颗粒流体系统宏观拟颗粒模拟的并行算法

基于宏观拟颗粒模型(MaPPM), 提出了一种适合不同粒径复杂粒子系统和多相流体系统的并行算法. 利用多重网格技术, 对每个计算处理器(PE)上不同粒径级别的粒子根据其所在位置进行分区管理. 应用所设计的算法, 模拟了一个二维气-固两相流系统并测算了系统中颗粒相所受的曳力和气-固相间滑移速度随时间的变化, 以及不同时刻流场中空隙率的波动情况. 计算分析结果表明该算法具有较高的并行效率和良好的可扩展性, 也体现了MaPPM模拟复杂流体系统所具有的独特优势.     

流化颗粒显示的新方法——颗粒荧光示踪法

随着流态化研究的深入,人们对于流化颗粒统计性质外的个体运动、即位移、轨迹、速度等愈来愈感到兴趣。近年来曾有人尝试用荧光物质示踪流化颗粒。然而至今不能提供定量数据。     

纳米颗粒跟踪分析仪用于二氧化钛纳米颗粒分散及检测

以纳米颗粒跟踪分析仪为检测手段,建立了二氧化钛(TiO2)纳米颗粒分散和检测的方法,考察了分散剂种类、超声方式、超声时间、超声温度、分散试剂浓度、pH值对TiO2分散的影响,以及本分散方法对于一般商品TiO2的通用性.采用NTA测定粒径和颗粒数量浓度,对检测过程中稀释试剂浓度、稀释倍数等检测条件进行了优化,颗粒数量浓度...     

大分子颗粒乳化剂研究进展

近年来,纳米科技的蓬勃发展将颗粒乳化剂的研究热点从传统乳化领域拓展到纳米材料的制备领域。颗粒乳化剂体系也从最初的无机颗粒拓展到有机／无机复合颗粒乳化剂、聚合物颗粒乳化剂、天然大分子颗粒乳化剂等体系,并引起了科学家们的广泛关注。本文主要对大分子颗粒乳化剂近期研究进展进行了综述,介绍了颗粒乳化剂的基本概念和乳化机理,按化学...     

单颗粒-电感耦合等离子体质谱测定金纳米颗粒

单颗粒-电感耦合等离子体质谱法(Single particle-inductively coupled plasma-mass spectrometry,SPICP-MS)是近年出现的一种纳米材料分析方法,可用于表征纳米材料的元素组成、粒径分布以及颗粒物浓度。本研究对比了驻留时间(Dwell time,t_d)和稳定时间(Settling time,t_s)等质谱参数对单颗粒分析结果的影响,分析了金纳米颗粒标准物质(NIST 8012,NIST 8013,GBWE 120127)。结果表明,使用短的驻留时间(0.05 ms)和稳定时间(0 ms),可以获得更高的信噪比,检测到更多的纳米颗粒。利用本方法分析了AuNP标准物质,得到的粒径结果与标准值相符。本方法对金纳米颗粒的数量检出限为1.1×10~5L~(-1),粒径检出限为8 nm。     

空心卤化银颗粒

近年来国际上发展了一系列严格控制卤化银微晶结构和排列的新方法,如薄片颗粒(亦称T颗粒,用于Kodak VR-1000)、双层结构颗粒(DSG,用于富士HR-1600),有序颗粒(参见本刊1985,No.1,12)等,使卤化银感光材料的性能获得了很大的改进。     

单颗粒电化学分析

颗粒因其在基础研究和实际应用中均具有重要的价值,因而得到了广泛的关注.由于颗粒的功能和性质与其形貌、尺寸、电荷密度和表面化学性质等密切相关,因此,发展可用于单个颗粒(简称单颗粒)检测和分析的方法对于了解颗粒结构与性能的关系,进而研究其功能将具有重要的意义.单颗粒电化学(electrochemic alanalysis of single nanoparticle)检测技术是在最近几年发展起来的,由于其可以精确地探测单个纳米颗粒的性质(如表面电荷、几何尺寸、表面化学),因而展现出了诱人的应用前景.本文将对最近发展起来的单颗粒电化学检测方法进行详细介绍,并根据检测原理将单颗粒电化学检测分为3类:基于碰撞原理的微电极技术、基于电阻-脉冲原理的纳米通道技术以及基于电化学和其他方法的联用技术.基于此分类,重点综述单颗粒电化学检测的原理、方法和潜在的应用.     

