焙烧温度对Mn/Al2O3-TiO2催化剂结构及氧化NO性能的影响

采用溶胶凝胶法和浸渍法制备10%Mn/Al_2O_3-TiO_2催化剂,借助TPO、XRD、O_2-TPD、Raman、XPS等手段,考察焙烧温度(450~650℃)对催化剂结构以及氧化NO性能的影响。TPO结果表明催化剂活性随焙烧温度的升高先增后减,其中焙烧温度为550℃时催化剂活性最好。XPS结果显示随着焙烧温度的升高(450~550℃),催化剂表面Mn~(3+)的含量逐渐升高,与催化剂活性的强弱成对应关系,并且催化剂晶格氧含量下降,而表面化学吸附氧从40.9%增加到64.8%。Raman分析显示550℃焙烧时,催化剂表面存在丰富的Mn_2O_3活性物种,并且O_2-TPD分析也表明随着焙烧温度的升高,晶格氧向表面化学吸附氧流动,提高了化学吸附态氧物种的含量。这些结果表明Mn_2O_3可能是NO氧化起主要作用的活性Mn物种,释放更多的表面化学吸附氧物种,将有助于促进NO的催化氧化。     

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.     

焙烧温度对Mn/Al2O3-TiO2催化剂结构及氧化NO性能的影响

采用溶胶凝胶法和浸渍法制备10% Mn/Al₂O₃-TiO₂催化剂,借助TPO、XRD、O₂-TPD、Raman、XPS等手段,考察焙烧温度(450~650 ℃)对催化剂结构以及氧化NO性能的影响。TPO结果表明催化剂活性随焙烧温度的升高先增后减,其中焙烧温度为550 ℃时催化剂活性最好。XPS结果显示随着焙烧温度的升高(450~550 ℃),催化剂表面Mn³⁺的含量逐渐升高,与催化剂活性的强弱成对应关系,并且催化剂晶格氧含量下降,而表面化学吸附氧从40.9%增加到64.8%。Raman分析显示550 ℃焙烧时,催化剂表面存在丰富的Mn₂O₃活性物种,并且O₂-TPD分析也表明随着焙烧温度的升高,晶格氧向表面化学吸附氧流动,提高了化学吸附态氧物种的含量。这些结果表明Mn₂O₃可能是NO氧化起主要作用的活性Mn物种,释放更多的表面化学吸附氧物种,将有助于促进NO的催化氧化。     

MnOx/Al2O3催化剂低温SCR脱硝性能

采用浸渍法制备了MnO_x/Al_2O_3低温脱硝催化剂,研究了Mn的含量对MnO_x/Al_2O_3催化剂低温烟气中NOx脱除率的影响,并通过XRD、SEM、BET、XPS、NH_3-TPD和H_2-TPR等手段对催化剂进行了表征.结果表明,当Mn含量为9%,空速为45 000 h-1时,MnO_x/Al_2O_3催化剂NO_x脱除率最高,在220℃时达79%;9MnO_x/Al_2O_3催化剂表面MnO_x氧化物分散较均匀,且稳定性及抗H_2O性能较好,但抗SO_2性能有待提高;MnO_x/Al_2O_3催化剂孔径主要分布在4~20 nm范围内,Mn含量对催化剂孔径变化影响较小;催化剂中活性组分Mn主要以Mn~(3+)和Mn~(4+)的形式存在;Mn~(4+)和Oα含量增加有利于NO_x的脱除;且添加Mn后,活性酸位点的数量增长,增强了催化剂还原能力,促进了NO_x脱除率的增加.     

Mn-Fe/Al2O3催化剂的低温脱硝性能研究

以Al_2O_3为载体,Fe、Mn为活性组分,采用浸渍法制备了Mn-Fe/Al_2O_3催化剂,研究了Mn-Fe/Al_2O_3催化剂的低温脱硝性能.实验结果表明,Fe负载量为7%时,7Fe/Al_2O_3催化剂显示出较佳的低温脱硝性能;添加Mn能明显改变7Fe/Al_2O_3催化剂低温脱硝性能,其中当Mn/Fe质量比为11∶7时,11Mn7Fe/Al_2O_3催化剂获得最佳低温脱硝效率.对催化剂的表征结果表明,比表面积和孔径的大小不是决定催化剂性能高低的主要因素;Mn O2和Fe2O3在x Mn7Fe/Al_2O_3催化剂中具有较强的相互作用,影响活性组分微观晶体结构,改善活性组分分散程度,从而提高了催化剂的低温脱硝性能;Fe的添加使催化剂表面酸性位点数目增加,从而提高7Fe/Al_2O_3催化剂的低温脱硝效率.添加Mn不仅增多了11Mn7Fe/Al_2O_3催化剂表面酸性位点数目增加,而且使催化剂表面出现新的中强性酸位点,使其低温脱硝效率进一步提高;经过详细分析,结果表明表面吸附氧Oβ、Mn4+和Fe3+的含量较高是11Mn7Fe/Al_2O_3催化剂脱硝活性较高的主要原因.     

