甲烷二氧化碳重整制合成气的镍基催化剂性能 Ⅰ.制备条件和载镍量的影响

甲烷二氧化碳重整制合成气的镍基催化剂性能Ⅰ．制备条件和载镍量的影响许峥李玉敏张继炎张鎏（天津大学化工系，天津３０００７２）韩森何菲（天津大学碳一化工国家重点实验室，天津３０００７２）关键词甲烷，二氧化碳，重整，镍，氧化铝，负载型催化剂甲烷二氧化碳重整...     

甲烷在Ni/TiO2催化剂表面的活化

考察了Ni/TiO2催化剂甲烷部分氧化和二氧化碳重整制合成气的反应活性,实验表明,以TiO2为载体的镍系催化剂对于甲烷部分氧化制合成气反应具有较好的活性,尤其对H2的选择性较高,对二氧化碳重整制合成气反应具有较好的低温反应活性.采用脉冲-质谱在线分析等技术,在无气相氧条件下向Ni/TiO2催化剂脉冲CH4,发现甲烷在催化剂表面的活化（转化）及其氧化产物的选择性与金属催化剂表面氧的浓度密切相关.CH4与Ni/TiO2催化剂作用过程中存在明显的氢溢流和氧溢流现象,可能是这种溢流效应使得Ni/TiO2催化剂具有良好的反应活性和抗积碳性能.     

双金属镍-锰／γ-Al2O3催化剂对甲烷二氧化碳重整反应的影响

用浸渍法制备γ-Al2O3负载的Ni-Mn双金属催化剂．在500-700。C按照17：17：2的C02／CHa／N2比例,以36mL／min的载气流速进行甲烷二氧化碳重整反应,利用甲烷二氧化碳的转化率、生成的合成气H2／CO比例以及长期稳定性等指标评价了催化剂的催化性能．实验表明,添加Mn提高催化性能并使双金属催化剂的稳定性更高,比单金属催化剂更好地抑制焦炭生成,Mn最合适的添加量为0．5wt％．通过BET、C02-TPD、TGA、XRD、SEM、EDX和FTIR各种技术对催化剂进行了表征．     

CH_4/CO_2重整制合成气Ni/Ce_xZr_(1-x)O_2催化剂性能研究

以水热法合成的介孔铈锆固溶体为载体,采用浸渍法制备了Ni/CexZr1-xO2催化剂,使用X射线衍射(XRD)、程序升温还原(TPR)和热重-差示扫描量热分析(TG-DSC)等测试手段对催化剂进行了表征。通过对比以ZrO2,CeO2,Ce0.6Zr0.4O2和Ce0.33Zr0.67O2为载体的Ni基催化剂性能,发现铈锆固溶体独特的氧化还原性质可以提高活性组分的分散度,增强催化剂的抗积炭性能,从而提高催化剂对甲烷二氧化碳重整制合成气的选择性。     

