F+NCO反应的机理和动力学

利用Ｇ２（ＭＰ２）理论研究Ｆ（＾２Ｐ）与ＮＣＯ（Ｘ＾２ＩＩ）在三重激发态（ａ＾３Ａ＂）势能面上的反应机理揭示了生成ＮＦ）Ｘ＾３Σ＾－）的两种反应途径,即顺式和反式加成－消除,其中顺式反应途径的势垒较低（２０．０ｋｊ．ｍｏｌ＾－１）,。动力学计算显示,在室温 上,Ｆ与ＮＣＯ反应于三重态势能面上只能较缓慢地生成ＮＦ（Ｘ＾３Σ＾－）自由基。预测ＦＣ（Ｎ）Ｏ是另一可能的反应产物     

[Nd（ONO2）6][Cu（Im）（Phen）2]2（OH）.4H2O的合成,晶体结构…

用Ｎｄ（ＮＯ３）３．６Ｈ２Ｏ、Ｉｍ（Ｃ３Ｈ４Ｎ２）、Ｐｈｅｎ（Ｃ１２Ｈ８Ｎ２）和Ｃｕ（ＮＯ３）２．３Ｈ２Ｏ为原料，两步反应合成了标题化合物，该化合物晶体属Ｐ１空间群，晶胞参数ａ＝１．０１２６（２）ｎｍ，ｂ＝１．１７９２（２）ｎｍ，ｃ＝１．３９８５ｎｍ，ａ＝１１１．３２（３）°，β＝９３．１７（３）°，γ＝９０．３３（３）°，Ｚ＝１，Ｒ＝０．０４３，测定了化合物的ＵＶ－Ｖｉｓ－ＮＩＲ及ＩＲ光谱和变温     

RE[CH2（CH2）4CONC4H9]3（NO3）3（RE=La,Dy）的合成和晶体结构

采用Ｘ－射线四园衍射仪测定了Ｄｙ「Ｃｈ２（ＣＨ２）４ＣＯＮＣ４Ｈ９」３（ＮＯ３）３和Ｌａ「ＣＨ２（ＣＨ２）４ＣＯＮＣ４Ｈ３」３（ＮＯ３）３的晶体结构。两个配合物具有相似的结构，均属单斜晶系，空间群为Ｐ２１／ｃ。晶体参数：Ｄｙ「Ｌａ」：ａ＝１．８５６４（３）「１．８５６４（２）」ｎｍ，ｂ＝０．９７６９（２）「０．９８３４（１）」ｎｍ，ｃ＝２．１８６３（６）「２．２００３８（７）」ｎｍ，β＝９６．０８     

（Cu（C14H11O3）（C10H8N2）2NO3.C2H5OH的合成,晶体结构和红外光谱

合成了（Ｃｕ（Ｃ１４Ｈ１１ｏ３）（Ｃ１０Ｈ８Ｎ２）ＮＯ３．Ｃ２Ｈ５ＯＨ化合物并测定其晶体结构，晶体属Ｐ空间群，ａ＝１．１９１１（２）ｎｍ，ｂ＝１．５３２２（２）ｎｍ，ｃ＝１．０４９２（２）ｎｍ，ａ＝１０８．９８（１）°β＝１０７．０４（１）°，γ＝７０．２５（１）°Ｚ＝２．在（Ｃｕ（Ｃ１４Ｈ１１Ｏ３）（Ｃ１０Ｈ８Ｎ２）２）配合阳离子中，２个２．２’－联吡啶的４个氮原子和二苯羟乙酸的１个羟基氧原子位     

