[Co(2,3-tri)(amp)Cl]^2^+几何经式异构体取代与重排规律、构效关系的研究

对[Co(2,3-tri)(amp)Cl]^2^+四个几何经式异构体在不同条件下的取代及重排反应进行了详细的考察。因二元胺中吡啶环造成的空间拥塞,使cis异构体碱水解速度比trans异构体约快100倍,控制碱水解实验结果表明,每一异构体的水解产物均含四个经式异构体,且具有相同分布。实验过程中未观察到面式异构体。在二甲亚砜中加热的重排反应中,异构体m1表现出最高的反应性,cis异构体均首先转化为trans异构体m3,而后可观察到trans异构体m3与m4的平衡。利用时间分辨核磁共振仪测定了氘代水里各异构体中各活性氢的氘代化速度。反应活性最低的异构体m4具有氘代速度最快的活性氢,当这些活性氢完全氘代化时仍未见其水解或重排产物;而相同实验条件下异构体m1或m2中相应活性氢的氘代化速度则要缓慢得多,但同时可观察到水解和重排产物。这说明在碱催化水解过程中氘代速度快的活性氢与异构体的反应性并非正比关系,然而活性氢的氘代化是观察到异构体水解重排的必要条件。利用量子化学从头计算法在赝势基组RHF/LANL2DZ的水平上对该体系各异构体进行了结构优化计算,与对应异构体的晶体结构参数比较,一般相对误差不超过3%,从能量角度来看,cis异构体比trans异构体高出约4kJ/mol,而面式异构体则至少比经式异构体高约17kJ/mol;考虑溶剂化影响,一般约低5kJ/mol。考察结构参数结果显示,结构变形性参数能较好地解释异构体反应活性。     

[Co(3,3-tri)(amp)CI]2+四个经式异构体取代、重排反应及其与结构关系的研究

对[Co(3,3-tri)(amp)Cl]2+四个几何经式异构体在不同条件下的取代及重排反应进行考察的实验结果表明,四个几何经式异构体碱性环境下的水解速率没有显著的差异,cis异构体比trans异构体约快20倍.实验中没有观察到面式异构体.     

[Co(3,3-tri)(amp)Cl]~(2+)四个经式异构体取代、重排反应及其与结构关系的研究

对犤Co(3,3-tri)(amp)Cl犦2+四个几何经式异构体在不同条件下的取代及重排反应进行考察的实验结果表明,四个几何经式异构体碱性环境下的水解速率没有显著的差异,cis异构体比trans异构体约快20倍。实验中没有观察到面式异构体。在100℃二甲亚砜中加热的重排反应实验中可观察到异构体进行配体翻转的历程,如异构体m1-Cl转化为m4-Cl,m2-Cl转化为m3-Cl。m3和m4相对较稳定。利用量子化学从头计算法,在赝势基组RHF/LANL2DZ的水平上对该体系各异构体进行了基态能量、几何优化的计算,与已测定的异构体m3犤ZnCl4犦H2O和m4犤ZnCl4犦晶体结构参数比较,键长及键角的相对误差不超过3%。根据各异构体基态能量说明了各异构体的平衡分布;讨论了键角变形性大小与各异构体反应性大小的关系。     

[Co(3,3-tri)(amp)Cl]2+四个经式异构体取代、重排反应及其与结构关系的研究

对[Co(3,3-tri)(amp)Cl]²⁺四个几何经式异构体在不同条件下的取代及重排反应进行考察的实验结果表明,四个几何经式异构体碱性环境下的水解速率没有显著的差异,cis异构体比trans异构体约快20倍。实验中没有观察到面式异构体。在100℃二甲亚砜中加热的重排反应实验中可观察到异构体进行配体翻转的历程,如异构体m1-Cl转化为m4-Cl,m2-Cl转化为m3-Cl。m3和m4相对较稳定。利用量子化学从头计算法,在赝势基组RHF/LANL2DZ的水     

