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采用液相还原法分别制备了碳纳米管(MWCNT)、活性炭(AC)、碳纳米纤维(CNF)和炭气凝胶(CA)负载质量分数3%的Pt催化剂,并对催化剂的结构和形貌进行了XRD和TEM等表征。以肉桂醛加氢作为探针反应,研究了其催化肉桂醛加氢的活性和产物选择性。结果表明,炭材料的结构对其催化肉桂醛加氢行为具有重要影响,纳米炭材料催化剂(Pt/MWCNT、Pt/CNF)表现出较高的CO选择性加氢行为,而无定形碳催化剂表现为C=C选择性加氢,同时Pt/MWCNT的催化活性最高。 相似文献
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《化工进展》2017,(4)
贵金属纳米晶对加氢反应具有良好的催化性能,特别是Pt纳米晶,其催化活性和选择性与纳米晶的纳米结构(形貌和尺寸)密切相关。由Gibbs-Wulff晶体生长定律可知,通过加入特定结构的封端剂可以有效控制纳米晶的形貌和尺寸。本文采用Na BH4在水溶液中还原Pt的前体H2Pt Cl6制备Pt纳米晶,并将其用于催化对硝基苯酚(p-NIP)的加氢反应。实验系统研究了碱基分子(如腺嘌呤A、鸟嘌呤G、胸腺嘧啶T、胞嘧啶C)及对应的核苷分子对Pt纳米晶构型和催化加氢活性的调控规律。研究发现,碱基分子和核苷分子对于Pt纳米晶的形貌以及尺寸具有明显的调控作用,通过不同结构生物分子的精密调控,实验制备得到了形貌和尺寸各异的Pt纳米晶。同时,所得Pt纳米晶在p-NIP的加氢反应中表现出了精密可调的催化性能。鸟嘌呤核苷、腺嘌呤核苷、β-胸腺嘧啶核苷调控制备的Pt纳米催化剂的TOFave均可达到无调控剂制备得到的催化剂的两倍以上,其中腺嘌呤核苷调控制备得到的Pt催化剂性能最好。 相似文献
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综述了催化加氢制备4,4′-二氨基二苯醚(4,4′-ODA)的研究进展,重点介绍了加氢催化剂、催化工艺和溶剂的选择。负载型镍(Ni)基催化剂、包覆Ni纳米颗粒催化剂和非晶态Ni-B合金催化剂均表现出优异的加氢活性和选择性,有望取代传统的贵金属加氢催化剂。混合溶剂比单一溶剂更理想,可以提高产品的收率和纯度。未来的发展重点是开发催化加氢连续化生产工艺及相应的催化剂,以降低生产成本,提高产品质量。 相似文献
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Structure Refinement of Mullite by the Rietveld Method and a New Method for Estimation of Chemical Composition 总被引:3,自引:0,他引:3
The structure of mullite was refined by the Rietveld method, and a new method for the estimation of chemical composition of mullite was proposed. Mullites were synthesized by firing the starting materials prepared by sol–gel and spray pyrolysis methods at various temperatures. Linear correlations were recongnized between the chemical composition of mullite analyzed with the Rietveld method and the lengths of a and b axes, but a small anomaly was found in the variation of the c axis. It was found to be caused by a difference in the c axis of pseudotetragonal mullite and that of orthorhombic mullite. A good correlation was found between the chemical composition of mullite and the intensity ratio of ( I 220 / I 111 ). This is a much more convenient method for estimating the chemical composition of mullite than Cameron's method, which uses a lattice constant. 相似文献
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Aluminosilicates of three compositions with mullite as the major phase were synthesized by a sol-gel process and characterized with bulk and microchemical analyses and microstructural observation. An apparatus for measuring the compressive creep up to 1900 K with a sensitivity of ±1 μm was constructed and used to measure the creep of singlephase mullite, mullite with second-phase glass, and mullite with second-phase corundum. Measurements in air at stresses of 15 to 100 MPa and temperatures of 1471 to 1724 K determined that samples with second-phase glass crept more rapidly than single-phase mullite or mullite with secondphase corundum. The apparent creep activation energies determined at 100 MPa were 742 kJ/mol for the mullite containing glass, 819 kJ/mol for the single-phase mullite, and 769 kJ/mol for the mullite with second-phase corundum. The stress exponents determined at 1724 K were 1.6 for the mullite plus glass, 1.5 for the single-phase mullite, and 1.2 for the mullite with α-Al2 O3 . The creep behavior of the aluminosilicates containing glass were consistent with rate control by the viscous flow of the glass and the measured creep rates were in good agreement with creep rates calculated from a model by Dryden. The creep behavior of the completely crystalline aluminosilicates was consistent with rate control by diffusional creep. 相似文献