呋喃醛双缩二氨基硫脲腙的合成和结构测定

由ＣＳ＿２，Ｎ＿２Ｈ＿４和Ｃ＿４Ｈ＿３ＯＣＨＯ合成Ｃ＿（１１）Ｈ＿（１０）Ｎ＿４Ｏ＿２Ｓ·１／２ＤＭＦ，Ｍ＿ｒ＝２９８．７９，橙黄针状晶体，三斜晶系，空间群Ｐ１，ａ＝８．９１２（３），ｂ＝９．９８９（３），ｃ＝１６．１０７（４），ａ＝８３．６１８（６），β＝８７．１０５（５），γ＝８６．１１５（３）°，Ｖ＝１４２０．４，Ｚ＝４，Ｄ＿ｘ＝１．３９７ｇ／ｃｍ￣３，λ（ＭｏＫα）＝０．７１０７３，μ＝２．１７０ｃｍ￣（－１），Ｆ（０００）＝６１６。３２２６个可观察的独立反射（Ｉ＞３σ（Ｉ）使结构顺利解出，并精修到Ｒ＝０．０４８，△ρ＿（ｍａｘ）＝０．２８６。单晶体结构分析表明不对称单位含有二个非结晶学对称相关的独立分子和一个溶剂分子ＤＭＦ，通过ＤＭＦ中的ｏ原子和亚胺Ｈ形成Ｎ－Ｈ…Ｏ…Ｈ－Ｎ类型双氢键，使两个分立分子缔合一起而自成独立的结构单元。     

Ln(NO_3)_3·C_(26)H_(38)N_2O_4(Ln=La、Ce)配合物的合成和La(NO_3)_3·C_(26)H_(38)N_2O_4·CH_3CN的晶体结构

合成了２个新的希土冠醚配合物Ｌｎ（ＮＯ３）３·Ｃ２６Ｈ３８Ｎ２Ｏ４（Ｌｎ＝Ｌａ、Ｃｅ；Ｃ２６Ｈ３８Ｎ２Ｏ４＝１，７，１０，１６－四氧－４，１３－二氮杂－Ｎ，Ｎ′－二苄基环十八烷）。通过元素分析，红外光谱，拉曼光谱及其１Ｈ核磁共振谱进行表征。用四圆衍射仪测定了Ｌａ（ＮＯ３）３·Ｃ２６Ｈ３８Ｎ２Ｏ４·ＣＨ３ＣＮ的晶体结构。晶体属三斜晶系，Ｐ１空间群，晶胞参数：ａ＝１．２８６９（４）ｎｍ，ｂ＝１．５８６８（６）ｎｍ，ｃ＝０．９１４７（２）ｎｍ；α＝１０１．８９（２）°，β＝１０５．３８（２）°，γ＝７１．９６（３）°；Ｚ＝２。ｄｃａｌｄ．＝１．５８ｇ·ｃｍ－３，μ（ＭｏＫα）＝１３．２５ｃｍ－１。中心镧离子与冠醚配体中的４个氧原子和２个氮原子配位，３个硝酸根中的６个氧原子也与Ｌａ３＋配位，形成配位数为１２的配合物。     

含硫杂核原子簇CpWFeCo(CO)_8(μ_3-S)和(CpW)_2Fe(CO)_7(μ_3-S)的合成及结构研究

本文利用过渡金属的亲硫性，通过Ｃｐ＊－Ｗ（ＣＯ）３Ｃｌ（Ｃｐ＊＝Ｃ５Ｈ５，Ｃ５Ｈ４ＣＨ３）与ＨＦｅ２Ｃｏ（ＣＯ）９（μ３－Ｓ）反应，得到四种含硫异核金属羰基原子簇化合物Ｃｐ＊ＷＦｅＣｏ（ＣＯ）８（μ３－Ｓ）（Ｃｐ＊＝Ｃ５Ｈ５，Ⅰ－ａ；Ｃｐ＊＝Ｃ５Ｈ４ＣＨ３，Ⅱ－ａ），（Ｃｐ＊Ｗ）２Ｆｅ（ＣＯ）７（μ３－Ｓ）（Ｃｐ＊＝Ｃ５Ｈ５，Ⅰ－ｂ；Ｃｐ＊＝Ｃ５Ｈ４ＣＨ３，Ⅱ－ｂ）。对合成的簇合物进行了ＩＲ，１Ｈ／１３Ｃ－ＮＭＲ，Ｃ／Ｈ及金属分析，并对Ⅰ－ａ进行了Ｘ－射线单晶结构分析。     