胶体颗粒稳定的界面及胶体颗粒在界面的相互作用

Particle-stabilized dispersions such as emulsions, foams and bubbles are catching increasing attentions across a number of research areas. The adsorption mechanism and role of these colloidal particles in stabilizing the oil-water or gas-water interfaces and how these particles interact at interfaces are vital to the practical use of these dispersion systems. Although there have been intensive investigations, problems associated with the stabilization mechanisms and particle-particle interactions at interfaces still remain to explore. In this paper, we first systematically review the historical understanding of particle-stabilized emulsions or bubbles and then give an overview of the most important and well-established progress in the understanding of particle-stabilized systems, including emulsions, foams and liquid marbles. The particle-adsorption phenomena have long been realized and been discussed in academic paper for more than one century and a quantitative model was proposed in the early 1980s. The theory can successfully explain the adsorption of solid particles onto interface from energy reduction approaches. The stability of emulsions and foams can be readily correlated to the wettability of the particles towards the two phases. And extensive researches on emulsion stability and various strategies have been developed to prepared dispersion systems with a certain trigger such as pH and temperature. After that, we discuss recent development of the interactions between particles when they are trapped at the interface and highlight open questions in this field. There exists a huge gap between theoretical approaches and experimental results on the interactions of particles adsorbed at interfaces due to demanding experimental devices and skills. In practice, it is customary to use flat surfaces/interfaces as model surfaces to investigate the particle-particle at interfaces although most of the time interfaces are produced with a certain curvature. It is shown that the introduction of particles onto interfaces can generate charges at the interfaces which could possibly account for the long range electrostatic interactions. Finally, we illustrate that particle-stabilized dispersions have been found wide applications in many fields and applications such as microcapsules, food, biomedical carriers, and dry water. One of the most investigated areas is the microencapsulation of actives based on Pickering emulsion templates. The particles adsorbed at the interface can serve as interfacial stabilizers as well as constituting components of shells of colloidal microcapsules. Emulsions stabilized by solid particles derived from natural and bio-related sources are promising platforms to be applied in food related industries. Emulsion systems stabilized by solid particles of the w/w (water-in-water) feature are discussed. This special type of emulsion is attracting increasing attentions due to their all water features. Besides of oil-water interface, particle stabilized air-water interface share similar stabilization mechanism and several applications reported in the literature are subsequently discussed. We hope that this paper can encourage more scientists to engage in the studies of particle-stabilized interfaces and more novel applications can be proposed based on this mechanism     

Structural and spectroscopic investigations on the quenching free luminescence of europium oxalate nanocrystals

The structural features leading to the intense quenching free luminescence exhibited by europium oxalate nanocrystals, poly[[hexaaquatri‐μ₂‐oxalato‐dieuropium] 4.34‐hydrate], {[Eu₂(C₂O₄)₃(H₂O)₆]·4.34H₂O}_n, is the focal point of this report. Europium oxalate nanocrystals were synthesized by a simple microwave‐assisted co‐precipitation method. Powder X‐ray diffraction analysis revealed the monoclinic structure of the nanocrystals and the phase purity. The morphology and particle size were examined by transmission electron microscopy (TEM) analysis. Luminescence measurements on a series of samples of La_2–xEu_x(C₂O₄)₃·10H₂O, with x varying in the range 0.1 to 2, established the quenching free nature exhibited by the europium oxalate nanocrystals. A single‐crystal structure analysis was carried out and the quenching free luminescence is explained on the basis of the crystal structure. A detailed photoluminescence characterization was carried out using excitation and emission studies, decay analysis, and CIE coordinate and colour purity evaluation. The various spectroscopic parameters were evaluated by Judd–Ofelt theoretical analysis and the results are discussed on the basis of the crystal structure analysis.     

Thermal studies on yttrium,neodymium and holmium oxalates

The thermal decomposition patterns of Y₂(C₂O₄)₃ · 9 H₂O, Nd₂(C₂O₄)₃ · 10 H₂O and Ho₂(C₂O₄)₃ · 5.5 H₂O have been studied using TG and DTG. The hydrated neodymium oxalate loses all the water of hydration in one step to give the anhydrous oxalate while Y₂(C₂O₄)₃ · 9 H₂O and Ho₂(C₂O₄)₃ · 5.5 H₂O involve four or more dehydration steps to yield the anhydrous oxalates. Further heating of the anhydrous oxalates results in the loss of CO₂ and CO to give the stable metal oxides.     

