六水合硝酸镁增塑改性淀粉-聚乙烯醇复合膜的合成与性能

以六水合硝酸镁[Mg(NO₃)₂·6H₂O]为增塑剂, 采用流延法制备了增塑改性的淀粉-聚乙烯醇(PVA)复合膜, 并研究了改性后淀粉-PVA复合膜的性能. 研究结果表明, Mg(NO₃)₂·6H₂O与淀粉和PVA发生一定的相互作用, 破坏了淀粉和PVA中的结晶结构. 因此, Mg(NO₃)₂·6H₂O的加入可提高淀粉与PVA间的相容性, 改变了淀粉-PVA复合膜的力学性能, 使其拉伸强度下降, 断裂伸长率提高.     

Preparation and characterization of a novel single crystal of Th(IV) with cucurbit[6]uril

One new single crystal [Th(NO₃)₂(H₂O)₆](CB₆)(NO₃)2·2H₂O was prepared using Th(NO₃)4·4H₂O and cucurbit[6]uril (CB₆) as reagents in HNO₃ aqueous solution by slow evaporation. The coordination number of Th⁴⁺ is ten. Th⁴⁺ is coordinated with six monodentate water molecules and two symmetric bidentate chelating nitrate ions, while other two nitrate ions act as the counterion anions. CB₆ is a second-sphere ligand which is hydrogen bonded to the water molecules of [Th(NO₃)₂(H₂O)₆]²⁺. Besides, there are also two free water molecules in the crystal system.     

喷雾热解制备稀土超细粉末(Ⅰ)——氧化钇粒子形态与形成机理

对Y(NO₃)₃·6H₂O的差热和热重分析表明,Y(NO₃)₃·6H₂O经脱水和热分解在580C以上完全分解为Y₂O₃.在此基础上,以Y(NO₃)₃·6H₂O为前驱体,采用喷雾热解过程制备出粒度为0.50～1.50μm的立方相球形Y₂O₃粉末.通过对产物粒子粒度的理论计算与实验结果的比较,推测Y₂O₃粒子形成机理符合液滴-粒子转变机理(One-Droplet-One-Particlemechanism).本喷雾热解过程同样适用于其它稀土超细粉末的制备,粒子粒度可以通过调节液滴尺寸和溶液浓度等操作条件进行控制.     

稀土冠醚类络合物的研究(Ⅲ)——硝酸钪与邻苯二酮-17-冠-5及邻苯二酮-14-冠-4固态络合物的合成与性质

制得硝酸钪与两种冠醚的固态络合物,确定其组成为Sc(NO₃)₃·C₁₆H₂₀O₇·H₂O及Sc(NO₃)₃·C₁₄H₁₆O₆·H₂O。研究了冠醚本身及其钪的相应络合物的合成及有关性质。     

锌(Ⅱ)配合物的超分子设计及对甲醇蒸气的吸附性能

采用饱和蒸气扩散技术, 将2,4-二羟基苯甲醛缩异烟酰腙(H₂dhbi)配体分别与Zn(ClO₄)₂·6H₂O和Zn(NO₃)₂·6H₂O进行配位作用, 得到2种不同配位模式的金属-有机框架材料[(dhbi)₂Zn₂·8H₂O]_n(1)和{[(dhbi)₂(H₂O)₂Zn₂]·4DMF]}_n(2). 利用X射线单晶衍射、 热分析技术(TG-DTA)和X射线粉末衍射(PXRD)等方法进行了结构表征. 进一步将配位聚合物1和2用于对甲醇分子的吸附性能研究, 结果表明, 化合物1是一种理想的微孔材料, 其对甲醇分子的吸附能力为化合物2的近5倍, 采用PLATON对材料的孔隙体积进行计算得到化合物1和2的孔隙率分别为38.2%和5.5%.     