一系列烷基对二烷氧基苯在不同硝化体系中反应的研究

２－烷基－１，４－二甲氧基苯１ａ－ｄ（烷基为ＣＨ３，ＣＨ３ＣＨ２，ＰｈＣＨ２，（ＣＨ３）３Ｃ）分别在ＨＮＯ３－ＨＯＡｃ和ＮＨ４ＮＯ３－ＨＯＡｃ中反应后生成占绝对优势的硝化产物２－烷基－５－硝基－１，４－二甲氧基苯４ａ－ｄ，而２－烷基－５－叔丁基－１，４－二甲氧基苯２ａ－ｄ及２，５－二叔丁基－１，４－二苄氧基苯３在上述二种硝化体系中的反应在很大程度上取决于所用的硝化体系的性质及反应物的结构。对上述反     

溶胶—凝胶合成（Mg,Ca）O—SiO2：Eu^3＋,Bi^3＋发光体及其发光行为

以Ｍｇ（ＮＯ３）２，Ｃａ（ＮＯ３）２，Ｅｕ（ＮＯ３）３，Ｂｉ（ＮＯ３）３和Ｓｉ（ＯＣ２Ｈ５）４为反应物，采用溶胶－凝胶法，在比较低的温度，首次合成０．７０１ｍｏｌＭｇＯ－０．１７５ｍｏｌＣａＯ－１．２５ｍｏｌＳｉＯ２：０．０６ｍｏｌＥｕ＾３＋，０．００２ｍｏｌＢｉ＾３＋（加入Ｌｉ＾＋作为电荷补偿剂）发光体，得到了最佳合成条件，研究了由溶胶向凝胶转变和凝胶向发光晶体的转变过程，探讨了发光体在不同激光     

金属键有机化合物的研究──非对称型η~5－取代环戊二烯基三羰基钼（钨）金属单键化合物的合成及表征

通过η５－Ｒ~１Ｃ＿５Ｈ＿４（ＣＯ）＿３ＭＮａ与η~５－Ｒ~２Ｃ＿５Ｈ＿４（ＣＯ）＿３ＭＮａ（Ｍ＝Ｍｏ，Ｗ）以及η~５－Ｒ~１Ｃ＿５Ｈ＿４（ＣＯ）＿３ＭｏＮａ与η~５－Ｒ~２Ｃ＿５Ｈ＿４（ＣＯ）＿３ＷＮａ在Ｆｅ＿２（ＳＯ＿４）＿３醋酸水溶液作用下的交叉氧化偶联反应，合成了７个新的非对称型金属单键化合物η~５－Ｒ~１Ｃ＿５Ｈ＿４（ＣＯ）－３Ｍｏ─Ｍｏ（ＣＯ）＿３Ｃ＿５Ｈ＿４Ｒ~２－η~５（Ｒ~１，Ｒ~２：Ｃ（Ｏ）Ｍｅ，ＣＯ２Ｅｔ），η５－Ｒ１Ｃ５Ｎ４（ＣＯ）３Ｗ─Ｗ（ＣＯ）３Ｃ５Ｈ４Ｒ２－η５（Ｒ１，Ｒ２：Ｃ（Ｏ）Ｍｅ，ＣＯ２Ｅｔ；Ｈ，ＣＯ２Ｅｔ）和η５－Ｒ１Ｃ５Ｈ４（ＣＯ）３Ｍｏ─Ｗ（ＣＯ）３Ｃ５Ｈ４Ｒ２－η５（Ｒ１，Ｒ２：Ｃ（Ｏ）Ｍｅ，Ｈ；Ｅｔ，Ｃ（Ｏ）Ｍｅ；Ｃ（Ｏ）Ｍｅ，ｎ－Ｂｕ；ＣＯ２Ｍｅ，ｎ－Ｂｕ）．用Ｃ／Ｎ分析、ＩＲ、１ＨＮＭＲ和ＭＳ表征了它们的结构，并对该氧化偶联反应的特点进行了讨论．     

DFT法研究3-羟基丙烯醛的双键旋转异构反应机理

利用密度泛函理论(DFT)分别在B3LYP/6-31G**和B3LYP/6-311＋＋G**的计算水平上优化了基态3-羟基丙烯醛分子在双键旋转异构反应过程中的平衡态以及过渡态的几何构型，分析了反应过程中键参数的变化，计算了该反应的内禀反应坐标(IRC)，发现在重排反应途径上存在一个四元环骨架的中间体.通过振动分析对平衡态和过渡态进行了确认，并得到了零点能.计算结果表明，基态3-羟基丙烯醛分子的双键旋转异构反应经过两步完成，第一步反应位垒稍高，第二步反应位垒较低，存在着发生重排反应的可能性.     