1-萘酚的紫外共振双光子电离光谱

利用脉冲分子束技术, 在305-322 nm范围内研究了1-萘酚(1NP)的共振双光子电离(R2PI)光谱. 1NP分子存在cis和trans两种旋转异构体, 但实验中仅观测到trans异构体的电子振动跃迁光谱, 其S1←S0跃迁的(0-0)带头出现在317.90 nm(即31456 cm-1)位置. 利用光谱选律及ab initio和密度泛函(DFT)计算, 对trans异构体在S1态的振动模进行标识, 得出主要对应于对称性为a'的平面内振动模. 计算显示, cis异构体在电子基态S0的能量较trans异构体高出439 cm-1, 而第一激发能却比trans异构体的低1216 cm-1, 与之相应的实验值分别是220和274 cm-1. 计算数值与实验结果在能量变化趋势上完全一致. 共振双光子电离谱中没有观测到cis异构体的光谱信号, 其原因可归结为分子束的有效冷却效应使得处于基态的cis异构体的布居数密度相对trans异构体极低, 导致cis光谱信号太小而未能被探测到.     

NMR对MDI在稀溶液中水解反应机理的表征

采用核磁共振波谱(NMR)研究了二苯基甲烷二异氰酸酯(MDI)在稀溶液中的水解反应机理.将同一MDI样品分别溶解在氘代氯仿、氘代丙酮和加入少量水分的氘代二甲基亚砜溶剂(DMSO)中,进行核磁共振氢谱(1H NMR)、核磁共振碳谱(13C NMR)测试.结果显示,MDI在含水的DMSO溶剂中测得的谱图与氘代氯仿、氘代丙酮中的差别显著.对该溶液进行了13C-1H异核近程相关(HMQC)、13C-1H异核远程相关(HMBC)及碳原子级数(DEPT 135)测试,并利用经验公式对其进行了详细归属,确认了反应产物的结构.分析得知MDI在含水溶剂中迅速反应,异氰酸酯基转化为脲基和氨基基团.异氰酸酯与水反应生成氨基基团,其与异氰酸酯反应活性比水高,对位取代氨基与水的竞聚率比值为7.1,邻位为1.4,对位取代氨基活性约是邻位的5倍.     

光催化的Schiff碱与N-乙烯基吡咯烷酮及N-乙烯基咔唑的Diels-Alder反应研究:合成4-杂环取代的四氢喹啉衍生物

四氢喹啉及其衍生物是一类在自然界广泛存在并具有重要生物活性的化合物,不仅用作药物、杀虫剂、抗氧化剂、抗腐蚀剂,还用于染料、光学记录材料中.因此其合成多年一直倍受关注[1].在众多的合成方法中,Schiff碱与不饱和化合物的Diels-Alder反应是构筑六元氮杂环最重要的方法之一[1,2].2,4,6-三苯基吡喃四氟化硼(TPT)是一种在光诱导电子转移反应中常用的光敏剂[3],特别是在催化富电子烯烃的光环加成反应方面,显示出独特的性能.我们在最近的研究中发现TPT也可以作为一种有效的Schiff碱与富电子烯烃光诱导Diels-Alder反应的催化剂[3].在进一步研究中,我们发现TPT还可以催化Schiff碱与N-乙烯基吡咯烷酮及N-乙烯基咔唑的Diels-Alder反应并生成高产率(75%～95%)的4-(1-吡咯烷酮基)四氢喹啉(3)和4-(9-咔唑基)四氢喹啉(4).Schiff碱与N-乙烯基吡咯烷酮的反应只生成cis产物,具有很高的立体选择性和区域选择性;而Schiff碱与N-乙烯基咔唑的反应则生成cis和trans混合物.     

拓扑异构体的研究(Ⅰ)C型与S型拓扑异构体的波谱性质及结构鉴定

利用 ¹H和 ¹³C NMR, IR, UV, SEM对合成的4种C型和S型拓扑异构体进行了结构表征和分析, 发现对于不同拓扑结构的C型和S型分子可以通过 ¹H NMR来鉴别, 而对于相同拓扑结构的S型cis(SC)和trans(ST)分子, C型 cis(CC)和trans(CT)分子则要结合 ¹³C NMR来鉴别. 四种拓扑异构体的IR, UV, 波谱性质以及SEM图象没有显著的差异.     

