铁合金厂回收的硅微粉在不同温度下晶相结构的研究

铁合金厂冶炼过程产生的大量硅微粉烟尘, 可以作为耐火材料和窑具材料的结合剂, 活性剂和矿化剂, 可促进耐火材料固相反应和烧结, 有利于晶型的转变, 提高耐火材料的高温性能。硅微粉在高于或等于1100 ℃不析晶。1200和1300 ℃析晶规律是:首先α-石英转变为α-方石英, 然后转变为α-鳞石英。在1400～1450 ℃首先析出卡片号为290085的石英变体, 然后转变为α-方石英。 而常规转化过程是α-方石英很难形成α-鳞石英, 而且不形成290085的变体, 因此其转化规律与常规不同。在液相存在情况下, 少量α-方石英转变为α-鳞石英, 不同温度下析晶结构探讨为实际生产提供适宜的升温曲线。     

原料杂质对堇青石窑具晶相结构与性能的影响

对重青石窑具原料中的CaO，TiO2，Fe2O3以及R2O（Na2O＋K2O）对窑具多晶结构与性能的影响进行研究，从而确定原料中的Cao，TiO2，Fe2O3和R2O允许的存在量为CaO（2．2～2．7）％，TiO2（1．0～1．5）％，Fe2O3（0．8）％和R2O≤0．9％。     

氧化钇对高速CBN砂轮用陶瓷结合剂玻璃料性能的影响

在CaO-Al2O3-SiO2(CAS)系统微晶玻璃中引入稀土氧化物Y2O3,制备出用于高速CBN砂轮的微晶玻璃结合剂。结合DTA,XRD,SEM等检测手段,研究了Y2O3的加入对微晶玻璃结合剂微观结构及其性能的影响。结果表明:随Y2O3含量的增加,微晶玻璃结合剂的耐火度降低,流动性增大。当Y2O3含量为0.8%(质量分数)时,钙铝硅系微晶玻璃结合剂具有最佳的力学性能(显微硬度753.26 MPa,抗折强度167.50 MPa,磨耗比1∶8.23)。加入Y2O3会影响玻璃的析晶性能,当加入Y2O3为0.8%时,促进析出新晶相Li2Al2SiO10和β-石英,尺寸大小约为0.2～1μm,其具有致密的微观结构,利于用于作CBN砂轮的结合剂。     

SA耐火材料多晶结构与性能的研究

本实验采用磨具废砂和炉皮SiC废砂生产SA耐火材料，通过XRD分析和计算机处理确定各试样中的晶相（4H－SiC，33R－SiC，3C－SiC，α－Al2O3，β-石英和Al6Si2O13）及其各相的含量。通过材料性能与结构综合分析，确定较好的配方，其含量：磨具废砂50％，炉皮砂45％，结合剂5％，外加矿化剂2％。     

堇青石窑具多晶结构与性能研究

利用X-射线衍射分析和电子显微镜分析的结果，确定堇青石窑具的多晶结构和各晶相的含量；结合窑具性能的研究，确定堇青石窑具具有优良性能的适宜配方。     

三元复合材料K8[Fe（H2O）W11MnO39]/PANI/TiO2的制备及光催化性能

采用静电自组装法制备出三元复合材料K8[Fe（H2O）W（11）MnO（39）]/PANI/TiO2.采用IR,UV,XRD,SEM,XPS和N2吸附-脱附的表征手段对K8[Fe（H2O）W（11）MnO（39）]/PANI/TiO2进行表征,并以龙胆紫为模型,在紫外光照射下,考察了K8[Fe（H2O）W（11）MnO（39）]/PANI/TiO2对龙胆紫染料的光催化性能,确定光催化最佳条件：龙胆紫溶液浓度为5mg/L,pH=3,K8[Fe（H2O）W11MnO39]/PANI/TiO2的用量为10mg,脱色率可达92.93%.     