亚甲基自由基(3CH2)与So反应机理的理论研究

白洪涛,黄旭日,于广涛,李吉来,于健康,孙家钟. 亚甲基自由基(3CH2)与SO反应机理的理论研究[J]. 化学学报, 2006, 64(2): 139-144.     

Thermochemistry of methyl and ethyl nitro, RNO2, and nitrite, RONO, organic compounds

Computational quantum theory is employed to determine the thermochemical properties of n-alkyl nitro and nitrite compounds: methyl and ethyl nitrites, CH3ONO and C2H5ONO, plus nitromethane and nitroethane, CH3NO2 and C2H5NO2, at 298.15 K using multilevel G3, CBS-QB3, and CBS-APNO composite methods employing both atomization and isodesmic reaction analysis. Structures and enthalpies of the corresponding aci-tautomers are also determined. The enthalpies of formation for the most stable conformers of methyl and ethyl nitrites at 298 K are determined to be -15.64 +/- 0.10 kcal mol-1 (-65.44 +/- 0.42 kJ mol-1) and -23.58 +/- 0.12 kcal mol-1 (-98.32 +/- 0.58 kJ mol-1), respectively. DeltafHo(298 K) of nitroalkanes are correspondingly evaluated at -17.67 +/- 0.27 kcal mol-1 (-74.1 +/- 1.12 kJ mol-1) and -25.06 +/- 0.07 kcal mol-1 (-121.2 +/- 0.29 kJ mol-1) for CH3NO2 and C2H5NO2. Enthalpies of formation for the aci-tautomers are calculated as -3.45 +/- 0.44 kcal mol-1 (-14.43 +/- 0.11 kJ mol-1) for aci-nitromethane and -14.25 +/- 0.44 kcal mol-1 (-59.95 +/- 1.84 kJ mol-1) for the aci-nitroethane isomers, respectively. Data are evaluated against experimental and computational values in the literature with recommendations. A set of thermal correction parameters to atomic (H, C, N, O) enthalpies at 0 K is developed, to enable a direct calculation of species enthalpy of formation at 298.15 K, using atomization reaction and computation outputs.     

双自由基CF2与O3的反应机理

主要用作致冷剂和发泡剂的氯氟烃（CFCs）是破坏臭氧层的主要物质之一．对氯氟烃类化合物及其降解产物（包括光解、光氧化、化学反应产物等）在大气中行为问题的研究是大气化学研究的重要内容．前人[1-3]从理论和实验两方面研究了自由基与臭氧的反应机制，但是氯氟烃光解过程中     