稀土冠醚类配合物的研究(Ⅺ)——硝酸钪、钇与二苯并-24-冠-8的固态配合物的合成及性质

以无水乙腈为反应介质,合成了硝酸钪及硝酸钇与DB24C8的固态配合物,确定其组成为Sc(NO₃)₃·DB24C8·2H₂O和[Y(NO₃)₃]₄·(DB24C8)₃·8H₂O,并对冠醚及其配合物的某些性质进行了对比研究。     

Mg-MOF-74对CO2/H2O的吸附性能

以Mg(NO₃)₂·6H₂O和2,5-二羟基对苯二甲酸为原料, 采用溶剂热法制备了金属有机骨架材料Mg-MOF-74. 利用X射线衍射(XRD)、 红外光谱(FTIR)和扫描电子显微镜(SEM)等测试手段对其结构、 形貌和性能进行了分析, 并利用自制穿透实验装置研究了产物吸附CO₂/H₂O的性能. 结果表明: 合成的样品纯度高, 结构完整, 形貌规则有序, 具有较高的CO₂吸附量. 双组分CO₂/H₂O穿透实验结果证实, 在水蒸气存在情况下, 与沸石13X相比, Mg-MOF-74仍具有较高的CO₂吸附能力, 可用于分离高湿烟道气中的CO₂.     

新型镁配合物[Mg(phen)2(H2O)2]·2HPbsa的合成与荧光性质

以Mg(NO₃)₂、苯基苯并咪唑-5-磺酸(H₂Pbsa)和1,10-邻菲罗啉（phen）为原料,采用水热法合成了单核镁配合物[Mg(phen)₂(H₂O)₂]·2HPbsa （1）,产率88%,其结构和性能经FL、 IR、元素分析、X-射线单晶衍射和TGA表征。结果表明：1中镁离子为六配位,与phen配体中的4个氮原子以及两个水分子中的氧原子配位形成扭曲的八面体配位构型。与配体相比,配合物1的荧光发射峰发生了红移,最大发射峰位于525 nm。     

系列Sm3+配合物的合成、结构及光物理性能

采用水热方法合成了4种Sm³⁺配合物, 即{[SmZn(2,5-pdc)₂(tp)_0.5(H₂O)]·2H₂O}_n(1), [Sm₂Zn₂(C₆H₅COO)₁₀(Imh)₂(H₂O)₂](2), {[Sm₂(NO₂C₆H₄COO)₆(H₂O)₄]·H₂O}_n(3)和{[SmN(CH₂COO)₃(H₂O)₂]·H₂O}_n(4)[2,5-pdc=2,5-吡啶二羧酸根, tp=对苯二甲酸根, C₆H₅COO=苯甲酸根, Imh=咪唑, NO₂C₆H₄COO=对硝基苯甲酸根, N(CH₂COO)₃=氨三乙酸根]. 通过单晶X射线衍射确定了其晶体结构. 在室温下测定了其红外光谱、 紫外-可见-近红外光谱以及在近红外区和可见区的发射光谱. 结果表明, 4种配合物在近红外区或可见区均出现Sm³⁺离子的特征发射. 这是形成配合物后, Zn-配体部分和配体对Sm³⁺离子发光的敏化作用所致. 此外, 讨论了不同有机配体或d过渡金属离子对Sm³⁺离子发光的影响, 并分析了配合物中Sm³⁺离子的近红外发射带位移、 劈裂和加宽的原因.     

多苯并咪唑锰( Ⅱ )配合物的合成及对DNA凝聚的促进作用

以多苯并咪唑配体1,1,4,7,7-五(2-苯并咪唑甲基)-二乙基三胺(DTPB)为主配体, 合成了锰(Ⅱ)配合物[Mn(DTPB)Ac]Ac·8H₂O(1)和[Mn₂(DTPB)(NO₃)₂(H₂O)₂][Mn₂(DTPB)(NO₃)₂(H₂O)(CH₃OH)]·(NO₃)₄·5CH₃OH·H₂O(2), 并对其进行了表征. 利用紫外-可见吸收光谱和黏度实验研究了配合物1和2与DNA的相互作用, 发现这2个配合物均能与DNA结合, 并对配合物与DNA作用的机理进行了探讨. 利用琼脂糖凝胶电泳和直角光散射(RALS)技术研究了配合物1和2促进DNA凝聚的性质. 结果表明, 在近中性条件下2个配合物都能促使DNA凝聚. 利用透射电子显微镜(TEM)观察了不同凝聚体的形态.     