松香基季铵盐为模板剂有序超微孔二氧化硅的合成

以松香基季铵盐(脱氢枞基三甲基溴化铵,标记为DTAB)为模板剂、正硅酸乙酯为硅源、氨水为碱性介质成功合成出具有纳米片状形貌的六方有序超微孔二氧化硅材料。采用X射线衍射、N2吸附-脱附、透射电镜、扫描电镜等手段对样品进行表征,结果表明,体系中模板剂添加量、硅源添加量、碱性介质添加量、晶化温度、搅拌时间对前驱体的有序度有着较大的影响。当物质的量之比为nSi O2∶nDTAB∶nNH3·H2O∶nH2O=1.0∶0.1∶11.3∶924.0,晶化温度为373 K,搅拌时间为24 h,所得样品有序度最高。经煅烧后样品具有较大的比表面积(1 024 m2·g-1)和孔容(0.56 cm3·g-1),以及狭窄的孔径分布(集中于1.80 nm)。     

二丙胺的结构微调对磷酸铝分子筛晶化过程影响的凝胶组成依赖性

以二丙胺异构体(二正丙胺DPA和二异丙胺D-i PA)为结构导向剂,在200℃加热2组反应原料物质的量之比不同的初始凝胶,合成出了高结晶度的磷酸铝分子筛Al PO4-11。利用X射线粉末衍射分析、元素分析等表征手段,研究了凝胶的晶化过程和液相的p H值以及Al和P的浓度演化。初始凝胶各组分物质的量之比为nAl2O3∶nP2O5∶nDPA/D-i PA∶nH2O=1.0∶1.0∶1.2∶75时,以DPA为结构导向剂,晶化过程中无中间相生成,而以D-i PA为结构导向剂时,晶化过程中生成了具有12元环孔道结构的磷酸铝分子筛Al PO4-5中间相;初始凝胶各组分物质的量之比为nAl2O3∶nP2O5∶nDPA/D-i PA∶nH2O=1.0∶1.0∶1.0∶75时,以DPA为结构导向剂,晶化过程中生成了具有18元环孔道结构的磷酸铝分子筛VPI-5中间相,而以D-i PA为结构导向剂时,晶化过程中同时出现了VPI-5及Al PO4-5两种中间相。表明对于同一种有机胺,凝胶物质的量之比的改变影响了其结构导向效应。理论计算结果显示质子化的DPA及D-i PA中N原子上的电荷有差异,表明有机胺的结构微调影响其结构导向效应,但该影响依赖于凝胶组成。     

铒铝硼硅酸盐玻璃的析晶

通过对Er2O3-A12O3-B2O3-SiO2玻璃样品的析晶热处理,使稀土玻璃结构与晶体联系起来研究,能在一定程度上揭示稀土玻璃的结构形式。对铒铝硼硅酸盐玻璃进行了差热分析,确定其析晶热处理温度;然后对铒铝硼硅酸盐玻璃热处理后的晶相及其微观形态进行了系统地研究,发现该玻璃样品受热析晶后析出的全部为ErBO3相,且呈层状排列。这表明在受热时玻璃发生了分相,Er^3 较多地在富硼相中偏聚而析出,富硅相则保持玻璃态。而玻璃本身也可能具有微不均匀性,存在富硼和富硅两种网络结构,而Er^3 则主要分布在偏硼酸盐结构的富硼环境中,这使得其析出时容易形成层状结构。     

稀土镧掺杂MnO2电极的制备及性能研究

以Mn(CH3COO)2·4H2O为原料,利用直流电沉积法合成MnO2电极材料,在制备过程中向溶液中添加h(NO3)3·6H2O对MnO2电极进行改性.分别采用X射线衍射(XRD)、扫描电子显微镜(SEM)和原子吸收方法分析了电极的结构、形貌以及组成.通过BET分析,发现掺La后MnO2的比表面积明显增大.采用循环伏安(CV)和恒流充放电技术测试了MnO2的电化学性能.结果表明,MnO2比容量为198.72 F·g-1,掺La后MnO2的电化学性能显著改善,其比容量为276.60 F·g-1.     

