分子筛对NO和NO2的吸附性能

在常压下研究了多种分子筛上NO和NO2的吸附和脱附情况.结果表明,有O2存在时,O2与NO生成的NO2可与NO共吸附在分子筛上,显著促进了NO在分子筛特别是Na型分子筛上的吸附.在所研究的ZSM-5,13X,SAPO,Y,β和A分子筛中,Hβ分子筛在无氧条件下对NO的吸附能力最强;13X分子筛在有氧条件下对NOx的吸附能力最强,且对NOx的吸附性能具有很好的重复性.     

无氧条件下Pd/CeO2催化剂表面NH3还原NO过程中N2O形成机理研究

氮氧化物(NO_x,主要包括NO和NO_2)是主要的大气污染物之一,造成酸雨,光化学烟雾和臭氧层破坏等环境问题,甚至直接危害人体健康.化石燃料燃烧和汽车尾气排放是NO_x的主要来源,严格控制火力发电厂,大型锅炉,汽车尾气等污染源中NO_x的排放刻不容缓.以NH_3为还原剂选择性催化还原NO_x(NH_3-SCR)是目前公认的最有效的NO_x脱除技术,然而在催化NO_x还原为N_2的过程中往往伴随着副产物N_2O的生成,降低了催化剂的选择性,造成温室气体效应和破坏臭氧层等环境问题.因此充分理解NH_3-SCR过程中N_2O的形成机理对于抑制N_2O的产生、提高催化剂的选择性十分重要.本文将高度分散的Pd纳米团簇负载在Ce O_2纳米棒上制成Pd/Ce O_2催化剂,结合NH_3-TPD, NO-TPD和原位傅里叶转换红外光谱等表征手段研究了无氧条件下该催化剂上利用NH_3催化还原NO过程中N_2O的产生路径.结果表明, N_2O的形成途径与反应温度和反应气体的浓度相关.当反应气体中NH_3含量大于化学计量比时,在反应温度低于200°C时,由NH_3活化产生的吸附态H·自由基与催化剂表面吸附的NO反应先生成中间产物HON,两个HON分子进一步反应生成N_2O;过量的吸附态的H·自由基也可以与HON反应生成N_2,所以低温下(200°C)随着反应气氛中NH_3的增加,解离生成的H·也随之增加,促进反应向着生成N_2的方向进行,从而抑制了N_2O的产生.随着反应温度增加, NH_3解离产生的H·被CeO_2表面的O捕获形成羟基,中间产物HON的生成被切断,从而阻断了N_2O的生成.同时由于体系中含有大量的NH_3,吸附态的NO会优先与活化态的NH_3物种反应生成N_2,阻碍了NO解离生成N_2O这一过程的发生,因此NH_3过量情况下在高温下观察不到N_2O的产生,可获得100%的N_2选择性.但是当反应气体中的NH_3含量不足时,即体系中含有过量的NO,当反应温度高于250°C, NO可在催化剂表面解离生成吸附态的N·自由基和O·自由基, N·自由基可进一步与吸附态的NO反应生成N_2O, NO的解离是N_2O生成的速控步,还原性吸附物种对O·自由基的捕捉将有利于N_2O的生成.当反应温度介于200–250°C, NH_3解离产生的H·自由基既可以与NO结合生成HON中间产物,又能被CeO_2表面的O捕获形成羟基,两个反应之间存在竞争,此时N_2O产生与反应气体浓度之间的关系不再呈单调变化.     

γ-Mo2N催化剂上H2及NO吸附性质的TPD-MS研究

采用TPD-MS方法研究了H2及NO在γ-Mo2N上的吸附状况．单独的H2-TPD结果表明,当H2在673K吸附时,在443K、573K及723K得到了三个H2脱附峰,表明γ-Mo2N上有三种不同能量的H2吸附位．NO－TPD结果表明,NO吸附后亦有三个脱附峰（383K、493K、543K）,对应着γ-Mo2N上三种不同能量的NO吸附位：低、中、高能吸附位．NO既可以以解离状态,又可以以一种NO三聚态（dimerordinitrosyl）的形式吸附在γ－Mo2N上,这些吸附物种在脱附过程中产生大量的N2及少量的N2O.对比NO吸附在不同处理条件的γ-Mo2N上的TPD结果可知,NO是吸附在γ-Mo2N上的MO的配位不饱和中心上,这些吸附中心既可通过还原催化剂,又可通过在773K抽空钝化态的γ－Mo2N而产生,H2和NO共吸附的结果表明,预吸附H2再吸附NO后,H2和NO的脱附量均大大减少,且只有两个脱附峰出现.NO只在363K及493K出现两个脱附峰,表明预吸附氢占据了NO的强吸附位,且NO很难取代它,从而使NO只能吸附在能量较低的吸附位上;而H2只在523K及723K出现两个脱附峰,且伴随着H2的脱出有N2和H2O的产生,表明在γ－Mo2N上NO可能与预吸附氢形成了一种复合相MoHx（NO）y,它在脱附时分解为H2、N2及H2O.     

