N-取代乙基吡唑热消除反应的量子化学研究

用MINDO/3方法研究了N-取代乙基吡唑热消除反应H₃C₃N₂CH₂CH₂X→H₄C₃N₂+H₂C=CHX(反应Ⅰ～Ⅲ,对应X=H,CH₃,F)的机理,结果表明,甲基的超共轭效应以及F的强吸电子作用和邻基参与使得反应Ⅱ和反应Ⅲ的活化势垒降低,比反应Ⅰ更易进行。     

气相离子-分子反应B2H3-+CS2——B2H3S-+CS的理论研究

用密度泛函方法B3LYP/6-311++G(d,p)和高级电子相关的偶合簇法CCSD(T)/6-311++G(d,p)研究了气相离子-分子反应B₂H₃^-+CS₂B₂H₃S^-+CS的机理.结果表明,B₂H₃最可能进攻CS₂中碳原子形成三元环中间体,随后通过氢迁移和最终消除CS的反应步骤形成硫原子转移产物H₃BBS^-+CS,反应大量放热且不需要活化能.B₂H₃直接对CS₂中硫原子进攻夺取硫原子的反应方式存在一定能垒阻碍.计算结果有助于深入了解B₂H₃,B₃H-6和B₄H₇^-等缺电子硼氢负离子的反应行为.     

甲亚胺系列气态分子结构及反应性质的ab initio研究

本文采用SCFMOabinitio法,用能量梯度优化(STO-3G和3-21G)给出了甲亚胺系列气态分子及有关离子的几何构型,研究了该系列分子的气相酸度及有H₂C=N^-参与的系列反应的△E,计算结果与实验值符合较好。     

过渡金属甲基磺酸盐催化醇的四氢吡喃化反应

以过渡金属甲基磺酸盐［Mn(CH₃SO₃)₂·2H₂O, Cu(CH₃SO₃)₂·4H₂O, Co(CH₃SO₃)₂·4H₂O和Zn(CH₃SO₃)₂·4H₂O］为催化剂,在室温条件下催化醇的四氢吡喃化反应,并对反应条件进行了优化。结果表明：当醇用量为30 mmol,醇和3,4-二氢吡喃摩尔比为1.0 ：1.1,甲基磺酸盐用量为1 mmol,二氯甲烷20 mL时,可高效催化醇的四氢吡喃化反应。与路易斯酸催化活性相比,过渡金属甲基磺酸盐催化醇的四氢吡喃化反应效果最好,催化酚的效果较差。用Mn(CH₃SO₃)₂·2H₂O和Cu(CH₃SO₃)₂·4H₂O催化正丁醇的四氢吡喃化反应,重复使用5次,收率分别为89%和92%。     

硼化合物的桥原子价及其反应活性的理论研究

根据原子价的量子化学定义,采用3-21G基组的ab initio方法,对B₂H₆及其桥原子取代物H₄B₂X₂(X=F,Cl,OH,NH₂,CH₃)进行几何构型优化,讨论桥原子的成键特征,并计算了B₄H₁₀、B₅H₉和B₅H₁₁等硼氢化合物的原子价,讨论了它们的亲电和亲核取代反应活性。     

Cl_2 2HI=2HCl I_2反应机理的理论研究

分别在MP2/3-21G!!、CCSD(T)/3-21G!!//MP2/3-21G!!和B3LYP/3-21G!!3种水平上,计算研究了气相反应Cl2 2HI=2HCl I2的机理,求得一系列四中心和三中心的过渡态.通过比较六种反应通道的活化能大小,得到了相同的结论:双分子基元反应Cl2 HI"HCl ICl和ICl HI"I2 HCl的最小活化能小于Cl2、HI和ICl的解离能,从理论上证明了反应Cl2 2HI=2HCl I2将优先以分子与分子作用形式分两步完成.用内禀反应坐标(IRC)验证了MP2/3-21G!!方法计算得到的过渡态.     