甲烷二氧化碳重整反应中微量氧化镁助剂对Ni基催化剂抗积碳性能的影响（英文）

甲烷二氧化碳重整反应不仅可以将两种温室气体转化为更具有工业应用价值的合成气,而且反应产物中的H_2/CO比也比较适宜合成气的深加工过程,兼具环境效益和经济效益,因此受到广泛的关注与研究.但是,阻碍该过程工业化的主要问题在于反应中Ni基催化剂非常容易积碳,从而导致催化剂失活.近年来,甲烷二氧化碳催化重整领域的研究主要集中在反应机理和催化剂设计,其中大多数的研究结果表明,Ni基催化剂的抗积碳性能取决于反应过程中积碳速率与消碳速率之间的平衡.CO_2是该反应体系中唯一的氧源,因此Ni基催化剂的消碳能力在很大程度上取决于其对CO_2裂解活化能力的强弱.早期的文献中一般认为,CO_2的裂解活化与载体的Lewis碱性位点强弱相关,因此添加碱性氧化物助剂,比如MgO和CaO等,能够增强Ni基催化剂的碱性强度和CO_2吸附性能,有利于催化剂表面碳物种的转化,从而增强催化剂的稳定性.已有文献报道,添加微量MgO助剂(1 wt%)尽管没有影响Ni基催化剂的碱性强度,但是能够明显增强Ni基催化剂的稳定性,但没有对此结果给出明确的解释.在非均相催化研究领域中,活性金属与助剂在催化剂表面的分散性,是研究其催化作用的重要前提.大部分甲烷二氧化碳催化重整研究工作中,助剂的引入通常采用浸渍法,但是这种制备方法并不能有效保证助剂的分散度.本研究工作利用了水滑石材料的"记忆效应",将0.42 wt%Mg~(2+)引入到由Ni-Al水滑石前驱体焙烧后得到的Ni/Al_2O_3催化剂中.X射线能谱仪的结果表明,微量MgO助剂均匀分散在Ni/Al_2O_3催化剂表面上.经X射线衍射、CO_2程序升温脱附和H_2程序升温还原表征验证,添加微量的MgO助剂并没有对Ni晶粒尺寸、金属载体相互作用以及Al_2O_3载体表面碱性强度产生明显作用;然而甲烷二氧化碳重整活性评价测试和反应后催化剂的O2程序升温氧化实验结果显示,微量MgO助剂能明显增强Ni/Al_2O_3催化剂的稳定性,并且有效地阻碍了石墨碳在催化剂表面的形成.表面脉冲吸附实验结果证实,微量MgO助剂促进了CO_2在Ni颗粒表面的裂解活化,进而可以及时消除Ni金属表面由甲烷裂解产生的碳物种,防止其迁移、聚集和生成石墨碳.     

Ba调变复合氧化物LaxBa1-xNiAl11O19-δ催化剂的制备和性能表征

制备了Ba调变Ni基复合氧化物催化剂LaxBa1-xNiAl11O19-δ,并通过XRD、XPS、TPR、TEM、BET和TGA等技术对催化剂的结构、性质和对甲烷二氧化碳重整制合成气反应的催化性能以及催化剂表面积炭情况进行了表征.结果表明,Ba调变后复合氧化物的微观结构随Ba调变量发生规律性变化,但结构的改变对催化剂的理化性质和催化性能均无明显影响,该系列Ni基复合氧化物都具有较好的催化活性以及较高的抗烧结和抗积炭性能,是甲烷二氧化碳重整制合成气反应选择氧化的良好催化剂.     

甲烷二氧化碳重整制合成气钴基催化剂

温室效应是人类面临的巨大挑战,温室气体的转化利用因而成为广泛研究的热点和难点课题。甲烷二氧化碳重整,即干重整制合成气因为可以同时将两种温室气体(CH-4/CO_2)转化为可用于清洁能源生产的合成气(H_2/CO)而被认为是极具前景的先进技术。此技术目前仍未大规模工业化,其主要瓶颈在于尚未研发出合适的催化剂。过渡金属催化剂因其高活性和相对低廉的成本而被认为最具工业化前景,此前的研究主要集中在镍基催化剂,但是镍基催化剂易因表面积碳和金属烧结而快速失活。近年来,研究者发现钴基催化剂在甲烷二氧化碳重整中也具有良好的催化性能,并进行了初步的研究。本文将对钴基重整催化剂的研究现状进行简要综述。论文首先介绍了催化剂的活性组分、载体、助剂以及制备方法等对钴基催化剂重整性能的影响,接着阐述了钴基催化剂的重整反应机理以及积碳-消碳过程,最后对钴基重整催化剂的设计及未来研究方向进行了展望。     

Yb_2O_3助剂对Ni/SiC催化剂甲烷二氧化碳重整性能的影响

采用浸渍法制备了Ni/SiC和Ni-Ybx/SiC(x=2%、4%、6%、10%,质量分数)催化剂,在固定床反应装置中考察了催化剂在甲烷二氧化碳重整反应中的性能。利用BET、ICP-AES、XRD、H2-TPR、TG-DTA、XPS和TEM等技术对催化剂进行了表征。实验结果表明,Yb的适宜添加量为4%~6%。在800℃条件下Ni-Yb4/SiC和Ni-Yb6/SiC催化剂具有优异的催化活性和稳定性,在100 h的重整反应中,甲烷和二氧化碳的转化率始终保持在90%以上。Yb2O3助剂能够抑制镍颗粒的生长和减少碳沉积量,因此,Ni-Yb/SiC催化剂在连续反应中表现出稳定的活性。     

