ZIF-67/CeO2催化CO2和甲醇直接合成碳酸二甲酯

采用沉淀法将ZIF-67负载到CeO₂上,制备了具有多重活性位点的非均相催化剂ZIF-67/CeO₂,并研究其催化CO₂和甲醇直接反应生成碳酸二甲酯(DMC)的性能。采用 X 射线衍射、N2吸附-脱附、傅里叶变换红外光谱和 X 射线光电子能谱研究了ZIF-67/CeO₂的各种理化性质。结果表明,ZIF-67的引入使ZIF-67/CeO₂催化剂产生更多的氧空位。在考察的ZIF-67/CeO₂系列催化剂中,0.3-ZIF-67/CeO₂(0.3为Co、Ce物质的量之比)在具有高的比表面积的同时还能保持介孔结构,具有丰富的酸碱位点,并且具有较高的CO₂吸附容量,表现出最好的催化性能。在反应温度为140℃、压力为4.5 MPa的条件下反应4 h,DMC收率可达到3.79 mmol_DMC·gcat^-1。     

CoMoSx/CeO2-γ-Al2O3催化剂的制备及其催化还原SO2的性能

采用等容浸渍法引入少量CeO₂助剂制备了CoMoS_x/CeO₂-γ-Al₂O₃催化剂。通过X射线衍射(XRD)、高角环形暗场像-扫描催化剂的形貌结构、还原性、吸附性能及反应过程等进行了表征,利用固定床反应器研究了其催化CO还原SO₂的催化性能及稳定性。结果表明:少量CeO₂的引入可以降低反应温度,随着CeO₂含量的增加,CoMoS_x/CeO₂-γ-Al₂O₃催化剂的催化活性先增剂具有优异的稳定性;等容浸渍法制备的催化剂表面的金属元素分散良好;CeO₂的引入提高了催化剂的硫化程度和低温还原进行。     

载体效应与镍晶粒尺寸对CO2甲烷化低温催化性能的影响

采用等体积浸渍法制备MgO和CeO₂负载的一系列不同镍含量催化剂，对其进行了二氧化碳甲烷化催化性能评价。研究结果表明NiO/CeO₂基催化剂具有优异的低温催化活性，其中80%NiO/CeO₂催化剂，在18 L/(g·h)、H₂/CO₂=4和350℃反应条件下甲烷产率为67%。探究了镍含量对NiO/MgO和NiO/CeO₂催化剂活性的影响，结果表明，随着镍含量增加，二氧化碳转化率、甲烷产率升高，在镍负载量为50%～80%时催化性能最佳。通过X射线衍射(XRD)、氢气程序升温还原(H₂-TPR)、拉曼(Raman)、CO₂-TPD表征探究不同载体和Ni晶粒大小对NiO/MgO,NiO/CeO₂催化剂催化活性的影响。本研究可为设计具有优异低温催化性能的二氧化碳甲烷化催化剂提供参考。     

载体形貌对Ni3Fe/CeO2催化剂甲烷干重整反应性能的影响

通过改变水热法条件合成了不同形貌CeO₂载体(棒状CeO₂-R、立方体CeO₂-C和多面体CeO₂-P),并用浸渍法制备了Ni₃Fe/CeO₂催化剂,继而研究了不同载体形貌Ni₃Fe/CeO₂催化剂对其甲烷干重整反应性能的影响。采用X射线衍射、N₂吸附-脱附、透射电镜、拉曼光谱、X射线光电子能谱、热重等对反应前后催化剂结构进行表征。结果表明,Ni₃Fe/CeO₂-R具有较大比表面积和较高的氧空位浓度,在甲烷干重整反应中表现出了优异的催化反应活性。800℃时,CH₄和CO₂的转化率分别为82%和91%,且反应10 h性能稳定并且其积炭石墨化程度较低。同时,通过CeO₂-R载体氧空位对CO₂活化,有效抑制了对亲氧性Fe物种的过度氧化行为,反应前后催化剂Ni_...     