EuI2—LiI和EuI2—NaI二元体系相图

用ＤＴＡ和Ｘ射线粉末衍射法研究了ＥｕＩ２－ＮａＩ和ＥｕＩ２－ＬｉＩ两个二元体系低压相图。ＥｕＩ２－ＮａＩ二元体系相图为一简单低共熔相图，低共熔点为４０９℃，其低共熔摩尔组成为３２％ＮａＩ；ＥｕＩ２－ＬｉＩ体系相图也为一简单低共熔相图。低共熔点为３８５℃，低共熔摩尔组成为６８．５％ＬｉＩ。     

LaCl_3－SrCl_2－MgCl_2三元体系相图

本文借助于ＤＴＡ和Ｘ射线结构分析测定了ＬａＣｌ_３－ＳｒＣｌ_２－ＭｇＣｌ_２三元体系相图，发现它属简单低共熔型，体系内有对应于ＬａＣｌ_３、ＳｒＣｌ_２和ＭｇＣｌ_２的３个液相面、３条２次结晶线和１个三元低共熔点Ｅ（１５．０ｗｔ％ＬａＣｌ_３，４９．５ｗｔ％ＳｒＣｌ_２，３５．５ｗｔ％ＭｇＣｌ_２；５４５℃），并且在固相下有一个不稳定的化合物生成，在约５００℃时分解。     

Phase study of the system Li2Se-In2Se3

The binary system Li₂Se-In₂Se₃ was investigated in the range of 40 to 100 mol% In₂Se₃ by thermoanalytical and X-ray methods. The system is characterized by two eutectic points. Beside the two binary components and the known ternary compound LiInSe2 another ternary compound crystallizes in this binary system at 83.3 mol% In₂Se₃. This compound was identified as LiIn₅Se₈. In contrast to (Cu, Ag)^IB₅ ^IIIC₈ ^VI compounds such as CuIn₅S₈ [1] it does not crystallize in the spinel structure. LiIn₅Se₈ shows a stratified structure. The melting point was determined to be at 810°C. Starting from room temperature up to the melting point no phase transitions were observed. This revised version was published online in July 2006 with corrections to the Cover Date.     

High Temperature Phase Transitions in Na_xCoO_2 Materials

1 INTRODUCTION In recent years, much attention has been focused on the NaxCoO2 system due to its notable properties and potential technologic applications as a cathode material in high-energy density, reversible solid state battery systems[1, 2]. Recently, large thermoelectric power[3～6] in NaxCoO2 and superconductivity (～4 K) in hydrated NaxCoO2yH2O (x = 0.35, y = 1.33) ma- terial have been observed[7]. This hydrated layered phase is the first 3d-transition metal oxide with superco…     

TiO_2的相变和热力学性质(英文)

利用第一性原理平面波赝势密度泛函理论方法对TiO2从金红石结构到萤石结构的相变进行了理论研究,并且通过准谐德拜模型分别得到了金红石和萤石结构TiO2的热力学性质.计算结果与实验值以及其它理论计算的结果都符合得很好,通过吉布斯能的计算得到TiO2从金红石结构到萤石结构的相变压强为47.74GPa,并成功地获得了相对体积(V/V0)、德拜温度(Θ)和热容(CV)随压强(p)和温度(T)的变化关系.     