三乙胺催化的双环氮杂锡氧烷配合物氘代反应研究

全面研究了三乙胺催化下双环氮杂锡氧烷配合物α 氢的氘代反应 .首先考察了三乙胺催化下双环氮杂锡氧烷配合物α 氢的氘代反应的核磁共振谱 ,研究发现 :在三乙胺存在下 ,有机锡配合物α 氢可以与CD3 OD溶剂发生氘代反应 ,其核磁共振峰强度随着时间而衰减 ,且氘代反应速率与三乙胺的浓度有关 .其次 ,利用核磁共振技术测定氘代反应速率 ,其反应表观速率常数为 2 .0× 1 0 -4 ～ 1 0 .0× 1 0 -4 s-1,推导了其动力学机理并讨论了取代基对氘代反应速率的影响 .     

示踪原子在有机化学中的应用(二)

V.水解反应 (一)Chloralquinaldine(XXI)的水解重排反应。(XXI)用醇碱溶液水解时,除了     

A reappraisal of the nature of the product from the reaction of bis(methylcyclopentadieny)tin(II) with tungsten(cyclopentadienyl) (tricarbonyl) hydride

The nature of the product obtained from the title reaction has been reexamined, and identified as ClSn[W(CO)₃C₅H₅)]₃.     

Modeling of the solid-state packing of charged chains (PEDOT) in the presence of the counterions (TSA) and the solvent (DEG)

Molecular mechanics and ab-initio calculations are performed in the framework of the interaction between the charged poly(ethylenedioxythiophene) (PEDOT), the p-toluensulphonic acid (TSA), and the diethylene glycol (DEG). Different possibilities of positioning the counterion along the conjugated polymer are studied. For each possibility (or orientation), the influence of relative position of the counterion on the stability of these charged interfaces is considered. The results indicate that the perpendicular orientation corresponds to the most stable structure of the PEDOT/TSA complex. The influence of the counterion on the charge distribution in the PEDOT is also investigated indicating that a strong influence of the interionic correlation on the stability of PEDOT by TSA. Further the packing of doped chains with their counterions is also determined. In the larger aggregates, the effect of the solvent is considered. These results give a new insight about the molecular arrangements of PEDOT/TSA interactions and allow to understand how charge transport along the stacks can take place.     

A reinterpretation of the magnetic properties of the mixed-valence (Nb(V)/Nb(IV)) Zintl phase, Cs(9)Nb(2)As(6)

A new mixed-valent (Nb(V)/Nb(IV)) Zintl phase, Cs(9)Nb(2)As(6), has been prepared and characterized, recently (Gascoin, F.; Sevov, S. C. Inorg. Chem. 2002, 41, 5920). Niobium is present in the form of isolated, edge-sharing tetrahedral, Nb(2)As(6)(9)(-) dimers. The reported magnetic susceptibility features a broad maximum at approximately 36 K which has been interpreted as the onset of long-range antiferromagnetic order. Such a high transition temperature is difficult to understand as the compound is insulating and the interdimer Nb-Nb distance is 7.2 A. It is shown here that the observed magnetic properties follow straightforwardly from a statistical occupation of the equivalent intradimer Nb sites by equal concentrations of Nb(IV)(4d(1), S = (1)/(2)) and Nb(V)(4d(0)). From this analysis the broad maximum arises from intradimer antiferromagnetic exchange with an exchange constant, J/k = -40 K, and there is no long-range magnetic order except, possibly, below 5 K.     

Complexes of the ethylpyridines with the halides of cobalt(II), nickel(II) and copper(II)

A series of complexes has been prepared with the halides of cobalt(II), nickel(II), copper(II) and 2-,3-,4-ethylpyridine. The compounds were essentially all octahedral with the exception of those formed between 2-ethylpyridine and the cobalt(II) halides. The stereochemical configurations were deduced using spectral and magnetic properties. The decomposition of the complexes was studied by thermogravimetry and differential thermal analysis.