多反应离子的质子转移反应质谱

在无放射性辉光放电离子源内, 采用不同试剂气体进行放电, 为质子转移反应质谱(PTR-MS)新增了强度在10⁵ cps量级的3种反应离子NH₄⁺, NO⁺和O₂⁺, 纯度大于95%; 测试了这3种反应离子的离子-分子反应特征. 采用H₃O⁺, NH₄⁺, NO⁺和O₂⁺等4种反应离子对同分异构体丙醛/丙酮进行检测发现, H₃O⁺和NH₄⁺均不能区分的丙醛/丙酮可采用NO⁺或O₂⁺进行区分. 结果表明, 增加反应离子不仅使PTR-MS的可检测有机物范围不再局限于质子亲和势(PA)大于H₂O的有机物, 还提高了PTR-MS区分同分异构体的能力.     

邻苯二酚衍生物与稀土元素配位反应的研究(Ⅴ)——3,4-二羟基苯甲酸与铈(Ⅲ)的配位与转型反应

研究了稀土元素铈(Ⅲ)离子与3,4-二羟基苯甲酸(H₃L)在水溶液体系中生成羧基配位化合物的条件,表征其组成为Ce(H₂L)₂(OH)·3H₂O,并研究了该配合物在一定条件下,铈离子由羧基配位反应变为由两个邻酚羟基配位的配合物[Ce(HL)_n]的转型反应及氧化成铈(Ⅳ)配合物的反应。     

抗坏血酸提高稀土复合材料催化降解染料性能研究

本文以β-环糊精(CD)为载体,通过负载Fe₃O₄和稀土铈(Ce),制备了稀土复合材料Ce-Fe-CD,形成了可有效降解有机物的非均相芬顿反应Ce-Fe-CD/H₂O₂体系。为提高催化降解效果,本文用两种方式引入还原剂抗坏血酸(AA):(1)在非均相芬顿反应过程中直接投加AA,形成AA/Ce-Fe-CD/H₂O₂体系;(2)利用AA活化稀土复合材料,获得AA-Ce-Fe-CD复合材料,形成AA-Ce-Fe-CD/H₂O₂体系。实验结果表明,AA-Ce-Fe-CD/H₂O₂和AA/Ce-Fe-CD/H₂O₂对染料的降解率分别为86.9%和83.0%,比未使用AA时分别提高了34.4%和30.5%,且AA-Ce-Fe-CD/H₂O₂体系有更高的H₂O₂     

2-甲基-1,4-萘醌的绿色合成方法

以2-甲基萘(2-MN)为原料、H₂O₂为氧化剂,经不同酸(硫酸、氢溴酸、三氟乙酸等)催化合成2-甲基-1,4-萘醌(2-MNQ),其结构经¹H NMR和¹³C NMR确证,其纯度经HPLC检测。对反应条件进行了优化。最佳反应条件为：20 eq. CH₃COOH为溶剂,6 eq. H₂O₂为氧化剂,在10%mol H₂SO₄催化下,于75 ℃反应,2-MNQ纯度95%,收率67%。     

Ab Initio Study of Ring Flipping of the Overcrowded Peri-Substituted Naphthalenes

Ab inintio molecular orbital and density functional theory method were used to investigate the structural and dynamic behavior of 1,8-di-tert-butyl naphthalene (1), 1,8-bis(trimethylsilyl)naphthalene (2), 1,8-bis(trimethylgermyl)naphthalene (3), and 1,8-bis(trimethylstannyl)naphthalene (4). HF/3-21G//HF/3-21G results revealed that the ring flipping barrier height of compound 1–4 is 92.59, 32.13, 26.76, and 15.46 kJ mol^?1 respectively. The obtained results show that the transition state structure for ring flipping of the bulky-groups is in a planar form with naphthalene ring. Contrary to compound 1, the ring flipping of compounds 2–4 occurred easily at room temperature. Also, MP2/3-21G//HF/3-21G energy calculation, show that the enantiomerization energy of compounds 1–4 are 97.99, 33.24, 26.80, and 15.38 kJ·mol^?1 respectively. The required energy for ring inversion of compounds 1–4 are 85.09, 27.26, 21.54, and 10.21 kJ mol^?1 respectively, as calculated by B3LYP/3-21G//HF/3-21G method. It can be concluded that the lower energy barrier of the ring flipping of compounds 2–4 is related to the increasing of the bond lengths of Si—C, Ge—C, and Sn—C, in contrast to C—C bond.     