Crystal structure and luminescence of europium(III) acrylate

The atomic structure of europium acrylate crystals [Eu₂(Acr)₅OH·3H₂O]·2(0.5H₂O) was studied by X-ray analysis (a = 24.360(3) Å, b = 18.466(2) Å, c = 8.5818(9) Å, β = 96.087(2)°, space group C2/c, Z = 6, ρ_calc = 2.036 g/cm³). The crystal structure involves chains of binuclear [Eu₂(C₃H₃O₂)₅OH·3H₂O] molecules, running infinitely in the [101] direction and having pairs of C₉H₉EuO₇H₂O molecules alternating with C₆H₆EuO₄OH·2H₂O molecules that link the pairs. The infinite chains are linked by hydrogen bonds and van der Waals interactions. The thermal behavior of luminescence of the europium(III) complex is discussed.     

Two bismuth oxalate hydrates and revision of their chemical formulae

The crystal structures of two bismuth(III) oxalate hydrates, previously described as `Bi<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub>·H<sub>2</sub>C<sub>2</sub>O<sub>4</sub>' and `Bi₂(C₂O₄)₃·7H₂O', were solved and refined from single‐crystal X‐ray diffraction data. The results led to the revised chemical formulae Bi₂(C₂O₄)₃·6H₂O and Bi₂(C₂O₄)₃·8H₂O, respectively. Both dibismuth(III) trioxalate hexahydrate (tetra­aqua­tri‐μ‐oxalato‐dibismuth(III) dihydrate, {[Bi₂(C₂O₄)₃(H₂O)₄]·2H₂O}_n) and dibismuth(III) trioxalate octahydrate (tetra­aqua­tri‐μ‐oxalato‐dibismuth(III) tetrahydrate {[Bi₂(C₂O₄)₃(H₂O)₄]·4H₂O}_n) are characterized by a three‐dimensional network of Bi atoms connected by tetradentate oxalate groups. All ligand and `free' water mol­ecules are located in channels and voids. The mean Bi—O bond lengths are ∼2.51 Å. The lone electron pairs on all Bi³⁺ cations are stereochemically inactive.     

Sur un nouveau Complexe entre l'oxyfluorure d'antimoine et l'oxalate. Structure cristalline de (NH4)4H2(C2O4)3(SbOF) 2 · H2O

On a New Complex of Antimony Oxide Fluoride and Oxalate. Crystal Structure of (NH₄)₄H₂(C₂O₄)₃(SbOF) ₂ · H₂O The crystal structure of (NH₄)₄H₂(C₂O₄)₃(SbOF) ₂ · H₂O has been fixed by X-ray diffraction on single crystal (R = 0.025 for 2124 planes). The antimony atom is complexed by the oxalate anions which are bidendate chelates. Antimony coordination is seven (five oxygen atoms, one fluorine atom, and the lone pair E). Antimony environment is a pentagonal bipyramid, one of the axial positions is occupied by the lone pair, the other one by the fluorine atom.     

3D Coordination Polymer Incorporating Discrete Molecular Octahedra

Copper(II) oxalate coordination polymer [{Cu₄(C₂O₄)₄(L)₄}₃ · {Cu₃(C₂O₄)₃(L)₆}₂ · 3L · 25H₂O]_n (L = 3,3′,5,5′‐tetramethyl‐4,4′‐bipyrazole) reveals a structure that is related to the Pt₃O₄ net topology. The 3D linkage is sustained with copper‐oxalate squares and copper‐bipyrazole triangles sharing vertices. The framework supports giant icosahedral cages and entraps discrete molecular octahedra formed by two molecular complexes Cu₃(C₂O₄)₃(L)₆ associated by means of NH‐‐‐N hydrogen bonding. The coexistence of the discrete and 3D portions formed by the same components suggests self‐templation as a key feature of the system. Simpler copper oxalate compounds [Cu(C₂O₄)(L)₂(H₂O)] · CH₃OH · 3.75H₂O and [Cu₂(C₂O₄)₂(L)₅] · L · 11H₂O are concomitant products of the reaction mixture and they exist in the form of molecular mono‐ and binuclear complexes.     