---

Zusammenfassung Eine Reihe von Komplexen wurde aus den Halogeniden von Cobalt(II), Nickel(II), Kupfer(II) und 2-, 3-, 4-äthylpyridin hergestellt. Die Verbindungen waren im Wesentlichen alle oktaedrisch, mit Ausnahme jener, die aus 2-äthylpyridin und den Cobalt(II) halogeniden gebildet wurden. Die stereochemischen Konfigurationen wurden aus den spektralen und magnetischen Eigenschaften abgeleitet. Der Zerfall der Komplexe wurde durch Thermogravimetrie und Differentialthermoanalyse untersucht.

---

Résumé Une série de complexes a été préparée avec les halogénures de cobalt(II), nickel(II), cuivre(II) et éthyl-2-, 3-, 4- pyridine. La plupart des composés sont octaédriques, à l'exception de ceux formés à partir de l'éthyl-2 pyridine et les halogénures de cobalt(II). Les configurations stéréochimiques ont été déduites des propriétés spectrales et magnétiques. La dé composition des complexes a été suivie par thermogravimétrie et analyse thermique différentielle.

---

2-, 3-, 4- (II), (II) (II). , , , (II) 2-. , . .

---

---

The authors wish to thank Beckman Instruments Ltd for the use of the Far IR spectrophotometer, IR 720 M.     

Investigation of the radical product channel of the CH(3)C(O)CH(2)O(2) + HO(2) reaction in the gas phase

The reaction of CH(3)C(O)CH(2)O(2) with HO(2) has been studied at 296 K and 700 Torr using long path FTIR spectroscopy, during photolysis of Cl(2)/acetone/methanol/air mixtures. The branching ratio for the reaction channel forming CH(3)C(O)CH(2)O, OH and O(2) () was investigated in experiments in which OH radicals were scavenged by addition of benzene to the system, with subsequent formation of phenol used as the primary diagnostic for OH radical formation. The observed prompt formation of phenol under conditions when CH(3)C(O)CH(2)O(2) reacts mainly with HO(2) indicates that this reaction proceeds partially by channel , which forms OH both directly and indirectly, by virtue of secondary generation of CH(3)C(O)O(2) (from CH(3)C(O)CH(2)O) and its reaction with HO(2) (). The secondary generation of OH radicals was confirmed by the observed formation of CH(3)C(O)OOH, a well-established product of the CH(3)C(O)O(2) + HO(2) reaction (via channel ). A number of delayed sources of OH also contribute to the observed phenol formation, such that full characterisation of the system required simulations using a detailed chemical mechanism. The dependence of the phenol and CH(3)C(O)OOH yields on the initial peroxy radical precursor reagent concentration ratio, [methanol](0)/[acetone](0), were well described by the mechanism, consistent with a small but significant fraction of the reaction of CH(3)C(O)CH(2)O(2) with HO(2) proceeding via channel . This allowed a branching ratio of k(3b)/k(3) = 0.15 +/- 0.08 to be determined. The results therefore provide strong indirect evidence for the participation of the radical-forming channel of the title reaction.     

On the origin of the square root of (7) x square root of (7) superstructure and the anomalous magnetic and transport properties of the layered compound Sr(6)V(9)S(22)O(2)

We examined why the 1T-VS(2) layer of the layered compound Sr(6)V(9)S(22)O(2) has the x superstructure in terms of electronic band structure calculations and metal-metal bonding across the shared edges of adjacent VS(6) octahedra. On the basis of this analysis we explored how the anomalous magnetic and transport properties of Sr(6)V(9)S(22)O(2) can be explained. Our work shows that the x superstructure is not caused by a charge density wave instability associated with Fermi surface nesting but by the metal-metal bonding through the shared edges of adjacent VS(6) octahedra. The weak and strong electron localizations observed for Sr(6)V(9)S(22)O(2) were discussed in terms of three-center two-electron and two-center two-electron V-V bonds in the 1T-VS(2) layers.     