高活性Cu-ZnO@SiO2纳米催化剂催化CO2加氢制甲醇

铜基催化剂可被广泛应用于CO₂加氢制甲醇,其催化活性高度依赖载体.本文通过St?ber法合成了SiO₂纳米微球,将其作为载体制备了Cu-Zn O@Si O₂催化剂；将该催化剂应用于CO₂加氢制甲醇,并与常规共沉淀法制备的Cu-Zn O催化剂进行了对比.通过X射线衍射(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)、氢气程序升温还原(H₂-TPR)和二氧化碳程序升温脱附(CO₂-TPD)等手段对催化剂进行了表征.结果表明，Cu-Zn O@Si O₂催化剂具有更高的Cu分散性和CO₂吸附能力,Si O₂的加入提高了催化剂表面Cu⁺/Cu⁰的比例,从而影响了催化性能.研究发现,在H₂/CO₂摩尔比为3,230℃,2.0 MPa和气体体积空速为3600 m L·g     

不同WO3含量对CeO2-ZrO2-WO3催化剂在NH3选择性催化还原NO中的影响

采用水热法制备了CeO₂-ZrO₂-WO₃(CZW)催化剂,考察了WO₃含量对CZW催化剂上NH₃选择性催化还原NO_x性能的影响,并利用X射线衍射、N₂吸附-脱附、H₂程序升温还原、NH₃和NO程序升温脱附等方法对其进行了表征。结果表明,WO₃以无定形的形式存在于催化剂中,添加WO₃后显著提高了催化剂的表面酸性,并且在CZW催化剂上出现了强吸附的NO物种,从而有利于提高催化剂的活性。另外,适量的WO₃引入将增大催化剂的比表面积,促进催化剂的氧化还原性能,这将有利于提高SCR的催化活性。和CeO₂-ZrO₂催化剂相比,当WO₃的含量为20%时,CZW催化剂表现出良好的抗硫性能。此外,当空速为60 000 h^-1时,在200~463 ℃,该催化剂显示出了大于90% NO_x转化率。     

负载型LaCoO3/MO2催化氧化甲苯与NO的性能研究

本研究采用柠檬酸溶胶-凝胶法制备了一系列不同载体负载的LaCoO₃/MO₂催化剂（M=Zr、Ti、Ce）,研究考察其催化氧化甲苯与NO的性能及关键机制。结果发现,以CeO₂为载体的LaCoO₃/CeO₂催化剂表现出最佳的催化氧化性能,其甲苯的t₉₀为245℃,同时在300℃时NO转化率可达68%。通过BET、XRD、H₂-TPR和XPS对各负载型钙钛矿催化剂的理化性质进行表征。结果表明,负载型钙钛矿催化剂拥有更大的比表面积,从而有效提供了更多的吸附位点,同时负载型钙钛矿催化剂具有更活跃的晶格氧和更好的氧化还原性能。其中,LaCoO₃与载体CeO₂在接触界面上观察到Co离子与Ce离子之间存在着相互作用,形成晶格缺陷,这有利于氧空位的形成。利用原位漫反射红外光谱进一步探寻了反应机理,LaCoO₃/CeO₂催化剂上NO氧化符合Langmuir-Hinsh...     

制备方法对Ni/CeO2-Al2O3催化剂甲烷部分氧化催化性能的影响

采用浸渍-沉淀法、水热合成法、共沉淀法和柠檬酸络合法制备了Ni/CeO₂-Al₂O₃催化剂,考察了制备方法对该催化剂的物理结构和甲烷部分氧化(POM)催化性能的影响。利用N₂物理吸附、X射线粉末衍射(XRD)、H₂-程序升温还原(H₂-TPR)、NH₃-程序升温脱附(NH₃-TPD)、热重(TG)分析等手段对反应前后催化剂的物理化学性质进行了表征。实验结果表明,浸渍-沉淀法制备催化剂的活性和产物H₂和CO的选择性最低。而柠檬酸络合法制备的Ni/CeO₂-Al₂O₃表现出最大的CH₄转化率和最高的CO、H₂选择性。BET和XRD表征结果表明,柠檬酸络合法制备的Ni/CeO₂-Al₂O₃的比表面积最大,且CeO₂晶粒粒径小、分散均匀;H₂-TPR测试表明,该催化剂负载的Ni物种和Ni与Al₂O₃相互作用产生的尖晶石NiAl₂O₄都较容易被还原成金属Ni,产生更多的活性中心;NH₃-TPD和TG分析表明,该催化剂具有较多酸性位点和表面积炭,但相比较于它的高反应活性,积炭速率较低、稳定性较高。     