镧助剂对模拟生物沼气重整制备合成气中Ni/SBA-15催化剂结构和性能的影响

以介孔分子筛SBA-15为载体, 采用浸渍法制备了镍质量分数(w)为12.5%, 并且分别添加质量分数(w)为2.5%的镧、铈、镁、钙、锶等助剂的系列Ni基催化剂. 以CH4/CO2体积比为2:1的模拟生物沼气和适量氧气作为原料气, 在常压固定床反应器上评价了催化剂对模拟生物沼气重整制合成气的反应性能. 采用X射线粉末衍射(XRD)、N2吸附/脱附、透射电子显微镜(TEM)、X射线光电子能谱(XPS)及H2程序升温还原(H2-TPR)等对催化剂的结构进行了表征. 催化活性评价显示, 添加镧助剂的2.5%La/12.5%Ni/SBA-15催化剂比添加铈、镁、钙、锶等助剂的催化剂具有更高的催化活性, 并且具有很好的稳定性. 因此, 文中着重研究了镧助剂对催化剂结构和模拟生物沼气重整制合成气的反应性能的影响. 结果表明, 镧能明显提高Ni/SBA-15催化剂的表面镍含量, 同时还具有很好的抗积炭作用, 在850 ℃的温度下反应820 h没有发现积炭生成, 这些可能是提高催化剂性能和稳定性的重要因素.     

六铝酸盐SrNiAl11O19-δ催化二氧化碳重整甲烷制合成气反应研究

本文通过品格取代作用,制备了以Ni为活性组分的六铝酸盐复合氧化物催化剂SrNiAl11O19-δ并通过XRD,XPS,TPR等实验技术,对催化剂的结构和性质进行了表征.结果表明,六铝酸盐SrNiAl11O19-δ对二氧化碳重整甲烷制合成气反应具有良好的催化活性和稳定性,在780℃反应2小时,CH,和CO2转化率分别为95.0%和93.4%,没有发现活性组分Ni高温烧结和催化剂失活.     

Ba3 (VO4)2-K2 Ba(MoO4)2 and Pb3 (VO4)2-K2 Pb(MoO4)2 systems

Phase equilibria in the Ba₃(VO₄)₂-K₂Ba(MoO₄)₂ and Pb3(VO₄)₂-K₂Pb(MoO₄)₂ systems have been investigated. In the first system, a continuous series of substitutional solid solutions with the palmierite structure is formed, and in the second one, the polymorphic transition in lead orthovanadate at 100°C restricts the extent of the palmierite-type solid solution to 10–100 mol % K₂Pb(MoO₄)₂. Original Russian Text ? V.D. Zhuravlev, Yu.A. Velikodnyi, A.S. Vinogradova-Zhabrova, A.P. Tyutyunnik, V.G. Zubkov, 2008, published in Zhurnal Neorganicheskoi Khimii, 2008, Vol. 53, No. 10, pp. 1746–1748.     

Investigation of phase equilibria in the systems K2SO4Sc2(SO4)3, Rb2SO4Sc2(SO4)3 and Cs2SO4Sc2(SO4)3

Phase diagrams of the systems K₂SO₄Sc₂(SO₄)₃, Rb₂SO ₄Sc₂(SO₄)₃ and Cs₂SO₄ Sc₂(SO₄)₃ have been investigated by X-ray diffraction phase analysis and differential thermal analysis techniques. A salient feature of all the systems is the formation of M₃Sc(SO₄)₃, which melt incongruently, and MSc(SO₄)₂, which on heating decompose in the solid state.     

Luminescence properties of efficient X-ray phosphors of YBa3B9O18, LuBa3(BO3)3, α-YBa3(BO3)3 and LuBO3

The samples of YBa₃B₉O₁₈, LuBa₃(BO₃)₃, α-YBa₃(BO₃)₃ and LuBO₃ powders have been synthesized by the solid-state reaction methods at high temperature and their X-ray excited luminescent properties were investigated. All the studied materials show a broad emission band in the wavelength range of 300-550 nm with the peak centers at about 385 nm for YBa₃B₉O₁₈ and LuBa₃(BO₃)₃, 415 nm for α-YBa₃(BO₃)₃ and 360 nm for LuBO₃ powders, respectively. Even though those compounds have the different atomic structures, they have the common structural feature of each yttrium or lutetium ion bonded to six separate BO₃ groups, i.e., octahedral RE(BO₃)₆ (RE=Lu or Y) moiety. This octahedral RE(BO₃)₆(RE=Lu or Y) moiety seems to be an important structural element for efficient X-ray excited luminescence of those compounds, as are the edge-sharing octahedral TaO₆ chains for tantalate emission.     

