碳前驱体CH3ArCH2NH2的热解性能及动力学研究

通过密闭压力容器法、常压DSC、高压DSC及紫外分光光度定量分析法等实验手段,对液相沉积法制碳／碳复合材料用碳前驱体CH3ArCH2NH2的热裂解行为进行了研究,获得不同温度、不同压力下该碳前驱体的热分解温度和残碳率,用等温动力学和非等温动力学方法获得了热裂解反应的表观活化能,实验结果表明,常压热裂解温度大约为530．15－556．55K,1－3MPa的高压范围内的热裂解温度大约在618．34－675．49K,密闭压力容器中的残碳率为56．23％,常压下的残碳率为28．96％－36．47％,而高压下残碳率可达59．11％,根据基辛格等方法获得了等温条件下和非等温条件下热裂解反应的表观活化能Ea分别为206．78kJ/mol和183．93kJ/mol, 反应级数N~1.     

碳前驱体CH3ArCH2NH2热解反应的热力学和动力学DFT研究

在实验研究基础上,通过量子化学理论计算对碳前驱体CH3ArCH2NH2的热裂解机理作了进一步的研究.利用Gaussian98程序包中AM1方法及DFTUB3LYP/3-21G*方法,对化合物5种可能热裂解路径的热力学和动力学计算结果表明,CH3ArCH2NH2热裂解的主反应路径为生成自由基CH3ArCH2*和NH2*,其主反应路径AM1计算的活化能Ea=230.78kJ/mol,DFT计算的活化能Ea=321.18kJ/mol;比较键焓计算的数据与相应的实验数据,发现DFT计算结果与实验结果吻合得较好;通过分析优化的反应物及产物自由基的部分结构参数,了解了理论支持主反应的原因;计算的产物自由基的空间构型表明主反应路径生成的产物自由基相互间若进行稠环缩合反应,将获得分子平面取向性很好的稠环芳烃产物.     

碳前驱体CH3ArCH2NH2热解反应的热力学和动力学DFT研究

在实验研究基础上 ,通过量子化学理论计算对碳前驱体 CH3 Ar CH2 NH2 的热裂解机理作了进一步的研究 .利用 Gaussian98程序包中 AM1方法及 DFT UB3 LYP/3 -2 1 G*方法 ,对化合物 5种可能热裂解路径的热力学和动力学计算结果表明 ,CH3 Ar CH2 NH2 热裂解的主反应路径为生成自由基 CH3 Ar CH2 ·和 NH2 · ,其主反应路径 AM1计算的活化能 Ea=2 3 0 .78k J/mol,DFT计算的活化能 Ea=3 2 1 .1 8k J/mol;比较键焓计算的数据与相应的实验数据 ,发现 DFT计算结果与实验结果吻合得较好 ;通过分析优化的反应物及产物自由基的部分结构参数 ,了解了理论支持主反应的原因 ;计算的产物自由基的空间构型表明主反应路径生成的产物自由基相互间若进行稠环缩合反应 ,将获得分子平面取向性很好的稠环芳烃产物     

ZrB2/SiC前驱体的制备、表征及裂解行为

以聚锆氧烷为锆源,聚硼硅氮烷兼作硼源、硅源和碳源,通过共混得到ZrB2/SiC液相前驱体,该前驱体经高温裂解得到ZrB2/SiC复相陶瓷.对ZrB2/SiC前驱体的裂解行为、陶瓷产物结构及微观形貌进行了表征.结果表明,ZrB2/SiC前驱体经1400℃裂解后保持无定形状态,1500℃处理后析出t-ZrO2晶体,1600℃时体系发生碳热还原反应生成ZrC,同时析出SiC晶体,1700℃时生成ZrB2,最终陶瓷产物晶相组成为ZrB2/SiC.在1500~2000℃范围内,随着处理温度的升高,陶瓷由致密结构变为多孔结构,最终陶瓷产物由尺寸为100~300 nm的纳米颗粒堆积而成,各元素分布均匀.     

以甲苯为前驱体化学液气相沉积法制备碳/碳复合材料

以甲苯为前驱体利用化学液气相沉积法,采用碳布叠层作预制体,于950℃下沉积9h制备了密度为1.63g/cm³的碳/碳复合材料.用金相显微镜、扫描电子显微镜(SEM)和X射线粉末衍射(XRD)等手段对所得的材料进行了组织结构分析,并测定了其力学性能.实验结果表明,以甲苯为前驱体利用该方法可以制备组织结构比较均匀的碳/碳复合材料.用GC/MS气相色谱质谱联用仪对甲苯热分解产物(不挥发成分)进行了成分分析,提出了甲苯裂解制备碳/碳复合材料的初期热裂解机理和热缩聚机理.     