Mg改性对Co/γ-Al2O3-TiO2催化燃烧丙烷性能影响

采用分步浸渍法制备了系列Mg改性的Co/γ-Al_2O_3-TiO_2催化剂,通过X射线衍射(XRD)、紫外可见漫反射光谱(DR-UV-vis)、N_2吸附-脱附(BET)、X射线光电子能谱(XPS)和H_2程序升温还原(H_2-TPR)等技术对催化剂进行表征,并考察了其对丙烷燃烧的催化性能。结果表明,Co在原始γ-Al_2O_3-TiO_2载体和Mg改性MgO/γ-Al_2O_3-TiO_2载体上均以Co_3O_4的形式存在;Mg掺入后与Al_2O_3作用形成MgAl_2O_4尖晶石,改善了载体的织构性质,提升了Co_3O_4在催化剂载体表面的暴露数量和分散程度。此外,MgAl_2O_4与Co_3O_4相互作用提升了Co_3O_4颗粒表面Co~(3+)/Co~(2+)和O_(ads)/O_(latt)的比例,并削弱了Co-O键键能,从而提升了其对丙烷的催化燃烧活性。当Mg负载量为15%(质量分数)时,在Co/MgO(15%)/γ-Al_2O_3-TiO_2催化剂上进行丙烷燃烧,丙烷90%转化率的温度比无Mg掺杂的Co/γ-Al_2O_3-TiO_2催化剂的降低了45℃,并且连续反应40 h其活性保持稳定。     

KIT-6负载CeO2催化CO2和甲醇合成碳酸二甲酯

采用不同老化温度(80、100、120和150℃)合成了一系列KIT-6载体,并通过浸渍法制备了相应的CeO_2/KIT-6催化剂。结合X射线衍射、N_2物理吸附、NH_3程序升温脱附、CO_2程序升温脱附、透射电子显微镜、傅里叶变换红外光谱和X射线光电子能谱等表征结果,详细考察了老化温度对KIT-6结构以及CeO_2/KIT-6催化剂直接催化CO_2和甲醇合成碳酸二甲酯(DMC)反应活性的影响。结果表明,不同老化温度下制备的KIT-6均保持其独特的三维孔道结构。随着老化温度升高,KIT-6比表面积先增大后减小,当老化温度为100℃时,KIT-6比表面积达到最大(683 m~2·g~(-1))。KIT-6较高的比表面积有利于提高CeO_2分散度,进而提高暴露的活性位点数量,催化活性随催化剂表面中等碱/酸性吸附位数量和Ce~(3+)含量的增加而逐渐提高。其中,CeO_2/100-KIT-6催化剂中CeO_2颗粒尺寸最小(5.9 nm),暴露的活性位数量最高,催化活性最佳。随后,考察了反应温度和压力对CeO_2/100-KIT-6催化活性的影响。随着反应温度提高,催化活性先升高后降低,当反应温度为140℃时,催化活性最高;且催化活性随反应压力的提高而逐渐增加。在反应温度为140℃、压力为6.8 MPa条件下,催化剂经6次循环后,DMC收率由15 mmol·g_(CeO_2)~(-1)逐渐降低至2.8 mmol·g_(CeO_2)~(-1),原因归结为反应过程中CeO_2纳米颗粒发生团聚,使暴露出的活性位数量减少。     