Theoretical study on the mechanism of the (3)CH(2) + NO(2) reaction

The complex doublet potential energy surface of the CH(2)NO(2) system is investigated at the B3LYP/6-31G(d,p) and QCISD(T)/6-311G(d,p) (single-point) levels to explore the possible reaction mechanism of the triplet CH(2) radical with NO(2). Forty minimum isomers and 92 transition states are located. For the most relevant reaction pathways, the high-level QCISD(T)/6-311 + G(2df,2p) calculations are performed at the B3LYP/6-31G(d,p) geometries to accurately determine the energetics. It is found that the top attack of the (3)CH(2) radical at the N-atom of NO(2) first forms the branched open-chain H(2)CNO(2) a with no barrier followed by ring closure to give the three-membered ring isomer cC(H(2))ON-O b that will almost barrierlessly dissociate to product P(1) H(2)CO + NO. The lesser followed competitive channel is the 1,3-H-shift of a to isomer HCN(O)OH c, which will take subsequent cis-trans conversion and dissociation to P(2) OH + HCNO. The direct O-extrusion of a to product P(3) (3)O + H(2)CNO is even much less feasible. Because the intermediates and transition states involved in the above three channels are all lower than the reactants in energy, the title reaction is expected to be rapid, as is consistent with the measured large rate constant at room temperature. Formation of the other very low-lying dissociation products such as NH(2) + CO(2), OH + HNCO and H(2)O + NCO seems unlikely due to kinetic hindrance. Moreover, the (3)CH(2) attack at the end-O of NO(2) is a barrier-consumed process, and thus may only be of significance at very high temperatures. The reaction of the singlet CH(2) with NO(2) is also briefly discussed. Our calculated results may assist in future laboratory identification of the products of the title reaction.     

Energy relationship and the polarization of C_(60) cage in the endohedral complexes (X@C_(60))

In this paper, we carry out the calculation on the system (X@C60)(X=Li, Na, K, Kb, Cs; F, Cl, Br, I), where the position of X changes along 5 typical symmetry directions. For the calculation of quantum chemistry we use EHMO/ASED method, for the calculation of molecular mechanics we use Buckingham potential (exp-6-1) function, and for the calculation of thermo-chemical cycle we use individually isolating the processes such as the structure variation, charge transfer and charge distribution, and their interactions etc. The calculation results show that (1) In the region of radius r≈0.2 nm of the Ceo cage, the potential field is nearly spherical; (2) Except for Li and Na, the systems are the most stable with minimum energies at the center of C60 cage. For Li and Na, the systems are the most stable with minimum energies at r≈0.16 nm and r≈0.13 nm, respectively. In view of the interactive region of chemical bonds, the interactions between X and the C60 cage do not belong to the classical chemical bonds; (     

Extending the coordination chemistry of molecular P(4)S(3): the polymeric Ag(P(4)S(3))(+) and Ag(P(4)S(3))(2)(+) cations

Upon reacting P(4)S(3) with AgAl(hfip)(4) and AgAl(pftb)(4) [hfip = OC(H)(CF(3))(2); pftb = OC(CF(3))(3)], the compounds Ag(P(4)S(3))Al(hfip)(4) 1 and Ag(P(4)S(3))(2)(+)[Al(pftb)(4)](-) 2 formed in CS(2) (1) or CS(2)/CH(2)Cl(2) (2) solution. Compounds 1 and 2 were characterized by single-crystal X-ray structure determinations, Raman and solution NMR spectroscopy, and elemental analyses. One-dimensional chains of [Ag(P(4)S(3))(x)](infinity) (x = 1, 1; x = 2, 2) formed in the solid state with P(4)S(3) ligands that bridge through a 1,3-P,S, a 2,4-P,S, or a 3,4-P,P eta(1) coordination to the silver ions. Compound 2 with the least basic anion contains the first homoleptic metal(P(4)S(3)) complex. Compounds 1 and 2 also include the long sought sulfur coordination of P(4)S(3). Raman spectra of 1 and 2 were assigned on the basis of DFT calculations of related species. The influence of the silver coordination on the geometry of the P(4)S(3) cage is discussed, additionally aided by DFT calculations. Consequences for the frequently observed degradation of the cage are suggested. An experimental silver ion affinity scale based on the solid-state structures of several weak Lewis acid base adducts of type (L)AgAl(hfip)(4) is given. The affinity of the ligand L to the silver ion increases according to P(4) < CH(2)Cl(2) < P(4)S(3) < S(8) < 1,2-C(2)H(4)Cl(2) < toluene.