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.     

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。     

等离子喷涂纳米Al2O3-TiO2复合陶瓷涂层的研究现状

等离子喷涂纳米Al2O3-TiO2复合陶瓷涂层具有耐磨、耐腐蚀、抗热氧化等优良性能,因而成为目前纳米涂层领域的研究热点之一。归纳了纳米结构Al2O3-TiO2喂料的制备方法,介绍了纳米结构涂层的显微结构和力学性能(断裂韧性、显微硬度、结合强度等),分析了纳米结构涂层的抗热氧化性和摩擦学性能,综述了等离子喷涂纳米Al2O3-TiO2复合陶瓷涂层的研究现状,讨论并展望了其未来的发展方向和应用前景。     

石墨表面Al_2O_3/SiO_2复合涂层的抗氧化性能

400 ℃下的石墨不能有效地冷却热气溶胶,且抗氧化失重性能差.采用sol-gel法在石墨表面制备了Al2O3/SiO2复合涂层,探讨了Al2O3粉末对涂层抗氧化性能的影响,研究了涂层的组成、结构形貌及抗氧化性能.结果表明:sol-gel法制备的Al2O3/SiO2复合抗氧化涂层除了少量的微孔外,比较致密完整,涂层主要由无定形的SiO2和Al2O3晶体组成;涂层700℃氧化40 min后失重为1.866%(质量分数),800℃氧化30 min后失重为2.750%(质量分数);Al2O3/SiO2复合溶胶中加入适量的Al2O3粉末能有效提高涂层的抗氧化性能.     

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。     

HVOF和APS喷涂制备掺杂超细Al2O3颗粒复合CoNiCrAlY涂层研究

在MCrACY中添加一定量Al2O3可提高其高温磨损性能.为此,将CoNiCrAlY和微米级Al2O3粉末颗粒按比例混合后在密封球磨机里球磨,筛分后得到复合CoNiCrAlY/Al2O3粉末颗粒.分别采用超音速火焰(HVOF)喷涂和大气等离子(APS)喷涂制备复合CoNiCrAlY/Al2O3涂层,并对喷涂粉末及2种涂...     

钛合金表面阴极微弧电沉积Al2O3-SiC复合涂层

通过高温烧结法在TC4钛合金表面制备了起弧阻挡层,然后采用阴极微弧电沉积工艺在TC4钛合金表面制备了Al2O3-SiC复合陶瓷涂层,重点研究了复合陶瓷涂层的制备工艺及影响因素,并采用扫描电镜、能谱仪等观测了起弧阻挡层及复合陶瓷涂层的表面微观形貌及成分组成。结果表明,阴极微弧电沉积技术能够在钛合金表面制备出Al2O3-SiC复合涂层,且起弧阻挡层至关重要,为起弧必备条件,SiC在Al2O3基体中的分散性较好,涂层较厚且分布均匀。     

C/C-SiC复合材料表面Y2O3-ZrO2-Al2O3涂层的涂刷法制备及其抗高温氧化性能

为了提高C/C复合材料的抗高温氧化性能,用包埋法在C/C复合材料表面制备SiC内涂层,再在其上刷涂制备Y2O3-ZrO2-Al2O3多组分涂层,对制备涂层的各种影响因素进行分析,确定最佳制备工艺,并考察了该涂层的组织结构和抗高温氧化性能。结果表明:最佳制备条件为以SiC为内涂层、10%聚乙烯醇(PVA)为分散剂,以Y2O3,ZrO2,Al2O3,Si及C为原料,室温涂覆,升温到1 873 K保温30 min,反复进行5次;该涂层在1 873 K下氧化19 h,失重率仅1.76%,有良好的短期抗高温氧化性能,氧化29 h时失重率为6.23%,涂层可能已破坏失效;涂层的失效是由于其表面形成的孔洞和裂纹不能愈合而导致的。     

等离子喷涂CNTs/Al2O3复合涂层力学性能研究

通过等离子喷涂工艺制备了不同碳纳米管含量的CNTs/Al2O3复合涂层,系统研究了碳纳米管含量对涂层孔隙率、洛氏硬度和断裂韧性的影响规律。实验结果表明:采用喷雾干燥工艺制备的CNTs/Al2O3颗粒为球形,CNTs均匀分布在团聚颗粒的表面;部分CNTs经等离子喷涂后保留在沉积涂层内部并且与Al2O3基体形成冶金结合,起到一定桥接作用。涂层孔隙率和洛氏硬度值均随CNTs含量的增加呈现降低的趋势。随CNTs含量从6%(质量分数)增加到12%(质量分数),CNTs增韧效果的增强和涂层孔隙率的降低导致涂层断裂韧性值从48MPa增加到90MPa。     

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.     

Thermoelectric power of single-phase samples of Tl2CaBa2Cu2O y and Ba2CaSr2Cu2O y

Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-T _c . The thermopower was positive and decreased linearly with increasing temperature aboveT _c (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.     

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     

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.