Influence of MnO_2 Mineralizer on the Crystal Structure,Properties of SiC Kiln Furniture Bonded with Fine Silicon Powder

lINTRODUCTIONSiCkilnfllrniturepossessesgoodhigh-temperaturepropertiesandsmoothness.Itishighlyresistanttowarddeforming,slaggingandthermalshock.Thefurniturecanpracticallyresultinimprovingqualityandproductionofceramicsandiswidelyusedovertheworld.However,SiChassinteringtemperatureofupto2OOO:Ct13landitisdifficulttosinterasproductbyusingcommonkilnfurnace.Toserveashigh-temperaturerefractorykilnfurniture,itmustbemixedwithabonder.Thisworkus-esfinesiliconpowderasabonder,whichisadustproducedfroms…     

Synthesis, crystal structure and magnetic properties of the new one-dimensional manganate Cs3Mn2O4

Cs(3)Mn(2)O(4), a new member of the small family of ternary manganese (II/III) mixed-valent compounds, has been synthesized via the azide/nitrate route and studied using powder and single crystal X-ray diffraction, magnetic susceptibility measurements and density functional theory (DFT). Its crystal structure (P2(1)/c, Z = 8, a = 1276.33(1) pm, b = 1082.31(2) pm, c = 1280.29(2) pm, β = 118.390(2)°) is based on one-dimensional MnO(2)(1.5-) chains built up from edge-sharing MnO(4) tetrahedra. The title compound is the first example of an intrinsically doped transition metalate of the series A(x)MnO(2), (A = alkali metal) where a complete 1:1 charge ordering of Mn(2+) and Mn(3+) is observed along the chains (-Mn(2+)-Mn(3+)-Mn(2+)-Mn(3+)-). From the magnetic point of view it basically consists of ferrimagnetic MnO(2) chains, where the Mn(2+) and Mn(3+) ions are strongly antiferromagnetically coupled up to high temperatures. Very interestingly, their long-range three-dimensional ordering below the Néel temperature (T(N)) ~12 K give rise to conspicuous field dependent magnetic ordering phenomena, for which we propose a consistent picture based on the change from antiferromagnetic to ferromagnetic coupling between the chains. Electronic structure calculations confirm the antiferromagnetic ordering as the ground state for Cs(3)Mn(2)O(4) and ferrimagnetic ordering as its nearly degenerate state.     

Comparative Studies on Structure and Electronic Properties Between Thermal Lithiated Li_(0.5)MnO_2 and LiMn_2O_4

Monoclinic Li0.5MnO2 was synthesized by solid state reaction and the spectral and magnetic properties were studied in comparison with those of spinel LiMn2O4.The XRD pattern and Raman spectrum of Li0.5MnO2 are different from those of LiMn2O4,which indicate the different long-range and short-range crystal structure.XPS result shows the binding energies of 2p3/2 and 2p1/2 in Li0.5MnO2 are located at 642.3 and 653.6 eV,respectively.Through fitting the XPS spectra,the valence state of Mn ion in Li0.5MnO2 coincides with that in LiMn2O4.The high-temperature susceptibility of Li0.5MnO2 can be fitted by Curie-Weiss law whose Curie and Weiss constants are 33 A·m2·K/(mol·T) and-277(6) K,respectively.Although Li0.5MnO2 shows spin glass ground state,the transition temperature of Li0.5MnO2 is about 9 K lower than that of LiMn2O4.     

Solvent effects on the oxidation of RuIV=O to O=RuVI=O by MnO4-. hydrogen-atom versus oxygen-atom transfer

The kinetics of the oxidation of trans-[RuIV(tmc)(O)(solv)]2+ to trans-[RuVI(tmc)(O)2]2+ (tmc is 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane, a tetradentate macrocyclic tertiary amine ligand; solv = H2O or CH3CN) by MnO4- have been studied in aqueous solutions and in acetonitrile. In aqueous solutions the rate law is -d[MnO4]/dt = kH2O[RuIV][MnO4-] = (kx + (ky)/(Ka)[H+])[RuIV][MnO4-], kx = (1.49 +/- 0.09) x 101 M-1 s-1 and ky = (5.72 +/- 0.29) x 104 M-1 s-1 at 298.0 K and I = 0.1 M. The terms kx and ky are proposed to be the rate constants for the oxidation of RuIV by MnO4- and HMnO4, respectively, and Ka is the acid dissociation constant of HMnO4. At [H+] = I = 0.1 M, DeltaH and DeltaS are (9.6 +/- 0.6) kcal mol-1 and -(18 +/- 2) cal mol-1 K-1, respectively. The reaction is much slower in D2O, and the deuterium isotope effects are kx/kxD = 3.5 +/- 0.1 and ky/kyD = 5.0 +/- 0.3. The reaction is also noticeably slower in H218O, and the oxygen isotope effect is kH216O/kH218O = 1.30 +/- 0.07. 18O-labeled studies indicate that the oxygen atom gained by RuIV comes from water and not from KMnO4. These results are consistent with a mechanism that involves initial rate-limiting hydrogen-atom abstraction by MnO4- from coordinated water on RuIV. In acetonitrile the rate law is -d[MnO4-]/dt = kCH3CN[RuIV][MnO4-], kCH3CN = 1.95 +/- 0.08 M-1 s-1 at 298.0 K and I = 0.1 M. DeltaH and DeltaS are (12.0 +/- 0.3) kcal mol-1 and -(17 +/- 1) cal mol-1 K-1, respectively. 18O-labeled studies show that in this case the oxygen atom gained by RuIV comes from MnO4-, consistent with an oxygen-atom transfer mechanism.     

