]_c and [001]_c. The YBCO layer is totally c-axis oriented and the YBCO lattices are tilted − 2.5° to + 2.5° as they grew on the rough surfaces of LCMO columnar grains. For the LCMO(140 nm)/YBCO(140 nm) bi-layers, the LCMO/YBCO interface is sharp and flat. The initial 12-nm thickness of the YBCO layer is composed of c-axis oriented domains, and the upper part of YBCO layer is [100] oriented. The LCMO layer was predominantly [001]_c oriented while [100]_c-oriented domains were occasionally observed.     

Syntheses of hollandite type Rb2Cr8O16, K2Cr2V6O16 and K2V8O16

Hollandite-type compounds, Rb₂Cr₈O₁₆, K₂Cr₂V₆O₁₆ and K₂V₈O₁₆, were synthesized under high P-T conditions up to 1200°C and 7GPa. The structural refinement using a single crystal of Rb₂Cr₈O₁₆ confirms that the structure is similar to that of K₂Cr₈O₁₆. Magnetic measurements indicate that Rb₂Cr₈O₁₆ is ferromagnetic below 295K, K₂Cr₂V₆O₁₆ paramagnetic down to 77K and K₂V₈O₁₆ has susceptibility anomaly at 175K. These compounds are all semiconductive and show discontinuities in temperature-resistivity curves at points corresponding to magnetic anomalies.     

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.     

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.     

静电纺丝法制备的Co0.6Ni0.3Cu0.1Fe2O4和Co0.6Ni0.3Zn0.1Fe2O4纳米纤维的结构及磁性能

采用静电纺丝技术制备出表面光滑、直径均匀的Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4/PVP和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4/PVP纳米纤维前驱丝,经500~900℃煅烧后得到Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维。用TG-DSC、XRD、SEM及VSM现代测试分析手段对Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的结构、形貌及磁学性能进行测试表征。结果表明:在空气气氛中经500~900℃煅烧后可得到纯尖晶石相、结晶度良好的纳米纤维或短纤维;当温度为700℃时,Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的形貌细长而光滑且直径相对均匀,大约为80nm;此时Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维则保有较高的剩磁比(M_r/M_s)及矫顽力,分别为0.56和1 088.87Oe。在500℃、600℃、700℃、800℃、900℃煅烧后,Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的饱和磁化强度分别比Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维增大了14.5%、7%、16%、10.7%、8%,而矫顽力则分别降低了38%、51%、50%、46%、46.7%。两种纳米纤维的饱和磁化强度及矫顽力存在差异,为CoNi铁氧体在电磁方面的应用提供了很好的参考。     

Structural study of Sr0.3Ba0.7Nb2O6 and La0.030Sr0.255Ba0.700Nb2O6 ceramic systems

Sr_0.3Ba_0.7Nb₂O₆ (SBN) and La_0.030Sr_0.255Ba_0.700Nb₂O₆ (LSBN) ceramic compounds have been prepared using the traditional ceramic method at two different calcination temperatures (900 and 1000 °C) and later sintered both at 1400 °C. A study of the effects of the calcination temperatures and La substitution on the morphological, compositional, and structural properties of SBN and LSBN is presented using scanning electronic microscopy (SEM), energy dispersive spectroscopy (EDS), and X-ray diffraction (XRD) analysis. From Rietveld refinement processes, the XRD patterns were interpreted to evaluate such effects in the structural parameters and the site occupation factors of the heavy metals and oxygen atoms. The effect of the incorporation of La resulted in a 0.25% cell contraction and turned out to be higher than the 0.08% dilation effect produced by the increase of calcination temperature. The La ion with similar effective ionic radius and higher electronegativity is incorporated into the structure occupying the A₁ site just like the Sr ions in the SBN compound. Differences in the site occupation factors between the SBN and LSBN samples lead to substantial changes in the physical properties such as temperature of relative dielectric constant maximum, relative dielectric constant, and dielectric loss, correlated with the distortion and the relative orientation of the oxygen octahedra.     

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.     

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.