Ni-Co/TiO2增强CO2加氢反应性能的研究

通过浸渍-沉淀法合成负载型双金属催化剂Ni-Co/TiO₂,采用X射线衍射(XRD)、场发射扫描电子显微镜(FESEM)、X射线能谱(EDS)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)和氮气吸附-脱附(BET)对其晶型、形貌、组成、表面元素价态和比表面积进行表征.在CO₂加氢反应中,Ni-Co/Ti O₂催化剂在3 h反应时间内生成84.4μmol CH₄,相较于Ni/Ti O₂催化剂,其CH₄产量提高了46.3%.二氧化碳程序升温脱附(CO₂-TPD)和氢气程序升温还原(H₂-TPR)测试结果证实,Co的引入能增强Ni-Co/Ti O₂对CO₂的吸附和活化,从而促进其加氢反应效率的提高.经过5次循环活性测试,Ni/Ti O₂的活性降低了20.5%,而Ni-Co/Ti O₂的活性仅仅降低了10.9%,这表明Co的引...     

CeO2-MnOx催化剂形貌对低浓度甲烷催化燃烧反应性能的影响

采用水热合成法制备了船形、扁球形及纳米片CeO₂-MnO_x复合氧化物。并运用低温N₂吸脱附、XRD、SEM、TEM、H₂-TPR、拉曼光谱、XPS等表征技术对不同形貌CeO₂-MnO_x复合氧化物的结构与其低浓度CH₄催化燃烧反应性能之间的关系进行了关联。结果表明,CeO₂-MnO_x复合氧化物的形貌与其催化性能密切相关。其中,扁球形CeO₂-MnO_x复合氧化物的氧空位、Ce³⁺含量及表面吸附活性氧物种最多,其CH₄催化燃烧反应活性最高,540℃时,可将CH₄完全转化;其次是船形CeO₂-MnO_x复合氧化物催化剂,540℃时其CH₄转化率为94.05%;与前两者相比,纳米片CeO₂-MnO_x复合氧化物催化剂的氧空位及表面吸附活性氧物种较少,活性较差,相同反应温度下,其CH₄转化率仅为89.68%。     

LiCoO2梯度包覆LiNi0.96Co0.04O2电极材料的电化学性能

镍钴酸锂(LiNi0.8Co0.2O2)与目前商业用锂离子电池正极材料钴酸锂(LiCoO2)相比,具有成本低、实际比容量高和环境友好等优势。但LiNi0.8Co0.2O2的充放循环性能还有待提高,对其进行阳离子掺杂或表面修饰可以改善其电化学性能,这方面的研究已经成为热点。Fey等人[1]用溶胶凝胶法制     

Preparation of ZrO2-TiO2-CeO2 and Its Application in the Selective Catalytic Reduction of NO with NH3

TiO₂,ZrO₂-TiO₂,andZrO₂-TiO₂-CeO₂ were prepared by co-precipitation method and characterized by X-ray diffraction (XRD), specific surface area measurements (BET), temperature programmed desorption (NH₃-TPD), oxygen storage capacity (OSC), and temperature programmed reduction (H₂-TPR). The results showed that ZrO₂-TiO₂-CeO₂ exhibited large number of surface strong acid, possessed some oxygen storage capacity, and strong redox property. The three materials were used as supports and the monolith catalysts were prepared with 1% (w) V₂O₅ and 9% (w)WO₃ for selective catalytic reduction (SCR) of NO with ammonia in the presence of excessive O₂, and the results of catalytic activity showed that the catalyst used ZrO₂-TiO₂-CeO₂ as support yielded nearly 100% NO conversion at 275 °C at a gas hourly space velocity (GHSV) of 10000 h⁻¹, and it had the best catalytic activity and showed great potential for practical application.     