CuMnCeLa-O/γ-Al2O3催化剂助燃脱硝性能研究

采用等体积浸渍法制备了Cu Mn-O/γ-Al_2O_3、Cu Mn Ce-O/γ-Al_2O_3和Cu Mn Ce La-O/γ-Al_2O_3催化剂.用XRD、BET、SEM、XPS和H_2-TPR技术对其物相和表面性质进行了表征.在连续固定床微反装置上评价了催化剂的CO+O_2和CO+NO反应性能.结果表明,催化剂样品中观测不到Cu O、Mn O_x、Ce O_2和La_2O_3的XRD晶相峰,活性组分在γ-Al_2O_3载体表面呈高度分散状态.Ce、La的引入对催化剂的比表面积、孔容和孔径分布影响不大.SEM谱图中未观测到活性组分的形貌,金属氧化物在载体表面均匀分布.Ce~(3+)!Ce~(4+)之间的可变价转换,引起Cu Mn Ce-O/γ-Al_2O_3催化剂表相Cu O中具有非完整结构的[Cu~(2+)_(1-x)Cu_x~+][O_(1-2)1_x□1_(2x)]增多,Cu~+/Cu~(2+)比例增大,表相氧空位增多,H_2-TPR还原峰温度向低温区偏移.Ce~(4+)、La~(3+)之间不平衡电荷以及共生过程中Cu-Mn-Ce-La-O之间的强相互作用,加大了Cu O和Mn O_x结构的不完整性,导致Cu Mn Ce La-O/γ-Al_2O_3催化剂样品表相产生更多的Cu~+、Mn~(2+)、Mn~(3+)和氧空位,相应的H_2-TPR还原峰温度进一步向低温区偏移.催化氧化CO和CO催化还原NO实验结果表明,在反应空速20 000 h~(-1),350℃反应温度下,Cu Mn Ce La-O/γ-Al_2O_3催化剂CO催化还原NO反应的CO转化率达到88.2%,NO转化率达到了96.1%,表现出了较好的氧化还原活性.     

Ti4+掺杂制备花状SnO2/Sn3O4异质结微米球及其光催化性能

通过水热法制备了由层状纳米片堆叠而成的花球状Sn_3O_4及x%Ti-Sn O_2/Sn_3O_4(x%为Ti与Sn的物质的量之比)。采用X射线粉末衍射、扫描电子显微镜、透射电子显微镜、X射线光电子能谱、紫外-可见漫反射光谱、红外光谱和光电流响应等物理化学方法对合成的样品进行表征分析。结果表明,由于Ti~(4+)电负性及离子半径与Sn~(4+)相似,可以很好地进入Sn_3O_4晶格中替代Sn~(4+)形成替代掺杂,但不引起大的晶格畸变。同时,掺入Ti~(4+)后使得一部分Sn~(4+)直接与O结合生成纳米球状Sn O_2颗粒分散覆盖在Sn_3O_4表面,形成Sn O_2/Sn_3O_4异质结。光催化活性表明,x%Ti-Sn O_2/Sn_3O_4不仅具有较强的还原Cr~(6+)能力,而且拥有氧化降解有机污染物甲基橙和酸性橙Ⅱ的能力。催化活性的增强归因于x%Ti-Sn O_2/Sn_3O_4具有比较大的比表面积和更强的光吸收,同时Sn O_2/Sn_3O_4异质结的生成有效地提升了光生电子与空穴的分离效率。     

焙烧温度对“软-硬”模板法制备的Pd/Ce0.65Zr0.35O2三效催化性能的影响

采用"软-硬"模板法制备了具有高热稳定性的Ce_0.65Zr_0.35O₂（CeZr）。考察了制备过程中焙烧温度对Ce_0.65Zr_0.35O₂及其负载的单Pd三效催化剂（TWC）性能的影响。对样品进行了X射线衍射、比表面、拉曼光谱、X射线光电子能谱、储氧性能和H₂程序升温还原性能测试。结果表明：焙烧温度显著影响催化剂的结构和性能。随着焙烧温度的增加，Ce_0.65Zr_0.35O₂的比表面下降，但在1 000℃焙烧的样品比表面为61 m²·g^-1，显著高于同温度下直接在空气中焙烧的样品。由于高温导致了物相重组，Ce_0.65Zr_0.35O₂的储氧量和还原性能随着焙烧温度的增加而提升。由于高温烧结导致Pd分散性的下降，其负载的催化剂的还原性能随着焙烧温度的增加而下降，从而最终导致催化剂活性的降低。但在"软-硬"模板法中1 000℃焙烧的样品负载的催化剂依然显示出很好的三效催化性能，该催化剂上C₃H₈、CO和NO的起燃温度分别为274、175和133℃，显著低于同温度下空气中直接焙烧的样品负载的催化剂。催化剂的氧化还原性能和Pd的分散性是影响催化活性的主要因素。     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Ion-beam irradiation of lanthanum compounds in the systems La2O3-Al2O3 and La2O3-TiO2