Synthesis and molecular structures of heptafluoroisopropylated fullerenes: C60(i-C3F7)8, C60(i-C3F7)6, and C60(CF3)2(i-C3F7)2

One isomer of C₆₀(i-C₃F₇)₈, three isomers of C₆₀(i-C₃F₇)₆, and the first mixed perfluoroalkylated fullerene, C₆₀(CF₃)₂(i-C₃F₇)₂, have been isolated by HPLC from a mixture prepared by reaction of C₆₀ with heptafluoroisopropyl iodide in a glass ampoule at 260-290 °C. The molecular structures of the four new compounds have been determined by means of X-ray single crystal diffraction partially also by use of synchrotron radiation. Theoretical calculations at the DFT level of theory have been employed to rationalize the energetics of isomers and of C₆₀-R_f binding.     

Syntheses, structures, and properties of Ag4(Mo2O5)(SeO4)2(SeO3) and Ag2(MoO3)3SeO3

Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) has been synthesized by reacting AgNO₃, MoO₃, and selenic acid under mild hydrothermal conditions. The structure of this compound consists of cis-MoO₂²⁺ molybdenyl units that are bridged to neighboring molybdenyl moieties by selenate anions and by a bridging oxo anion. These dimeric units are joined by selenite anions to yield zigzag one-dimensional chains that extended down the c-axis. Individual chains are polar with the C₂ distortion of the Mo(VI) octahedra aligning on one side of each chain. However, the overall structure is centrosymmetric because neighboring chains have opposite alignment of the C₂ distortion. Upon heating Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) looses SeO₂ in two distinct steps to yield Ag₂MoO₄. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): orthorhombic, space group Pbcm, a=5.6557(3), b=15.8904(7), c=15.7938(7) Å, V=1419.41(12), Z=4, R(F)=2.72% for 121 parameters with 1829 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ was synthesized by reacting AgNO₃ with MoO₃, SeO₂, and HF under hydrothermal conditions. The structure of Ag₂(MoO₃)₃SeO₃ consists of three crystallographically unique Mo(VI) centers that are in 2+2+2 coordination environments with two long, two intermediate, and two short bonds. These MoO₆ units are connected to form a molybdenyl ribbon that extends along the c-axis. These ribbons are further connected together through tridentate selenite anions to form two-dimensional layers in the [bc] plane. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): monoclinic, space group P2₁/n, a=7.7034(5), b=11.1485(8), c=12.7500(9) Å, β=105.018(1) V=1002.7(2), Z=4, R(F)=3.45% for 164 parameters with 2454 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ decomposes to Ag₂Mo₃O₁₀ on heating above 550 °C.     

Synthesis and structural investigation of the compounds containing HF2 anions: Ca(HF2)2, Ba4F4(HF2)(PF6)3 and Pb2F2(HF2)(PF6)