Entropy effects in the fragmentation of 1,1-dimethylhydrazine ions

The 1,1-dimethylhydrazine ion ((CH3)2NNH2+*) has two low-energy dissociation channels, the loss of a hydrogen atom to form the fragment ion m/z 59, (CH3)(CH2)NNH2+, and the loss of a methyl radical to form the fragment ion m/z 45, the methylhydrazyl cation, CH3NNH2+. The dissociation of the 1,1-dimethylhydrazine ion has been investigated using threshold photoelectron-photoion coincidence (TPEPICO) spectroscopy, in the photon energy range 8.25-31 eV, and tandem mass spectrometry. Theoretical breakdown curves have been obtained from a variational transition state theory (VTST) modeling of the two reaction channels and compared to those obtained from experiment. Seven transition states have been found at the B3-LYP/6-31+G(d) level of theory for the methyl radical loss channel in the internal energy range of 2.32-3.56 eV. The methyl loss channel transition states are found at R(N-C) = 4.265, 4.065, 3.965, 3.165, 2.765, 2.665, and 2.565 A over this internal energy range. Three transition states have been found for the hydrogen atom loss channel: R(H-C) = 2.298, 2.198, and 2.098 A. The DeltaS++(45) value, at an internal energy of 2.32 eV and a bond distance of R(N-C) = 4.265 A, is 65 J K-1 mol-1. As the internal energy increases to 3.56 eV the variational transition state moves to lower R value so that at R(N-C) = 2.565 A, the DeltaS++ decreases to 29 J K-1 mol-1. For the hydrogen atom loss channel the variation in DeltaS++ is less than that for the methyl loss channel. To obtain agreement with the experimental breakdown curves, DeltaS++(59) = 26-16 J K-1 mol-1 over the studied internal energy range. The 0 K enthalpies of formation (DeltafH0) for the two fragment ions m/z 45 and m/z 59 have been calculated from the 0 K activation energies (E0) obtained from the fitting procedure: DeltafH0[CH3NNH2+] = 906 +/- 6 kJ mol-1 and DeltafH0[(CH3)(CH2)NNH2+] = 822 +/- 7 kJ mol-1. The calculated G3 values are DeltafH0[CH3NNH2+] = 911 kJ mol-1 and DeltafH0[(CH3)(CH2)NNH2+] = 825 kJ mol-1. In addition to the two low-energy dissociation products, 21 other fragment ions have been observed in the dissociation of the 1,1-dimethylhydrazine ion as the photon energy was increased. Their appearance energies are reported.     

(CH3)2S与HOCl分子间的卤键和氢键相互作用

在DFT-B3LYP/6-311++G**水平上分别求得(CH3)2S…ClOH卤键复合物和(CH3)2S…HOCl氢键复合物势能面上的稳定构型. 频率分析表明, 与单体HOCl相比, 在两种复合物中, 10Cl—11O和12H—11O键伸缩振动频率发生显著的红移. 经MP2/6-311++G**水平计算的含基组重叠误差(BSSE)校正的气相中相互作用能分别为-11.69和-24.16 kJ·mol-1. 自然键轨道理论(NBO)分析表明, 在(CH3)2S…ClOH卤键复合物中, 引起10Cl—11O键变长的因素包括两种电荷转移: (i) 孤对电子LP(1S)1→σ*(10Cl—11O); (ii) 孤对电子LP(1S)2→σ*(10Cl—11O), 其中孤对电子LP(1S)2→σ*(10Cl—11O)转移占主要作用, 总的结果是使σ*(10Cl—11O)的自然布居数增加0.14035e, 同时11O原子的再杂化使其与10Cl成键时s成分增加, 即具有与电荷转移作用同样的“拉长效应”; 在(CH3)2S…HOCl氢键复合物中也存在类似的电荷转移, 但是11O原子的再杂化不同于前者. 自然键共振理论(NRT)进行键序分析表明, 在卤键复合物和氢键复合物中, 10Cl—11O和12H—11O键的键序都减小. 通过分子中原子理论(AIM)分析了复合物中卤键和氢键的电子密度拓扑性质.     

Computational study of the reactions of SiH3X (X=H, Cl, Br, I) with HCN

Ab initio calculations were carried out for the reactions of silane and halosilanes (SiH3X, X=H, Cl, Br, I) with HCN. Geometries of the reactants, transition states, intermediates and products were optimized at HF, MP2, and B3LYP levels of theory using the 6-31G(d) and 6-31G(d,p) basis sets. Energies were also obtained using G3MP2 and G3B3 levels of theory. Intrinsic reaction coordinate (IRC) calculations were performed to characterize the transition states on the potential energy surface. It was found that HCN can react with silane and halosilanes via three different mechanisms. One involves HX elimination by a one-step pathway producing SiH3CN. The second mechanism consists of H2 elimination, producing SiH2XCN via a one-step pathway or three multiple-step pathways. The third mechanism involves dissociation of SiH3X to various products, which can then react with HCN. Activation energies, enthalpies, and free energies of activation along with the thermodynamic properties (DeltaE, DeltaH, and DeltaG) of each reaction pathway were calculated. The reaction of SiH3X with HCN produce different products depending on substituent X. We have found that the standard 6-31G(d) bromine basis set gave results which were in better agreement with the G3MP2 results than for the Binning-Curtiss basis set. Computed heats of formation (DeltaHf) for SiH3CN, SiH3NC, SiH2ClCN, SiH2BrCN, SiH2ICN, SiHCl, SiHBr, and SiHI were found to be 133.5, 150.8, -34.4, 23.6, 102.4, 48.7, 127.1, and 179.8 kJ mol-1, respectively. From enthalpies calculated at G3MP2, we predict that the DeltaHf for SiH2 to be 262.8 kJ mol-1 compared to the experimental value of 273.8+/-4.2 kJ mol-1.     