Synthesis and properties of the double perovskites La2NiVO6, La2CoVO6, and La2CoTiO6

The double perovskites La₂CoVO₆, La₂CoTiO₆, and La₂NiVO₆, are described. Rietveld fitting of neutron and powder X-ray diffraction data show La₂NiVO₆ and La₂CoVO₆ to have a disordered arrangement of B-cations whereas La₂CoTiO₆ shows ordering of the B-cations (with ∼5% Co/Ti inversion). Curie-Weiss fits to the linear region of the 1/χ plots reveal Weiss temperatures of −107, −34.8, and 16.3 K for La₂CoVO₆, La₂CoTiO₆, and La₂NiVO₆, respectively, and magnetic transitions are observed. La₂CoTiO₆ prepared by our method differs from material prepared by lower-temperature routes. A simple antiferromagnetic spin model is consistent with the data for La₂CoTiO₆. These compounds are semiconductors with bandgaps of 0.41 (La₂CoVO₆), 1.02 (La₂CoTiO₆) and 0.45 eV (La₂NiVO₆).     

WS2/CuGa2O4复合材料的制备及其气敏性

采用共沉淀法制备了CuGa₂O₄纳米材料,并利用水热法制备了一系列WS₂/CuGa₂O₄复合材料。结合X射线衍射(XRD)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)等对制备的材料进行了物相组成、表面形貌以及元素价态的分析。研究了WS₂的复合量对 CuGa₂O₄材料检测乙醇气体敏感性能的影响。实验结果表明,当 WS₂与 CuGa₂O₄质量比为 1%时,该复合材料制备的传感器在室温下对 100 μL·L^-1乙醇气体表现出 345.3 的灵敏度,响应时间和恢复时间分别为 184 和 69 s,且最低检测限为 0.1μL·L^-1。     

WS2/CuGa2O4复合材料的制备及其气敏性

采用共沉淀法制备了CuGa₂O₄纳米材料,并利用水热法制备了一系列WS₂/CuGa₂O₄复合材料。结合X射线衍射(XRD)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)等对制备的材料进行了物相组成、表面形貌以及元素价态的分析。研究了WS₂的复合量对CuGa₂O₄材料检测乙醇气体敏感性能的影响。实验结果表明,当WS₂与CuGa₂O₄质量比为1%时,该复合材料制备的传感器在室温下对100μL·L^-1乙醇气体表现出345.3的灵敏度,响应时间和恢复时间分别为184和69 s,且最低检测限为0.1μL·L^-1。     

Transport and optical properties of heavily hole-doped semiconductors BaCu2Se2 and BaCu2Te2

Experimental and theoretical studies of the electronic and optical properties of orthorhombic BaCu₂Se₂ and BaCu₂Te₂ are reported. Experimental data include the electrical resistivity, Hall coefficient, Seebeck coefficient, thermal conductivity, and lattice constants for , and optical transmission and diffuse reflectance data at room temperature. Nominally stoichiometric, polycrystalline samples form with hole concentrations inferred from Hall measurements of 2×10¹⁸ and 5×10¹⁹ cm⁻³ near room temperature for the selenide and telluride, respectively. The corresponding mobilities are near 15 cm² V⁻¹ s⁻¹ for both materials. Optical measurements reveal a transition near 1.8 eV in BaCu₂Se₂, while no similar feature was observed for BaCu₂Te₂. First principles calculations indicate both materials are direct or nearly direct gap semiconductors with calculated gaps near 1.0 eV and 1.3 eV for the telluride and selenide, respectively, and predict weak absorption below about 2 eV. Transport properties calculated from the electronic structure are also presented.     