介质阻挡放电引发氮氧化物等离子体化学反应

在523 K介质阻挡放电条件下,研究了不同气体组分体系中NO的转化.实验表明,在无氧体系(NO/N2)中,转化的NO主要分解为N2和O2.在富氧(NO/O2/N2)条件下,由于NO和NO2的生成, NO的转化率最低.体系中加入C2H4(NO/C2H4/N2)时, NO转化率与NO/N2体系几乎一样,与NO相比,生成的O更易与C2H4作用,几乎没有NO2的生成.当C2H4和O2共存时(NO/O2/C2H4/N2),NO主要被氧化为NO2.当能量密度为125 J•L－1时, 与其它体系相比,NO/O2/C2H4/N2体系中NO转化率和NO2生成量最大,转化每个 NO分子能耗最小(61 eV).体系中C2H4主要被氧化为CO.四个体系中N2O的生成量都较少.讨论了介质阻挡放电条件下上述四个体系可能的反应机制.     

V2O5-CeO2/TiO2催化剂上低温氨选择性催化还原NO的性能

考察了V2O5-CeO2/TiO2催化剂中V、Ce活性组分的担载量和焙烧温度对催化剂低温催化还原NO活性的影响及其在单独SO2、H2O和两者共存气氛下的抗毒化性能。结果表明,焙烧温度400℃下制备的5V30Ce/TiO2催化剂具有良好的低温催化还原NO活性,空速为10000h-1,165℃时NO转化率达99.2%;500℃以下低焙烧温度时,添加的Ce不与V相互作用,在催化剂表面主要以CeO2形式存在,有利于增大催化剂比表面积,增强V2O5在催化剂上的分散度,提高催化活性。而在500℃以上较高焙烧温度下,Ce与V会形成CeVO4,对活性提高不利。催化剂具有良好的低温抗水中毒性能,但受SO2毒化作用明显,其在SO2、H2O共存气氛下中毒程度较单独SO2下浅。     

富氧条件下钯催化剂上氢气还原氧化氮微观反应动力学研究

 通过单位键指标-二次指数势(UBI-QEP)方法估算反应的表观活化能进行反应机理的随机模拟,并结合实验结果研究了富氧条件下Pd基催化剂上H2还原NO的反应. 结果表明,反应的控制步骤是H2吸附活化产生H*(*表示活性位,H*表示吸附的H原子)的过程,当反应温度低于270 ℃时, H*来自基元反应O*+H*2OH*+H*,反应温度上升到310 ℃时, H*2+*2H*成为H*的主要来源. NO以(NO)*2的形式吸附在Pd催化剂表面,还原产物N2O来自两条途径,分别是(NO)*2的分解以及相邻的两个NO*分子之间的结合; N2主要来自N2O*的分解以及相邻的N*和NO*分子的结合; NH3则由中间产物HNO*经过逐步加氢生成. 富氧条件下, NO和O2之间存在吸附和反应的竞争,低温下NO在Pd表面的吸附几率远大于O2, 此时H2优先还原NO. 反应温度的升高导致各物种的吸附能力下降,其中NO的降低最明显,因此高温下催化剂表面的主要吸附物种由NO变为O2, 此时H2优先与O2反应. 在150～310 ℃范围内,实验结果和模拟数据非常吻合.     

NO在Au／Al2O3催化剂上还原反应的TPD-MS研究

 考察了沉积－沉淀法制备的Au／Al2O3催化剂在O2存在下催化C3H6还原NO的反应，并用程序升温脱附－质谱（TPD－MS）手段研究了吸附于催化剂上的NO或NO－O2的脱附性能．结果表明：在O2存在的条件下，对于C3H6还原NO的反应，1％Au／Al2O3的催化活性最高，可于375℃左右使NO生成N2，转化率达60％．这与催化剂对所吸附NO的脱附性能密切相关，N2O可能是C3H6还原NO反应过程中产生的比较稳定的中间体．     

影响CeO2纳米粉体尺寸的液相反应因素研究

较为系统地论述了沉淀法制备高纯度CeO2纳米粉体过程中影响颗粒团聚的液相工艺参数.实验结果表明, 在如下液相反应条件下制备得到的纳米CeO2平均尺寸小于10 nm; Ce(NO3)4溶液浓度为0.13～0.18 mol*L-1, NH3*H2O浓度为6.8 mol*L-1, 反应温度15～30 ℃, VCe(NO3)4∶VNH3*H2O=1.5∶20～2.5∶20, 分散剂选用乙醇+异丙醇.     