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Kaolin undergoes a series of phase changes on heating to elevated temperature, proceeding through kaolin, metakaolin, γ-Al2 O3 spinel, and mullite. The morphologic evolution of the kaolin–mullite reaction series was investigated in the present study. A highly textured kaolin green body was prepared by a tape-casting technique, and the morphology evolution from kaolin flakes to mullite aciculars on firing from 450° to 1600°C was then monitored using X-ray diffractometry and scanning electron microscopy. Equiaxed mullite nuclei first appeared at 1000°C; the aspect ratio of the mullite grains then increased with increased firing temperature. The mullite aciculars rearranged their orientation in a glassy phase until they impinged on each other. A highly textured mullite specimen was prepared by firing the kaolin tape at a temperature >1500°C. 相似文献
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Development of Textured Mullite by Templated Grain Growth 总被引:4,自引:0,他引:4
Highly textured mullite was obtained by enhancing anisotropic grain growth by TiO2 doping and by templating grain growth on oriented acicular mullite seed particles in a mullite precursor. Upon heating, the mullite precursor crystallized and densified to an equiaxed microstructure of 1-2 µm mullite grains at which time the mullite seed particles grew rapidly in the length direction ( c -axis) to produce a highly textured microstructure. By changing the seed (template) particle concentration, a range of oriented microstructures and anisotropic grains could be produced. 相似文献
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Ling Bing Kong Tian Shu Zhang Jan Ma Freddy Yin Chiang Boey 《Journal of the American Ceramic Society》2007,90(12):4055-4058
High-energy ball milling was applied to a commercial mullite powder, which had a particle size ranging from 2 to 10 μm, and was considerably refined to be <1 μm after milling for 10 h. Anisotropic grain growth of mullite was observed in the milled mullite powder, starting at relatively low temperatures (1200°C). The anisotropic grain growth was possibly attributed to the special anisotropic structure of mullite and refined mullite powder as a result of the high-energy ball milling, although other factors, such as lattice defects, localized stress of the milled powder, and impurities or contaminations caused by the high-energy milling also could be factors. This anisotropic grain growth of mullite might be useful in the fabrication of reinforced ceramics based on mullite and other materials. 相似文献
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《应用陶瓷进展》2013,112(6):349-353
Alumina/mullite ceramic nanocomposites were prepared by the mixtures of nano-sized starting powders of alumina with silica and alumina with silicon carbide. Silica from deliberate addition and as the product of silicon carbide oxidation reacted completely with alumina to form mullite. Silica from direct addition segregated at the grain boundary and intergranular mullite was formed whereas silica from oxidation was surrounded by alumina matrix and intragranular mullite was formed after reaction sintering. The most significant difference was fracture behaviour where intragranular mullite nanoparticles promoted transgranular fracture in alumina matrix due to thermal mismatch around nanoparticles and intergranular mullite nanoparticles gave rise to intergranular fracture similar to pure alumina. Wear resistance of the nanocomposites was better than that of alumina. Pull-out formation in the nanocomposites was less and pull-out size was also smaller. Fracture toughness of the nanocomposites was significantly higher than that of alumina. 相似文献