Structural changes, P-P bond energies, and homolytic dissociation enthalpies of substituted diphosphines from quantum mechanical calculations

The molecular structures of the diphosphines P(2)[CH(SiH(3))(2)](4), P(2)[C(SiH(3))(3)](4), P(2)[SiH(CH(3))(2)](4), and P(2)[Si(CH(3))(3)](4) and the corresponding radicals P[CH(SiH(3))(2)](2), P[C(SiH(3))(3)](2), P[SiH(CH(3))(2)](2), and P[Si(CH(3))(3)](2) were predicted by theoretical quantum chemical calculations at the HF/3-21G*, B3LYP/3-21G*, and MP2/6-31+G* levels. The conformational analyses of all structures found the gauche conformers of the diphosphines with C(2) symmetry to be the most stable. The most stable conformers of the phosphido radicals were also found to possess C(2) symmetry. The structural changes upon dissociation allow the release of some of the energy stored in the substituents and therefore contribute to the decrease of the P-P bond dissociation energy. The P-P bond dissociation enthalpies at 298 K in the compounds studied were calculated to vary from -11.4 kJ mol(-1) (P(2)[C(SiH(3))(3)](4)) to 179.0 kJ mol(-1) (P(2)[SiH(CH(3))(2)](4)) at the B3LYP/3-21G* level. The MP2/6-31+G* calculations predict them to be in the range of 52.8-207.9 kJ mol(-1). All the values are corrected for basis set superposition error. The P-P bond energy defined by applying a mechanical analogy of the flexible substituents connected by a spring shows less variation, between 191.3 and 222.6 kJ mol(-1) at the B3LYP/3-21G level and between 225.6 and 290.4 kJ mol(-1) at the MP2/6-31+G* level. Its average value can be used to estimate bond dissociation energies from the energetics of structural relaxation.     

First principle computational study on the full conformational space of L-proline diamides

Ab initio molecular orbital computations were carried out at three levels of theory: RHF/3-21G, RHF/6-31G(d), and B3LYP/6-31G(d), on four model systems of the amino acid proline, HCO-Pro-NH2 [I], HCO-Pro-NH-Me [II], MeCO-Pro-NH2 [III], and MeCO-Pro-NH-Me [IV], representing a systematic variation in the protecting N- and C-terminal groups. Three previously located backbone conformations, gammaL, epsilonL, and alphaL, were characterized together with two ring-puckered forms syn (gauche+ = g+) or "DOWN" and anti (gauche- = g-) or "UP", as well as trans-trans, trans-cis, cis-trans, and cis-cis peptide bond isomers. The topologies of the conformational potential energy cross-sections (PECS) of the potential energy hypersurfaces (PEHS) for compounds [I]-[IV] were explored and analyzed in terms of potential energy curves (PEC), and HCO-Pro-NH2 [I] was also analyzed in terms of potential energy surfaces (PESs). Thermodynamic functions were also calculated for HCO-Pro-NH2 [I] at the CBS-4M and G3MP2 levels of theory. The study confirms that the use of the simplest model, compound [I] with P(N) = P(C) = H, along with the RHF/3-21G level of theory, is an acceptable practice for the analysis of peptide models because only minor differences in geometry and stability are observed.     

CC Triple-bond stabilization in three-membered ring compounds: Boriryne,dilithiumcyclopropyne and berylliryne

Ab initio calculations have been performed on the title compounds. At 3-21G, boriryne is not a minimum on the potential energy hypersurface. The 3-21G optimized minimum of dilithiumcyclopropyne corresponds to dilithiumcyclopropenylidene with a planar tetracoordinated carbon atom and CC bond lengths intermediate between single and double bonds. Berylliryne is calculated to be a stable molecule, being the global minimum at the C₂ Be energy hypersurface at MP2/6-31G*//6-31G* with a CC bond length of 1.258 Å.     

On the flexibility of beta-peptides

The full conformational space was explored for an achiral and two chiral beta-peptide models: namely For-beta-Ala-NH2, For-beta-Abu-NH2, and For-beta-Aib-NH2. Stability and conformational properties of all three model systems were computed at different levels of theory: RHF/3-21G, B3LYP/6-311++G(d,p)//RHF/3-21G, B3LYP/6-311++G(d,p), MP2//B3LYP/6-311++G(d,p), CCSD//B3LYP/6-311++G(d,p), and CCSD(T)//B3LYP/6-311++G(d,p). In addition, ab initio E = E(phi, micro, psi) potential energy hypersurfaces of all three models were determined, and their topologies were analyzed to determine the inherent flexibility properties of these beta-peptide models. Fewer points were found and assigned than expected on the basis of Multidimensional Conformational Analysis (MDCA). Furthermore, it has been demonstrated, that the four-dimensional surface, E = E(phi, mu, psi), can be reduced into a three-dimensional one: E = E[phi, f(phi), psi]. This reduction of dimensionality of freedom of motion suggests that beta-peptides are less flexible than one would have thought. This agrees with experimental data published on the conformational properties of peptides composed of beta-amino acid residues.     