CeO2改性Ag-V2O5/TiO2催化剂的甲基吡啶氧化脱甲基性能

以锐钛矿TiO_2为载体,考察了CeO_2改性对Ag-CeO_2-V_2O_5/TiO_2催化3-甲基吡啶氧化脱甲基性能的影响,并优化了催化剂组成与制备条件.结果表明:Ce掺杂改性不仅能够与V物种作用形成Ce VO_4,而且促进V_2O_5分散,改善活性组分的氧化还原性能,从而提高3-甲基吡啶脱甲基转化率与选择性,改善Ag-V_2O_5/TiO_2催化性能.适宜的催化剂组成为V_2O_5负载量15%,Ce/V的摩尔比0.33,Ag质量分数1.0%.过高的焙烧温度将导致TiO_2载体向金红石型转变,Ag-CeO_2-V_2O_5/TiO_2适宜制备条件为450℃焙烧4 h.     

Conversion of NO in NO/N2, NO/O2/N2, NO/C2H4/N2 and NO/C2H4/O2/N2 Systems by Dielectric Barrier Discharge Plasmas

An experimental study on the conversion of NO in the NO/N₂, NO/O₂/N₂, NO/C₂H₄/N₂ and NO/C₂H₄/O₂/N₂ systems has been carried out using dielectric barrier discharge (DBD) plasmas at atmospheric pressure. In the NO/N₂ system, NO decomposition to N₂ and O₂ is the dominating reaction; NO conversion to NO₂ is less significant. O₂ produced from NO decomposition was detected by an on-line mass spectrometer. With the increase of NO initial concentration, the concentration of O₂ produced decreases at 298 K, but slightly increases at 523 K. In the NO/O₂/N₂ system, NO is mainly oxidized to NO₂, but NO conversion becomes very low at 523 K and over 1.6% of O₂. In the NO/C₂H₄/N₂ system, NO is reduced to N₂ with about the same NO conversion as that in the NO/N₂ system but without NO₂ formation. In the NO/C₂H₄/O₂/N₂ system, the oxidation of NO to NO₂ is dramatically promoted. At 523 K, with the increase of the energy density, NO conversion increases rapidly first, and then almost stabilizes at 93–91% of NO conversion with 61–55% of NO₂ selectivity in the energy density range of 317–550 J L⁻¹. It finally decreases gradually at high energy density. A negligible amount of N₂O is formed in the above four systems. Of the four systems studied, NO conversion and NO₂ selectivity of the NO/C₂H₄/O₂/N₂ system are the highest, and NO/O₂/C₂H₄/N₂ system has the lowest electrical energy consumption per NO molecule converted.     

Cr2(WO4)3和Cr2(MoO4)3的负热膨胀特性研究

用液相反应-前驱物烧结法制备了Cr₂(WO₄)₃和Cr₂(MoO₄)₃粉体。298～1 073 K的原位粉末X射线衍射数据表明Cr₂(WO₄)₃和Cr₂(MoO₄)₃的晶胞体积随温度的升高而增大, 本征线热膨胀系数分别为(1.274±0.003)×10^-6 K^-1和(1.612±0.003)×10^-6 K^-1。用热膨胀仪研究了Cr₂(WO₄)₃和Cr₂(MoO₄)₃在静态空气中298～1 073 K范围内热膨胀行为，即开始表现为正热膨胀，随后在相转变点达到最大值，最后表现为负热膨胀，其负热膨胀系数分别为(-7.033±0.014)×10^-6 K^-1和(-9.282±0.019)×10^-6 K^-1。     

Why pressure induces an abrupt structural rearrangement in PdTe2 but not in PtTe2

High-pressure X-ray diffraction measurements were carried out for polymeric CdI₂-type compounds MTe₂ (M=Pt, Pd) to investigate if they undergo a structural phase transition under pressure as does IrTe₂. Up to 27 GPa at room temperature PtTe₂ does not undergo any structural phase transition. In contrast, however, an abrupt change in the inter-atomic distances occurs in PdTe₂ above 15.7 GPa at room temperature, and above 5 GPa at 300 °C, but the volume vs. pressure curve exhibits no discontinuity. To account for the differences between the isostructural compounds PtTe₂, PdTe₂ and IrTe₂, their electronic structures and bonding were analyzed on the basis of first principles electronic band structure calculations.