碳/碳复合材料碳源化合物乙苯热裂解机理的热力学研究

主要采用Gaussian 03程序中的密度泛函理论(DFT),在UB3LYP/6-31G*水平上对碳材料用碳源化合物乙苯的初期热裂解反应机理进行了研究.对反应物和产物的结构进行了能量梯度法全优化,计算了不同温度下(298～1573 K)的热力学参数.结果表明:在298～1573 K下,热力学首先支持生成甲苯自由基和甲基自由基的反应为主反应路径.低温下,生成苯乙基自由基(α位脱氢)的反应比例大于生成苯基自由基的反应,而高温下(823 K),生成苯基自由基的反应比例大于苯乙基自由基(α位脱氢)的反应.     

聚合物前驱体方法低温合成LiTaO3纳米粉体

采用聚合物前驱体方法,以柠檬酸为配位剂,乙二醇为酯化剂,低温合成纳米LiTaO3粉体.以红外光谱和拉曼光谱研究了柠檬酸与金属离子的配位情况.当柠檬酸和金属离子物质的量的比为2.5:1、柠檬酸和乙二醇的物质的量比为1:2时可形成稳定的Li-Ta前驱体溶胶.用差热.热重对凝胶前驱体的热分解历程进行分析,采用X射线衍射和红外光谱对Li-Ta凝胶前驱体及不同温度下煅烧所得粉体的相组成进行分析.结果表明,凝胶前驱体经600℃下煅烧2 h可以得到纯钙钛矿型纳米LiTaO3粉体.平均粒径为60～80 nm.     

用不同前驱体制备的Co/SiO2催化剂的结构及其CO2/CH4重整反应性能

分别采用硝酸钴、醋酸钴、硫酸钴和氯化钴为前驱体制备了Co/SiO     

Ru 前驱体对 Ru/MgO-CeO2 氨合成催化剂性能的影响

 分别以 K₂RuO₄, Ru(Ac)₃ 和 RuCl₃ 为 Ru 前驱体, 制备了 Ru/MgO-CeO₂ 催化剂, 并运用 X 射线衍射、X 射线荧光光谱, CO 吸附、N₂ 物理吸附和 H₂程序升温还原等技术对催化剂进行了表征, 考察了 Ru 前驱体对 Ru/MgO-CeO₂ 催化剂氨合成性能的影响. 结果表明, Ru 前驱体对载体 MgO-CeO₂ 和 Ru 的还原性能、氯残留量和催化剂比表面积的影响都很大, 从而导致催化剂的氨合成性能的不同. 其中以 K₂RuO₄ 为 Ru 前驱体制备的催化剂的载体和 Ru 容易还原, 无氯离子, 且比表面积较高, 因而催化剂活性和氨合成转换频率较高. 在 10 MPa, 425 °C, 10 000 h^-1 条件下, K₂RuO₄, Ru(Ac)₃ 和 RuCl₃ 作前驱体制备的催化剂上氨合成转换频率比为 1.33:1.05:1.     

前驱体溶液pH值对V2O5-WO3/TiO2催化剂的低温NH3-SCR性能的影响

采用调节前驱体溶液pH值的方法制备了用于低温NH₃-SCR的V₂O₅-WO₃/TiO₂催化剂。通过XPS、Raman光谱、H₂-TPR、NH₃-TPD、NH₃-DRIFT、XRD及物理吸附等手段对催化剂进行了表征分析,并对其脱硝催化活性进行了测试。结果表明,前驱体溶液酸性的增强能够提高催化剂表面聚合态钒物种和V⁴⁺⁽³⁺⁾/V⁵⁺的比值以及表面酸性,增加活性位数量、降低反应的活化能、提高其脱硝催化性能。因此,通过提高前驱体溶液的酸性,有助于制备出脱硝活性较好的NH₃-SCR催化剂。     

表面配体调控的CH3NH3PbBr3纳米片的聚集自组装

采用热注入的方法合成了CH3NH3Pb Br3纳米片,荧光光谱分析发现稀释一定的倍数会使荧光光谱由451 nm红移到531nm。TEM及XRD分析表明,发光红移是由CH3NH3Pb Br3纳米片聚集自组装导致的颗粒变大引起的。进一步的对比实验表明,油胺在纳米片聚集自组装的过程中起到了至关重要的作用,由此结合XRD和TEM表征,阐述了CH3NH3Pb Br3纳米片聚集自组装的机理。     

Layered structure of the silver coordination polymer with nonrigid aromatic diamine {Ag[CH2(C6H4NH2)2]2(CH3C6H4NH2)}NO3

The complex [Ag(DDM)₂(CH₃C₆H₄NH₂)]NO₃, where DDM is 4,4-diaminodiphenylmethane [CH₂(C₆H₄NH₂)₂], was synthesized and its structure was determined. The crystals are monoclinic, space group P2₁/n, a = 9.543(2) ?, b = 18.056(4) ?, c = 1.901(2) ?, β = 106.94(3)°, V = 1796.8(6) ?³, ρ_calcd = 1.443 g/cm³, Z = 4. The Ag atom (at the inversion center) is coordinated at the vertices of an almost undistorted octahedron by six nitrogen atoms of the primary amino groups from four bridging DDM molecules and two terminal p-toluidine molecules (Ag-N, 2.546(3) ?; NAgN, 89.7–90.3°). Wavelike layers composed of conjugate multiunit metal rings, each containing four Ag⁺ ions and four bridging DDM ligands, are formed in the structure in the [101] direction (a 2D polymer). Uncoordinated NO ₃ ⁻ anions are arranged in the cavities between the layers and link them by N-H⋯O hydrogen bonds. Original Russian Text ? Yu.V. Kokunov, V.V. Kovalev, Yu.E. Gorbunova, 2007, published in Zhurnal Neorganicheskoi Khimii, 2007, Vol. 52, No. 12, pp. 1992–1998.     