Theoretical studies on the gas-phase pyrolysis of 2-phenoxycarboxylic acids: an ONIOM approach

Various ONIOM combinations-ONIOM(HF/6-31G*: PM3), ONIOM(B3LYP/6-31G*: PM3), ONIOM(MP2/6-31G*: PM3), and ONIOM(MP2/6-31G*: HF/3-21G)--were applied to investigate thermal decomposition mechanisms of four 2-phenoxycarboxylic acids (2-phenoxyacetic acid, 2-phenoxypropionic acid, 2-phenoxybutyric acid, and 2-phenoxyisobutyric acid) in the gas phase. All the transition states and intermediates of the reaction paths were optimized. The reaction pathway of four reactants yielding the phenol, CO, and the corresponding carbonyl compound was characterized on the potential energy surface and found to proceed stepwise. The first step corresponds to the elimination of phenol and the formation of alpha-lactone intermediate through a five-membered ring transition state, and the second step is the cycloreversion process of alpha-lactone intermediate to form CO and the corresponding carbonyl compound. The reaction pathway of latter three compounds to produce the carboxylic acid and phenol via a four-membered cyclic transition structure was also examined theoretically. Comparison with experiment indicates that the activation parameters for the fist reaction channel are accurately predicted at the ONIOM(MP2/6-31G*: HF/3-21G) level of theory.     

THEORETICAL STUDIES ON THE STRUCTURES AND REACTIVITY OF SILYLENOIDS (Ⅰ)——STRUCTURES AND ISOMERIZATION OF SILYLENOID H_2SiLiCl

The structures of silylenoid H_2SiLiCl have been studied by RHF/3-21G gradient method. Three equilibrium states and two isomerization transition states are located. The electronic energy, Mulliken populations, dipole moments and frontier molecular orbitals (FMO) of every structure and the isomeric barriers are also given and analyzed. Further single point calculations on the 3-21G optimum geometries were performed using 6-21G basis set. The calculations show that three-membered ring structure of H_2SiLiCl is the most stable and detectable, and the "classical" tetrahedral form is not the local minimum on the potential energy surface.     

Density functional theory calculations of selected Ru(II) two ring diimine complex dications

Geometry optimization for a series of ten, two-ring diimine Ru(II) complexes was effected using the Gaussian 98 protocol at density functional theory (DFT) B3LYP level with basis sets 3-21G*and 3-21G**. HOMO-LUMO energy difference values compared favorably to the experimental data from electrochemistry [Delta E(1/2) = (E(1/2ox) - E(1/2red))] and the lowest energy absorption maxima, which for these complexes correspond to the metal-to-ligand charge transfer (MLCT) band. The HOMO and LUMO distributions from DFT support the idea that the lowest energy transitions are metal-to-ligand charge transfer and that the lowest energy LUMO for the mixed ligand complexes is located on 2,2'-bipyrazine (bpz), followed by 2,2'-bipyrimidine (bpm) and then 2,2'-bipyridine (bpy).     

TATB与二氟甲烷以及与聚偏二氟乙烯的分子间相互作用

动用密度泛函理论(SFT)B3LYP方法,取3－21G*基组,求得TATB(1,3,5-三氨基-2,4,6-三硝基苯)与CH~2F~2混合体系的三种优化构型以Boys-Bernardi方案校正基组叠加误差求得结合能。在B3LYP/6----311G*//B3LYP/3---21G*水TATB与CH~2F~2间的最大结合能为4.62kJ·mol^-1,还用MO－PM3方法计算TATB与---（CF~2CH~2}－(N=1,2,3,4,5,)的混合体系,由色散校正电子相关近似地求得其结合能力。当n＝5时,求得TATB与－（CF~2CH~2）--~n的最大结合能约为52.97kJ·MOL^-1。此外,自然键轨道分析用于讨论TATB与CH~2F~2之间的电荷转移。