Three new compounds Ca(HF₂)₂, Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) were obtained in the system metal(II) fluoride and anhydrous HF (aHF) acidified with excessive PF₅. The obtained polymeric solids are slightly soluble in aHF and they crystallize out of their aHF solutions. Ca(HF₂)₂ was prepared by simply dissolving CaF₂ in a neutral aHF. It represents the second known compound with homoleptic HF environment of the central atom besides Ba(H₃F₄)₂. The compounds Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) represent two additional examples of the formation of a polymeric zigzag ladder or ribbon composed of metal cation and fluoride anion (MF⁺)_n besides PbF(AsF₆), the first isolated compound with such zigzag ladder. The obtained new compounds were characterized by X-ray single crystal diffraction method and partly by Raman spectroscopy. Ba₄F₄(HF₂)(PF₆)₃ crystallizes in a triclinic space group P1¯ with a=4.5870(2) Å, b=8.8327(3) Å, c=11.2489(3) Å, α=67.758(9)°, β=84.722(12), γ=78.283(12)°, V=413.00(3) Å³ at 200 K, Z=1 and R=0.0588. Pb₂F₂(HF₂)(PF₆) at 200 K: space group P1¯, a=4.5722(19) Å, b=4.763(2) Å, c=8.818(4) Å, α=86.967(10)°, β=76.774(10)°, γ=83.230(12)°, V=185.55(14) ų, Z=1 and R=0.0937. Pb₂F₂(HF₂)(PF₆) at 293 K: space group P1¯, a=4.586(2) Å, b=4.781(3) Å, c=8.831(5) Å, α=87.106(13)°, β=76.830(13)°, γ=83.531(11)°, V=187.27(18) Å³, Z=1 and R=0.072. Ca(HF₂)₂ crystallizes in an orthorhombic Fddd space group with a=5.5709(6) Å, b=10.1111(9) Å, c=10.5945(10) Å, V=596.77(10) Å³ at 200 K, Z=8 and R=0.028.     

Vibrational spectra of the peroxotantalates (NH4)3[Ta(O2)4], K3[Ta(O2)4], Rb3[Ta(O2)4] and Cs3[Ta(O2)4] and the crystal structure of Rb3[Ta(O2)4]

The compounds (NH₄)₃[Ta(O₂)₄], K₃[Ta(O₂)₄], Rb₃[Ta(O₂)₄] and Cs₃[Ta(O₂)₄] have been prepared and investigated by X-ray powder methods as well as Raman- and IR-spectroscopy. In the case of Rb₃[Ta(O₂)₄] the structure has been solved from single crystal data. It is shown that all these compounds are isotypic and crystallize in the K₃[Cr(O₂)₄] type (SG , No. 121). The infrared- and Raman spectra (recorded on powdered samples) are discussed with respect to the internal vibrations of the peroxo-group and the dodecahedral [Ta(O₂)₄]³⁻ ion. Symmetry coordinates for the [Ta(O₂)₄]³⁻ ion are given from which the vibrational modes of the O-O stretching vibrations of the O₂²⁻ groups, the Ta-O stretching vibrations and the Ta-O bending vibrations are deduced.     

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。     

Vapour-liquid equilibrium data for the systems C2H6 + N2, C2H4 + N2, C3H8 + N2, and C3H6 + N2

High pressure vapour-liquid equilibrium data for the C₂H₆ + N₂, C₂H₄ + N₂, C₃H₈ + N₂, and C₃H₆ + N₂ systems are presented. The data are obtained isothermally in the range from 200 K to 290 K. For each point of data, temperature, pressure and liquid and vapour phase mole fractions are measured.Values for the vapour phase mole fractions are calculated from the obtained pressure, temperature and liquid phase mole fractions. The calculated values are compared with the experimental results, and it is found that the average mean deviation between calculated and experimental mole fractions is less than 0.009 for the systems considered in this work.     

Synthesis and crystal structure of gallosilicate- and aluminogermanate tetrahydroborate sodalites Na8[GaSiO4]6(BH4)2 and Na8[AlGeO4]6(BH4)2

Tetrahydroborate enclathrated sodalites with gallosilicate and aluminogermanate host framework were synthesized under mild hydrothermal conditions and characterized by X-ray powder diffraction and IR spectroscopy. Crystal structures were refined in the space group P-43n from X-ray powder data using the Rietveld method. Na₈[GaSiO₄]₆(BH₄)₂: a=895.90(1) pm, V=0.71909(3)×10⁻⁶ nm³, R_P=0.074, R_B=0.022, Na₈[AlGeO₄]₆(BH₄)₂: a=905.89(2) pm, V=0.74340(6)×10⁻⁶ nm³, R_P=0.082, R_B=0.026. The tetrahedral framework T-atoms are completely ordered in each case and the boron atoms are located at the centre of the sodalite cages. The hydrogen atoms of the enclathrated anions were refined on x, x, x positions, restraining them to boron-hydrogen distances of 116.8 pm as found in NaBD₄.The IR-absorption spectra of the novel phases show the typical bands of the tetrahedral group as found in the spectrum of pure sodium boron hydride.The new sodalites are discussed as interesting -containing model compounds which could release pure hydrogen.