Thin crystals of La₂O₃, LaAlO₃, La_2/3TiO₃, La₂TiO₅, and La₂Ti₂O₇ have been irradiated in situ using 1 MeV Kr²⁺ ions at the Intermediate Voltage Electron Microscope-Tandem User Facility (IVEM-Tandem), Argonne National Laboratory (ANL). We observed that La₂O₃ remained crystalline to a fluence greater than 3.1×10¹⁶ ions cm⁻² at a temperature of 50 K. The four binary oxide compounds in the two systems were observed through the crystalline-amorphous transition as a function of ion fluence and temperature. Results from the ion irradiations give critical temperatures for amorphisation (T_c) of 647 K for LaAlO₃, 840 K for La₂Ti₂O₇, 865 K for La_2/3TiO₃, and 1027 K for La₂TiO₅. The T_c values observed in this study, together with previous data for Al₂O₃ and TiO₂, are discussed with reference to the melting points for the La₂O₃-Al₂O₃ and La₂O₃-TiO₂ systems and the different local environments within the four crystal structures. Results suggest that there is an observable inverse correlation between T_c and melting temperature (T_m) in the two systems. More complex relationships exist between T_c and crystal structure, with the stoichiometric perovskite LaAlO₃ being the most resistant to amorphisation.     

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.     

The reaction of MgCl2·4H2O with CCl2F2

A new reaction of MgCl₂·4H₂O with CCl₂F₂ is investigated by DTA and TG from room temperature to 350 °C. It is observed that MgF₂ was obtained between 252 and 350 °C, Below the temperature, MgCl₂·4H₂O dehydrates and hydrolyzes to MgCl₂ and Mg(OH)Cl, which are the real reactants of the reaction with CCl₂F₂. The formation of MgF₂ is ascribed to the reaction of MgCl₂ and Mg(OH)Cl with HF, which forms by decomposition of CCl₂F₂ with the taking part in of H₂O released from dehydration of hydrated magnesium chloride on the surface of MgCl₂ and Mg(OH)Cl, which catalyzes the decomposition of CCl₂F₂ in this case. Consequently, the reactions are tested in the fluid-bed condition. It is found that MgF₂ formed at temperatures down to 200 °C in a fluid-bed reactor. This reaction may be used as a method of disposing of the environmentally sensitive CCl₂F₂ (rather than release into the atmosphere). It is also a method for the preparation of MgF₂.     

(Cl2AlNH2)n和(H2AlNH2)n(n=1～5)簇结构及其热力学性质

用HF自洽场理论和密度泛函理论(DFT)的B3LYP方法,在6 31G水平上研究了低聚物(Cl2AlNH2)n和(H2AlNH2)n(n=1～5)簇的几何构型、电子结构和聚合反应热力学性质,比较了两个系列化合物中化学键的强度.结果表明,Cl2AlNH2和H2AlNH2分子为C2 (EC)平面型结构,其中Al－N为由一个σ键和一个键组成的双键.(Cl2AlNH2)n和(H2AlNH2)n(n=1～5)分子为Dnh对称,Al－N是典型的σ单键 .低聚物(Cl2AlNH2)n和(H2AlNH2)n的稳定性顺序分别为: 3 > 2 > 4> 5 > 1和8 > 7 > 9 > 11 > 6.     

The crystal structure determinations and refinements of K2S2O7, KNaS2O7 and Na2S2O7 from X-ray powder and single crystal diffraction data

The crystal structures of K₂S₂O₇, KNaS₂O₇ and Na₂S₂O₇ have been solved and/or refined from X-ray synchrotron powder diffraction data and conventional single-crystal data. K₂S₂O₇: From powder diffraction data, monoclinic C2/c, Z=4, a=12.3653(2), b=7.3122(1), , β=93.0792(7)°, R_Bragg=0.096. KNaS₂O₇: From powder diffraction data; triclinic , Z=2, a=5.90476(9), b=7.2008(1), , α=101.7074(9), β=90.6960(7), γ=94.2403(9)°, R_Bragg=0.075. Na₂S₂O₇: From single-crystal data; triclinic , Z=2, a=6.7702(9), b=6.7975(10), , α=116.779(2), β=96.089(3), γ=84.000(3)°, R_F=0.033. The disulphate anions are essentially eclipsed. All three structures can be described as dichromate-like, where the alkali cations coordinate oxygens of the isolated disulphate groups in three-dimensional networks. The K-O and Na-O coordinations were determined from electron density topology and coordination geometry. The three structures have a cation-disulphate chain in common. In K₂S₂O₇ and Na₂S₂O₇ the neighbouring chains are antiparallel, while in KNaS₂O₇ the chains are parallel. The differences between the K₂S₂O₇ and Na₂S₂O₇ structures, with double-, respectively single-sided chain connections and straight, respectively, corrugated structural layers can be understood in terms of the differences in size and coordinating ability of the cations.     