Synthesis and structural study on MnO2 nanosheet material by X-ray absorption spectroscopic technique

MnO2 nanosheet with acetylene black composite material has been synthesized from layered K0.45MnO2 powder. The electrochemical lithiation reaction of nanosheet composite material proceeds in a different manner from that of the parent material, layered K0.45MnO2 powder. To elucidate the origin of the changes in discharge profile, the electronic and local structures for the nanosheet composites and its parent and protonated material have been investigated by Mn K-edge and O K-edge X-ray absorption spectroscopy (XAS). The results showed that local and electronic structure around Mn ions does not vary during nanosheet formation, while significant changes in electronic structure around oxide ions were observed. Accordingly, it is suggested that the difference observed in discharge profile is due to the electronic structural change induced by nanosheet formation.     

New layered hydrogenophosphate, protonic conductor: Mn(H2PO4)2

A new hydrogenophosphate Mn(H 2PO 4) 2 has been synthesized from an aqueous solution. Its ab initio structure resolution shows that the original layered structure of this phase consists of PO 2(OH) 2 tetrahedra and MnO 5OH octahedra, sharing corners to form [MnP 2O 8H 4] infinity layers, whose cohesion is ensured through hydrogen bonds. The excitation and emission spectra of this phase are characteristic of Mn (2+) species. This phosphate is shown to be a good protonic conductor with a conductivity of 10 (-4.4) S/cm at 90 degrees C (363 K).     

Controlled synthesis, characterization, and catalytic properties of Mn(2)O(3) and Mn(3)O(4) nanoparticles supported on mesoporous silica SBA-15

A method established in the present study has proven to be effective in the synthesis of Mn(2)O(3) nanocrystals by the thermolysis of manganese(III) acetyl acetonate ([CH(3)COCH=C(O)CH(3)](3)-Mn) and Mn(3)O(4) nanocrystals by the thermolysis of manganese(II) acetyl acetonate ([CH(3)COCH=C(O)-CH(3)](2)Mn) on a mesoporous silica, SBA-15. In particular, Mn(2)O(3) nanocrystals are the first to be reported to be synthesized on SBA-15. The structure, texture, and electronic properties of nanocomposites were studied using various characterization techniques such as N2 physisorption, X-ray diffraction (XRD), laser Raman spectroscopy (LRS), temperature-programmed reduction (TPR), transmission electron microscopy (TEM), and X-ray photoelectron spectroscopy (XPS). The results of powder XRD at low angles show that the framework of SBA-15 remains unaffected after generation of the manganese oxide (MnO(x)) nanoparticles, whereas the pore volume and the surface area of SBA-15 dramatically decreased as indicated by N2 adsorption-desorption. TEM images reveal that the pores of SBA-15 are progressively blocked with MnO(x) nanoparticles. The formation of the hausmannite Mn(3)O(4) and bixbyite Mn(2)O(3) structures was clearly confirmed by XRD. The surface structures of MnO(x) were also determined by LRS, XPS, and TPR. The crystalline phases of MnO(x) were identified by LRS with corresponding out-of-plane bending and symmetric stretching vibrations of bridging oxygen species (M-O-M) of both MnO(x) nanoparticles and bulk MnO(x). We also observed the terminal Mn=O bonds corresponding to vibrations at 940 and 974 cm-1 for Mn(3)O(4)/SBA-15 and Mn(2)O(3)/SBA-15, respectively. These results show that the MnO(x) species to be highly dispersed inside the channels of SBA-15. The nanostructure of the particles was further identified by the TPR profiles. Furthermore, the chemical states of the surface manganese (Mn) determined by XPS agreed well with the findings of LRS and XRD. These results suggest that the method developed in the present study resulted in the production of MnO(x) nanoparticles on mesoporous silica SBA-15 by controlling the crystalline phases precisely. The thus-prepared nanocomposites of MnO(x) showed significant catalytic activity toward CO oxidation below 523 K. In particular, the MnO(x) prepared from manganese acetyl acetonate showed a higher catalytic reactivity than that prepared from Mn(NO(3))2.     