介质阻挡放电等离子体辅助CuO/CeO2-TiO2/r-Al2O3

在介质阻挡等离子体放电(DBD)辅助催化剂(6%CuO/15%TiO2/γ-Al2O3,6%CuO/5%CeO2/15%TiO2/γ-Al2O3)反应装置上,研究了4种不同反应条件下(NO+CH4,NO+CH4+O2,NO+CH4+NTP,NO+CH4+O2+NTP)NO和CH4反应,采用BET、XRD、H2-TPR和XPS等手段对催化剂进行了表征.结果表明在上述4种反应条件下,对于NO+CH4的反应,O2的存在有利于NO脱除,在等离子体条件下,O2的加入对NO的转化有所抑制;而等离子体的活化极大增强了NO的低温脱除活性.在等离子体存在条件下,6%CuO/5%CeO2/15%TiO2/γ-Al2O3(6Cu5Ce15TA)对NO的转化率都优于6%CuO/15%TiO2/γ-Al2O3(6Cu15TA).BET结果显示添加TiO2和CeO2于γ-Al2O3表面后,比表面积都有少量降低;而各载体负载6%CuO后比表面积也有所下降.XRD结果表明6Cu15TA和6Cu5Ce15TA催化剂由锐钛矿相TiO2组成,CuO在各催化剂表面呈现高度分散.H2-TPR数据和XPS实验结果显示负载CuO后,催化剂表面的铜物种由高度分散的CuO和嵌入到CeO2或TiO2晶格中Cu2+所组成.6Cu5Ce15TA表面含有较6Cu15TA多的Cu+,从而增强了NO的脱除活性.     

t-ZrO2/α-Al2O3超细晶复合粉体的低温燃烧合成

以Al(NO3)3*9H2O、ZrO(NO3)2*2H2O和Y(NO3)3*6H2O为原料,采用低温燃烧合成(LCS)法制备了多种不同ZrO2/Al2O3比的复合粉体,对其物相和形貌进行了表征.实验结果表明,采用LCS法在400℃合成的t-ZrO2/α-Al2O3复合粉体晶粒超细,其结晶程度随ZrO2/Al2O3比的增加逐渐降低,晶粒大小也随ZrO2/Al2O3比的变化而有规律地变化.     

Sc2MgGa2 and Y2MgGa2

Scandium magnesium gallide, Sc₂MgGa₂, and yttrium magnesium gallide, Y₂MgGa₂, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo₂FeB₂‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc₂MgGa₂ was determined from single‐crystal diffraction intensities and the isostructural Y₂MgGa₂ was identified from powder diffraction data.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

Summary The ability of [MoS₄]^2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe²⁺. The present study has been restricted to linear complexes such as (NEt₄)₂ [Cl₂FeS₂MoS₂] and (NEt₄)₂[Cl₂FeS₂MoS₂FeCl₂]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS₂, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl₂]^2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl₄Fe₂MoS₄]^2–[Cl₂FeMoS₄]^2–+FeCl₂. The equilibrium constant, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

The structures of the hypophosphites KH₂PO₂ (potassium hypophosphite), RbH₂PO₂ (rubidium hypophosphite) and CsH₂PO₂ (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

On Dialkali Metal Dichalcogenides β-Na₂S₂, K₂S₂, α-Rb₂S₂, β-Rb₂S₂, K₂Se₂, Rb₂Se₂, α-K₂Te₂, β-K₂Te₂ and Rb₂Te₂ The first presentation of pure samples of α- and β-Rb₂S₂, α- and β-K₂Te₂, and Rb₂Te₂ is described. Using single crystals of K₂S₂ and K₂Se₂, received by ammonothermal synthesis, the structure of the Na₂O₂ type and by using single crystals of β-Na₂S₂ and β-K₂Te₂ the Li₂O₂ type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na₂O₂ type to the Li₂O₂ type will be explained by means of the examples α-/β-Na₂S₂ and α-/β-K₂Te₂. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb₂S₂ is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(n‐Bu)₂Sn(O₂PPh₂)₂] ( 1 ), and [Ph₂Sn(O₂PPh₂)₂] ( 2 ) have been synthesized by the reactions of R₂SnCl₂ (R=n‐Bu, Ph) with HO₂PPh₂ in Methanol. From the reaction of Ph₂SnCl₂ with diphenylphosphinic acid a third product [PhClSn(O₂PPh₂)OMe]₂ ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P2₁/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)₂ linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

Photoionization Mass Spectra of SCl₂, S₂Cl₂, and S₂Br₂ Photoionization mass spectra of SCl₂, S₂Cl₂, and S₂Br₂ have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.