Theoretical Study of Decomposition Mechanism of Azoisobutyronitrile

The decomposition mechanisms of azoisobutyronitrile were systematically investigated. Density function theory B3LYP/6-311G*, B3LYP/6-311+G* and BHandH/6-31+G** methods were employed to optimize the geometry parameters of the reactants, transition states, possible intermediates and products based on the detailed potential energy surfaces scanned with AM1. The reaction mechanisms were also analyzed theoretically. The results indicate that the decomposition of azoisobutyronitrile is a two-bond (three body) synchronouscleavage process in the ground state (CH3)2CNC-N=N-CCN(CH3)2→2(CH3)2CNC·+N2; and is a twobond asynchronous cleavage process while in the triple state (CH3)2CNCN=N-CCN(CH3)2→(CH3)2CNCN=N· · ·CCN(CH3)2→2(CH3)2CNC·+N2. The calculations rationalize and verify all experimental facts.     

Dynamics of the gas-phase reactions of chloride ion with fluoromethane: high excess translational activation energy for an endothermic S(N)2 reaction.

Guided ion beam tandem mass spectrometry techniques are used to examine the competing product channels in the reaction of Cl(-) with CH(3)F in the center-of-mass collision energy range 0.05-27 eV. Four anionic reaction products are detected: F(-), CH(2)Cl(-), FCl(-), and CHCl(-). The endothermic S(N)2 reaction Cl(-) + CH(3)F --> CH(3)Cl + F(-) has an energy threshold of E(0) = 181 +/- 14 kJ/mol, exhibiting a 52 +/- 16 kJ/mol effective barrier in excess of the reaction endothermicity. The potential energy of the S(N)2 transition state is well below the energy of the products. Dynamical impedances to the activation of the S(N)2 reaction are discussed, including angular momentum constraints, orientational effects, and the inefficiency of translational energy in promoting the reaction. The fluorine abstraction reaction to form CH(3) + FCl(-) exhibits a 146 +/- 33 kJ/mol effective barrier above the reaction endothermicity. Direct proton transfer to form HCl is highly inefficient, but HF elimination is observed above 268 +/- 95 kJ/mol. Potential energy surfaces for the reactions are calculated using the CCSD(T)/aug-cc-pVDZ and HF/6-31+G(d) methods and used to interpret the dynamics.     

·OH自由基与CH3CN反应机理及动力学

在CBS-QB3水平上研究了CH3CN 和·OH反应的势能面, 其中包括两个中间体和9个反应过渡态. 分别给出了各主要物质的稳定构型、相对能量及各反应路径的能垒. 根据计算的CBS-QB3势能面, 探讨了CH3CN+·OH反应机理. 计算结果表明, 生成产物P1(·CH2CN+H2O)的反应路径在整个反应体系中占主要地位. 运用过渡态理论对产物通道P1(·CH2CN+H2O)的速率常数k1(cm3·molecule-1·s-1)进行了计算. 预测了k1(cm3·molecule-1·s-1)在250-3000 K温度范围内的速率常数表达式为k1(250-3000 K)=2.06×10^-20T^3.045exp(-780.00/T). 通过与已有的实验值进行对比得出, 在实验所测定的250-320 K 范围内, 计算得到的k1的数值与已有的实验值比较吻合. 由初始反应物生成产物P1 (·CH2CN+H2O)只需要克服一个14.2 kJ·mol-1的能垒. 而产物·CH2CN+H2O生成后要重新回到初始反应物CH3CN+·OH, 则需要克服一个高达111.2 kJ·mol-1的能垒,这就表明一旦产物P1生成后就很难再回到初始反应物.