Synthesis, characterisation and thermal properties of [Cu(VO)2(C2O4)3(4,4′-bpy)2·2H2O]A 2D polymer

The heterometallic complex [Cu(VO)₂(C₁₀H₈N₂)₂(C₂O₄)₃·2H₂O] has been prepared and characterised by electronic and IR spectra, molecular electrical conductivity and thermal behaviour. A polymeric structure is proposed with oxalate and 4,4′-dipyridine acting as bridging ligands and VO(IV) of C_4v symmetry and Cu(II) in octahedral surrounding the oxalate anion V_4h.     

Supramolecularly assembled water layers stabilized by sebacic anions in complexes of Zn(II) and Co(II)

Two three-dimensional supramolecular water architectures, [Zn(phen)₃]₂·[Zn(C₁₀H₁₆O₄)·(H₂O)₃]·(C₁₀H₁₆O₄)₂·20H₂O (1) and [Co(phen)₃]₂·[Co(H₂O)₆]·(C₁₀H₁₆O₄)₃·30H₂O (2) [phen = 1,10-Phenanthroline, C₁₀H₁₆O₄ = sebacic dianion], have been synthesized and characterized by IR, elemental analysis, thermogravimetric analysis, and single-crystal X-ray diffractions. The two structures both contain extensive hydrogen bonding between water molecules as well as between water molecules and sebacic anions. The water molecules and sebacic acid O atoms assembled 2D supramolecular corrugated sheets with different morphology in the two complexes.     

Oxalate-2-ethanolamine complexes of some bivalent cations (Mn,Co, Ni,Cu, Zn and Cd)

On the refluxing ofM(II) oxalate (M=Mn, Co, Ni, Cu, Zn or Cd) and 2-ethanolamine in chloroform, the following complexes were obtained: MnC₂O₄·HOCH₂CH₂NH₂·H₂O, CoC₂O₄·2HOCH₂CH₂NH₂, Ni₂(C₂O₄)₂·5HOCH₂CH₂NH₂·3H₂O, Cu₂(C₂O₄)₂·5HOCH₂CH₂NH₂, Zn₂(C₂O₄)₂·5HOCH₂CH₂NH₂·2H₂O and Cd₂(C₂O₄)₂·HOCH₂CH₂NH₂·2H₂O. Following the reaction ofM(II) oxalate with 2-ethanolamine in the presence of ethanolammonium oxalate, a compound with the empirical formula ZnC₂O₄·HOCH₂CH₂NH₂·2H₂O¹ was isolated. The complexes were identified by using elemental analysis, X-ray powder diffraction patterns, IR spectra, and thermogravimetric and differential thermal analysis. The IR spectra and X-ray powder diffraction patterns showed that the complexes obtained were not isostructural. Their thermal decompositions, in the temperature interval between 20 and about 900°C, also take place in different ways, mainly through the formation of different amine complexes. The DTA curves exhibit a number of thermal effects.     

Synthesis,open-framework structure and thermal behaviour of ammonium tin oxalate,Sn2(NH4)2(C2O4)3·3H2O

A new mixed ammonium tin oxalate trihydrate, Sn₂(NH₄)₂(C₂O₄)₃·3H₂O, has been prepared from evaporation of a solution of tin and ammonium oxalates. Its crystal structure has been solved from single-crystal diffraction data. The symmetry is orthorhombic, space group Pnma (No. 62), cell dimensions a=15.1821(5) Å, b=11.7506(2) Å, c=10.8342(3) Å, and Z=4. The structure consists of macroanionic layers built from [Sn(C₂O₄)₃]^2– groups. The SnO₆ polyhedron can be described as a pseudo pentagonal bipyramid, with the lone pair of electrons presumably occupying one apex. The resulting framework displays holes in which the water molecules and ammonium groups are located. The thermal behaviour of the mixed ammonium tin oxalate has been investigated with temperature-dependent X-ray powder diffraction and conventional thermal analysis. The degradation process has been completely explained, as well as that of oxammite, a phase always obtained in the preparations. The thermal decomposition of oxammite leads to (NH₄)₂C₂O₄ and a new acid salt, NH₄HC₂O₄. The mixed ammonium tin oxalate decomposes successively into the amorphous compounds, Sn₂(NH₄)₂(C₂O₄)₃·H₂O and Sn₂(NH₄)₂(C₂O₄)₃, SnC₂O₄ and, finally, cassiterite SnO₂.