Energetics of copper diphosphates – Cu2P2O7 and Cu3(P2O6OH)2

Differential scanning calorimetry and high temperature oxide melt solution calorimetry are used to study enthalpy of phase transition and enthalpies of formation of Cu₂P₂O₇ and Cu₃(P₂O₆OH)₂. α-Cu₂P₂O₇ is reversibly transformed to β-Cu₂P₂O₇ at 338–363 K with an enthalpy of phase transition of 0.15 ± 0.03 kJ mol⁻¹. Enthalpies of formation from oxides of α-Cu₂P₂O₇ and Cu₃(P₂O₆OH)₂ are −279.0 ± 1.4 kJ mol⁻¹ and −538.8 ± 2.7 kJ mol⁻¹, and their standard enthalpies of formation (enthalpy of formation from elements) are −2096.1 ± 4.3 kJ mol⁻¹ and −4302.7 ± 6.7 kJ mol⁻¹, respectively. The presence of hydrogen in diphosphate groups changes the geometry of Cu(II) and decreases acid–base interaction between oxide components in Cu₃(P₂O₆OH)₂, thus decreasing its thermodynamic stability.     

XRD and Si MAS-NMR spectroscopy across the β-Lu2Si2O7-β-Y2Si2O7 solid solution

Samples in the system Lu_2−xY_xSi₂O₇ (0?x?2) have been synthesized following the sol-gel method and calcined to 1300 °C, a temperature at which the β-polymorph is known to be the stable phase for the end-members Lu₂Si₂O₇ and Y₂Si₂O₇. The XRD patterns of all the compositions studied are compatible with the structure of the β-polymorph. Unit cell parameters are calculated as a function of composition from XRD patterns. They show a linear change with increasing Y content, which indicates a solid solubility of β-Y₂Si₂O₇ in β-Lu₂Si₂O₇ at 1300 °C. ²⁹Si MAS NMR spectra of the different members of the system agree with the XRD results, showing a linear decrease of the ²⁹Si chemical shift with increasing Y content. Finally, a correlation reported in the literature to predict ²⁹Si chemical shifts in silicates is applied here to obtain the theoretical variation in ²⁹Si chemical shift values in the system Lu₂Si₂O₇-Y₂Si₂O₇ and the results compare favorably with the values obtained experimentally.     

EuZn2Si2 and EuZn2Ge2 Grown from Zn or Ga(ln)/Zn Flux

Single crystals of the novel ternary compounds EuZn₂Si₂ and EuZn₂Ge₂ were grown from pure gallium, indium, or zinc metal used as a flux solvent. Crystal properties were characterized using X-ray single-crystal analyses via Gandolfi and Weissenberg film techniques and by four-circle X-ray single-crystal diffractometry. The new compounds crystallize with ternary derivative structures of BaAl₄, i.e., EuZn₂Si₂ with ThCr₂Si₂-type (a=0.42607(2) nm, c=1.03956(5) nm, I4/mmm, R₁=0.038) and EuZn₂Ge₂ with CaBe₂Ge₂-type (a=0.43095(2) nm, c=1.07926(6) nm, P4/nmm, R₁=0.067). XAS and magnetic measurements on EuZn₂Si₂ and EuZn₂Ge₂ revealed in both compounds the presence of Eu²⁺ ions carrying large magnetic moments, which order magnetically at low temperatures. The magnetic phase transition occurs at T_N=16 and 7.5 K for the silicide and the germanide, respectively. In EuZn₂Si₂ there occurs a spin reorientation at 13 K and furthermore some canting of antiferromagnetically ordered moments below about 10 K. In EuZn₂Ge₂ a canted antiferromagnetic structure is formed just at T_N.