微弧等离子喷涂碳纳米管/纳米Al2O3-TiO2复合涂层高温性能研究

采用等离子喷涂技术制备了5wt%CNTs/Al2O3-TiO2复合涂层,借助SEM、热红联仪和RAM反射率测试系统对CNTs/Al2O3-TiO2复合涂层的组织结构、高温氧化性能、电磁特性进行了分析.结果表明:CNTs/Al2O3-TiO2复合涂层的组织结构致密、孔隙率低,CNTs分散均匀,碳纳米管与Al2O3-TiO2陶瓷粘结剂之间具有良好的界面相容性.在20～700℃高温氧化过程中,CNTs起始失重温度为471.29℃,CNTs/Al2O3-TiO2复合涂层的高温氧化性能有一定提高,起始失重温度从471.29℃提高到507.8℃,而碳纳米管的失重率从100%下降到33.68%.CNTs/Al2O3-TiO2复合涂层具有较好的高温吸波性能,25℃时复合涂层的反射率峰值为-7.86dB.随温度的升高,CNTs/Al2O3-TiO2复合涂层的反射率峰值不断减小,谐振频率向低频移动,300℃时复合涂层的反射率峰值为-12.88dB,小于-5dB频带宽为4.48GHz.     

CNTs-SiC/Al2O3-TiO2复合涂层的制备及其性能

采用微弧等离子喷涂技术制备了CNTs-SiC/Al2O3-TiO2复合涂层,借助SEM、X射线衍射、仪热分析仪和网络分析仪对CNTs-SiC/Al2O3-TiO2涂层的组织结构、高温氧化性能、电磁特性进行了测试分析.结果表明:多功能微弧等离子喷涂枪内中心轴向送粉方式制备的CNTs-SiC/Al2O3-TiO2复合涂层的组织结构致密、孔隙率低,SiC和CNTs的物相也保留下来.CNTs-SiC/Al2O3-TiO2涂层的高温氧化性能有所提高,涂层在35～700℃升温阶段失重率为0.71wt%,700℃恒温氧化60min后失重率为0.41wt%.随着频率的增加,CNTs-SiC/Al2O3-TiO2复合粉末的介电常数的实部从17.3下降到10.3,而虚部在6.3～2.9之间,具有频散效应.制备的CNTs-SiC/Al2O3-TiO2复合涂层在一定的范围内随着涂层厚度的增加,吸波能力显著提高,其谐振频率不断向低频移动.     

不同管径CNTs/Al2O3-TiO2复合吸波涂层的拉曼光谱特征及吸波性能研究

采用超声共混法制备了不同管径的CNTs/Al2O3-TiO2复合粉末,利用等离子喷涂技术制备了CNTs/Al2O3-TiO2复合涂层,对不同管径的CNTs/Al2O3-TiO2复合粉末和喷涂后的复合吸波涂层进行了拉曼光谱分析,等离子喷涂处理后,CNTs的拉曼光谱特征D峰和G峰强度明显增大,随CNTs管径的增大,复合涂层中CNTs的D峰和G峰的强度比ID/IG值减小,石墨化程度提高。吸波反射率结果显示:涂层厚度为1.0 mm的CNTs/Al2O3-TiO2复合涂层的吸波效果不佳,随着厚度的增加,涂层的吸波性能提高。随管径的增大,涂层厚度为1.5 mm的CNTs/Al2O3-TiO2复合涂层的反射率峰值先减小后增大,小于–5 dB频带宽逐渐减小,小于–10 dB频带宽不断增大,谐振频率向高频移动。涂层厚度增加到2.0 mm,CNTs/Al2O3-TiO2复合涂层的反射率峰值向低频移动。     

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。     

等离子喷涂纳米Al2O3/TiO2复合陶瓷涂层的显微组织与性能

采用液相喷雾造粒方法将纳米级Al2O3/TiO2团聚成微米级颗粒,制备了适用于等离子喷涂的陶瓷复合粉体,并利用等离子喷涂技术成功的制备出了含有纳米结构的陶瓷涂层.利用X射线衍射、扫描电镜、透射电镜和显微硬度计等设备对涂层的微观结构和性能做了初步的检测.结果表明,涂层中含有适当比例的未熔或半熔的纳米颗粒,涂层的硬度、韧性和耐磨性等性能与普通涂层相比都有了较大提高.     