聚合物-溶剂-超临界CO_2三元体系的相行为

研究了聚合物－超临界二氧化碳二元体系溶解性,并考查了添加共溶剂对溶解性的影响,结果表明,添加共溶剂会大大提高ＣＯ２的溶解度．此外,还研究了聚合物－溶剂－超临界二氧化碳三元体系在高压时的相行为,探讨了组分性质、含量等对温度 压力相图的影响．随着ＣＯ２含量的增加,压力－温度相图Ｌ－ＬＶ（单一液相向液气两相共存）边界线的斜率会出现突变点,发生由Ｌ－ＬＶ边界线向Ｌ－ＬＬ（单一液相向液液两相共存）边界线的过渡,而Ｌ－ＬＶ边界线对不同聚合物并不敏感．     

Phase relations in the system ZnV2O6 -ZnFe2O4

Using DTA and XRD methods, a diagram of phase equilibria in ZnV₂O₆-ZnFe₂O₄ system has been constructed. System ZnV₂O₆-ZnFe₂O₄ is in subsolidus area a real binary system and its components form a compound Zn₂FeV₃O₁₁. Zn₂FeV₃O₁₁ melts incongruently at 835±5°C with deposition of two solid phases: b-Zn₂V₂O₇ and ZnFe₂O₄. This revised version was published online in July 2006 with corrections to the Cover Date.     

Die Phase La2U2N5

In the system U–La–N a new phase of composition La₂U₂N₅ was observed. The differaction pattern of this phase can be indexed with a tetragonal unit cell:a=8.43 Å,c=8.50 Å andc/a=1.008. The pseudocubic sub-cell withaca/2 is closely related to the CsCl-type.

Auszug aus der von der Technisch-Naturwissenschaftlichen Fakuktät der TU Wien approbierten Diplomarbait des Herrn Dipl.-Ing.J. Waldhart.     

吸附相反应技术制备纳米TiO2/SiO2复合材料

以SiO₂表面形成的吸附层为反应器,在载体表面制备了纳米TiO₂粒子.溶剂置换实验直接给出了吸附层的存在以及吸附层作为纳米反应器的实验证据,TEM,XRD和电子能谱分析表明,载体表面形成一层比较均匀的纳米粒子.初步探讨了温度和反应物浓度对产物分布的影响,分析了各种现象产生的可能成因.     

Time‐Resolved High and Low Temperature Phase Transitions of the Nanocrystalline Cubic Phase in the Y2O3‐ZrO2 and Fe2O3‐ZrO2 System

The nanocrystalline cubic Phase of zirconia was found to be thermally stabilized by the addition of 2.56 to 17.65 mol % Y₂O₃ (5.0 to 30.0 mol % Y, 95.0 to 70.0 mol % Zr cation content). The cubic phase of yttria stabilized zirconia was prepared by thermal decomposition of the hydroxides at 400°C for 1 hr. 2.56 mol % Y₂O₃‐ZrO₂ was stable up to 800°C in an argon atmosphere. The samples with 4.17 to 17.65 mol % Y₂O₃ were stable to 1200°C and higher. All samples at temperatures between 1450°C to 1700°C were cubic except the sample with 2.56 mol % Y₂O₃ which was tetragonal. The crystallite sizes observed for the cubic phase ranged from 50 to 150 Å at temperatures below 900°C and varied from 600 to 800 nm between 1450°C and 1700°C. Control of furnace atmosphere is the main factor for obtaining the cubic phase of Y‐SZ at higher temperature. Nanocrystalline cubic Fe‐SZ (Iron Stabilized Zirconia) with crystallite sizes from 70 to 137 Å was also prepared at 400°C. It transformed isothermally at temperatures above 800°C to the tetragonal Fe‐SZ and ultimately to the monoclinic phase at 900°C. The addition of up to 30 mol % Fe(III) thermally stabilized the cubic phase above 800°C in argon. Higher mol % resulted in a separation of Fe₂O₃. The nanocrystalline cubic Fe‐SZ containing a minimum 20 mol % Fe (III) was found to have the greatest thermal stability. The particle size was a primary factor in determining cubic or tetragonal formation. The oxidation state of Fe in zirconia remained Fe³⁺. Fe‐SZ lattice parameters and rate of particle growth were observed to decrease with higher iron content. The thermal stability of Fe‐SZ is comparable with that of Ca‐SZ, Mg‐SZ and Mn‐SZ prepared by this method.