Interactions of O(2) with Pd nanoparticles on alpha-Al(2)O(3)(0001) at low and high O(2) pressures

The interaction of O(2) with small Pd particles (2-10 nm) supported on an alpha-Al(2)O(3)(0001) single crystal under both ultrahigh vacuum (UHV) and high-pressure conditions has been studied by temperature-programmed desorption (TPD), temperature-programmed low-energy ion scattering (TP-LEIS), and X-ray photoelectron spectroscopy (XPS). A low O(2) exposure (30 L) at 500 K leads to surface oxygen adatoms on the Pd nanoparticles, which desorb in TPD as O(2) in a peak at approximately 880 K. Surface O adatoms on the smallest Pd particles move to subsurface sites starting at 400 K, and they almost all move subsurface by approximately 750 K, desorbing mainly at considerably higher temperature. The dominant oxygen species above 700 K is subsurface, implying that it is more stable than oxygen adatoms on Pd. Exposures of the Pd nanoparticles to 25 Torr O(2) at 373-473 K readily convert the Pd to a species whose Pd XPS peak shifts by the same amount as the binding energy difference between bulk Pd and bulk PdO. We attribute this to PdO nanoparticles (or a thin film of PdO on or under the Pd for the larger particles). The decomposition of the PdO on these nanoparticles to Pd in an equilibrium O(2) pressure of 10-7 Torr does not occur until approximately 750 K, or approximately 200 K higher than the equilibrium decomposition of bulk PdO. This is attributed to the higher energy of Pd nanoparticles compared to bulk Pd and, for the larger particles, to the adhesion energy of the PdO film to the Pd, both of which stabilize the PdO on these Pd nanoparticles relative to bulk PdO. This PdO-like film on the larger particles may be similar to the ordered oxide thin film previously reported to form on Pd(111) but may also reside at the alpha-Al(2)O(3) interface and be partially stabilized by adhesion to this interface.     

低浓度甲烷甲醇深度氧化Ag/La0.6Sr0.4MnO3催化剂

用柠檬酸溶胶－凝胶法制备钙钛矿型Ｌａ０．６Ｓｒ０．４ＭｎＯ３氧化物,并用Ａｇ对其进行修饰,制得Ａｇ／Ｌａ０．６Ｓｒ０．４ＭｎＯ３系列催化剂。结果表明,６％Ａｇ／Ｌａ０．６Ｓｒ０．４ＭｎＯ３催化剂上甲烷或甲醇氧化转化９５％时的反应温度Ｔ９５可低至７３５Ｋ（对ＣＨ４）或４２１Ｋ（对ＣＨ３ＯＨ）;适量Ａｇ的负载修饰并不改变催化剂基质氧化物Ｌａ０．６Ｓｒ０．４ＭｎＯ３的纳米级钙钛矿型结构;Ａｇ的掺杂诱使催     

2D层状焦磷酸锰髤[NH_4]_2[Mn_3(P_2O_7)_2(H_2O)_2]的结构和磁性研究

由于具有开放骨架的金属磷酸盐在催化、吸附、主客体组装以及光学、磁学等方面的应用[1~3],因此合成具有开放骨架的金属磷酸盐一直吸引着人们的广泛关注。自从1982年美国联合碳化公司(U.C.C.)开发出系列磷酸铝分子筛AlPO4鄄n[4]以来,大量具有开放骨架的金属磷酸盐(金属=Ga,In,F