纳米掺杂Al2O3/ZrO2等离子喷涂涂层组织结构研究

利用大气等离子喷涂技术,在N80钢基体上制备纳米掺杂Al2O3/ZrO2热障涂层。利用XRD、SEM等观察分析了纳米掺杂Al2O3/ZrO2粉末及等离子喷涂涂层组织形貌及结构,结果表明,Al2O3/ZrO2等离子喷涂粉末是由纳米包覆微米级粒子及少量的纳米团聚体球团粒子构成。纳米掺杂等离子喷涂Al2O3/ZrO2涂层的微观组织形貌复杂,存在着纳米柱状晶薄壳内包裹着微米级柱状晶、未熔化的ZrO2陶瓷粒子嵌镶在晶体内部的独特晶内结构。涂层主要由α-Al2O3及亚稳四方相t,-ZrO2相构成。     

大气等离子喷涂Al2O3/ZnO/TiO2涂层微波介电性能的研究

采用高焓大气等离子喷涂技术,以纳米级ZnO、Al2O3和TiO2为原料,通过固相反应制得以ZnAl2O4为主相的陶瓷粉末,加入粘结剂聚乙烯醇(PVA),通过喷雾造粒的方法制备复合吸波陶瓷涂层(简称为AZT涂层).分析了AZT涂层的微观结构和相组成,探究了喷涂功率对AZT涂层微波介电性能的影响.结果表明,AZT涂层对比粉...     

Fe3Al-Al2O3陶瓷梯度涂层性能研究

利用等离子喷涂制备了不同成分设计的多种Fe3Al-Al2O3陶瓷复合涂层，采用金相显微镜、SEM、XRD及电子探针等手段，研究了涂层的微观组织及成分分布，并对涂层的结合强度、显微硬度及抗热震性能进行了试验研究。结果表明，Fe3Al过渡层的引入可有效地改善涂层的质量，Fe3Al金属间化合物是钢基体上制备陶瓷涂层较为理想的过渡材料。涂层成分的梯度化有利于涂层结合强度和抗热震性能的提高。     

纳米Si3N4和喂料等离子处理对等离子喷涂Al2O3-YSZ涂层抗热震性能的影响

Si3N4可以提高Al2O3-ZrO2涂层的力学性能和抗氧化性能,但其对Al2O3-YSZ(Y2O3部分稳定的ZrO2)抗热震性能的影响未见报道.采用等离子喷涂的方法在304不锈钢表面制备了Al2O3-YSZ涂层.在喂料制备过程中加入纳米Si3N4,然后对添加和未添加纳米Si3N4的喂料进行等离子处理,研究纳米Si3N4和喂料等离子处理对涂层在800℃和1 000℃下抗热震性能的影响.采用扫描电子显微镜和X射线衍射仪分析了涂层热震试验前后的形貌及物相的变化.结果表明:喂料添加纳米Si3N4和等离子处理的综合作用显著地提高了涂层的抗热震性能;与喂料未添加纳米Si3N4且未经等离子处理的涂层相比,喂料添加纳米Si3N4且经等离子处理的涂层在800℃和1 000℃条件下的抗热震寿命分别提高了0.7倍和1.1倍;热震过程中涂层发生了α-Al2O3到γ-Al2O3的相变;在1 000℃下热震,涂层中形成了较宽的裂纹,涂层抗热震性能明显下降.     

等离子喷涂MoSi2/Al2O3涂层材料的力学与介电性能

以MoSi2为吸收剂,纳米Al2O3粉为基体,采用大气等离子喷涂法制备出MoSi2/Al2O3复合涂层。研究了MoSi2含量对复合涂层力学及介电性能的影响。结果表明,MoSi2颗粒均匀分布于Al2O3基体中;随MoSi2含量的增加,复合涂层的抗弯强度、断裂韧性及冲击强度逐渐增强;根据测定的复介电常数与频率的关系及计算出的介电损耗角正切可以看出,复合涂层的介电常数与MoSi2含量有关,MoSi2掺量越高,复合材料涂层的介电常数越小;随频率的逐渐增大,材料的复介电常数表现出减小的趋势,具有频散效应。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

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 ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O