Infrared multiple-photon dissociation of N2H4 and CH3NH2 fluence dependence of the production of NH2

The multiple-photon dissociation of N₂H₄ and CH₃NH₂ by pulsed CO₂ laser light to produce NH₂(X?²B_I has been studied using the laser-induced fluorescence detection method. The relative NH₂ yield, represented by the fluorescence signal, has been measured as a function of the fluence from the threshold at about 0.1 J/cm² to about 100 J/cm², at different CO₂-laser lines and at pressures down to 10^?4 Torr.     

CH3NO2和CH3自由基吸氢反应途径和变分速率常数计算

采用MP2(full)/6-311G(d, p)从头算方法,优化了硝基甲烷和甲基自由基吸氢反应的过渡态结构,经QCISD(T)方法进行能量校正,得出该反应的正逆向反应的活化位垒分别是58.21 kJ•mol－1和67.17 kJ•mol－1.沿IRC分析指出该反应是氢转移协同反应,而且在反应途径上存在一个引导反应进行的振动模式,这一反应模式引导反应进行的区间在反应坐标S的-0.9～1.0(amu)1/2bohr之间;在温度为800～2600 K范围内,运用改进的变分过渡态理论(ICVT),计算了该反应的速率常数,并与实验类比所得的速率常数随温度的变化趋势进行了比较.     

Low-temperature single crystal X-ray diffraction and high-pressure Raman studies on [(CH3)2NH2]2[SbCl5]

The structure of bis(dimethylammonium) pentachloroantimonate(III), [(CH₃)₂NH₂]₂[SbCl₅], BDP, was studied at 15 K and ambient pressure by single-crystal X-ray diffraction as well as at ambient temperature and high pressures up to 4.87(5) GPa by Raman spectroscopy. BDP crystallizes in the orthorhombic Pnma space group with a=8.4069(4), b=11.7973(7), c=14.8496(7) Å, and Z=4; R₁=0.0381, wR₂=0.0764. The structure consists of distorted [SbCl₆]³⁻ octahedra forming zig-zag [{SbCl₅}_n]²ⁿ⁻ chains that are cross-linked by dimethylammonium [(CH₃)₂NH₂]⁺ cations. The organic and inorganic substructures are bound together by the N-H…Cl hydrogen bonds. The distortions of [SbCl₆]³⁻ units increase, partly due to the influence of the hydrogen bonds which became stronger, with decreasing temperature. The preliminary room temperature, high-pressure X-ray diffraction experiments suggest that BDP undergoes a first-order phase transition below ca. 0.44(5) GPa that destroys single-crystal samples. The transition is accompanied by changes in the intensities and positions of the Raman lines below 400 cm⁻¹.     

Crystal structure, phase transitions and ferroelastic properties of [(CH3)2NH2]3[Bi2Cl9]

A sequence of structural phase transitions in [(CH₃)₂NH₂]₃[Bi₂Cl₉] (DMACB) is established on the basis of differential scanning calorimetry (DSC) and dilatometric studies. Four phase transitions are found: at 367/369, 340/341, 323/325 and 285/292 K (on cooling/heating). The crystal structure of DMACB is determined at 350 K. It crystallizes in monoclinic space group P2₁/n: a=8.062(2), b=21.810(4), c=14.072(3) Å, β=92.63(3)°, Z=4, R₁=0.0575, wR₂=0.1486. The crystal is built of the double chain anions (“pleated ribbon structure”) and the dimethylammonium cations. Dielectric studies in the frequency range 75 kHz-900 MHz indicate relatively fast reorientation of the dimethylammonium cations over the I, II, III and IV phases. Infrared spectra are recorded in the temperature range 40-300 K and analyzed in region assigned to the symmetric and asymmetric NC₂ stretching vibrations. Optical observations show the existence of the ferroelastic domain structure over all phases below 367 K. The possible mechanisms of phase transitions are discussed on the basis of presented results.     

Synthesis and structure of a new uranyl selenate complex with 1-butylamine [CH3(CH2)3NH3](H5O2)[(UO2)2(SeO4)3(H2O)]

Crystals of a new uranyl selenate complex [CH₃(CH₂)₃NH₃](H₅O₂)[(UO₂)₂(SeO₄)₃(H₂O)] were obtained by isothermal evaporation at room temperature of its aqueous solution. The crystal structure was determined by the X-ray diffraction analysis. The observed character of the arrangement of organic molecules in the interlayer space confirms the concept of hydrophilic and hydrophobic zones.