甲基肼自由基在高温燃烧分解反应下的非谐振效应（英文）

基于过渡态理论(TST)和RRKM(Rice-Ramsperger-Kassel-Marcus)理论,使用MP2/6-311++G(3df,2p)//B3LYP/6-311++G(3df,2p)基组和方法,本文分别计算了甲基肼自由基在高温燃烧下分解反应的谐振以及非谐振速率常数。因此,甲基肼自由基的详细机理得以研究。在正则系综中,谐振以及非谐振速率常数都随着温度的升高而增加;而在微正则系综中,速率常数随着能量的升高而增加。整体上看,在正则系综和微正则系综中,非谐振效应分别随着温度和能量的升高而变得越来越明显。因此甲基肼自由基在高温燃烧下分解反应的非谐振效应是不能被忽视的。     

H2FCS单分子分解反应的直接动力学研究

采用量子化学QCISD(T)/6-311++G(d,p)//B3LYP/6-311+G(d,p)方法研究了H2FCS单分子分解反应的微观动力学性质, 构建了反应势能剖面. 利用经典过渡态理论(TST)与变分过渡态理论(CVT)并结合小曲率隧道效应模型(SCT), 分别计算了在200～3000 K温度范围内的速率常数kTST、kCVT和kCVT/SCT. 计算结果表明, H2FCS可经过不同的反应通道生成10种小分子产物, 脱H反应和HF消去反应为标题反应的主反应通道, 其中HF消去反应产物HCS可由两条反应通道生成. 在200~3000 K温度区间内得到三条反应通道的表观反应速率常数三参数表达式分别为 , 和 . 速率常数计算结果显示, 量子力学隧道效应在低温区间对反应速率常数的影响显著, 而变分效应在计算温度范围内可以忽略.     

CH3S与NO基态反应的机理及动力学

在G3(MP2)水平上,通过对CH3S与NO反应势能面(PES)上关键驻点的能量计算,共找到3种中间体、7个过渡态、9种产物通道,并对其反应机理进行了讨论.结果表明此反应主要以两种方式进行一是加成反应,先生成CH3SNO,然后发生单分子解离和异构化反应;二是直接抽提反应,生成CH2S+HNO.用多通道RRKM-TST模型计算了反应随温度和压力变化的速率常数.以295 K的N2作浴气,在200.0～39996.6 Pa压力范围的速率常数为1.6×10-12～1.28×10-11 cm3·molecule-1·s-1.我们计算的速率常数与Balla等的实验值符合较好.反应的速率常数有明显的负温度效应和较强的压力依赖关系.预测常压低温下反应以生成CH3SNO为主,在常压高温1000 K以上以生成CH2S+HNO为主.     

HS+HO2气相反应机理及主通道速率常数的理论研究

采用CCSD(T)/6-311++G(3df, 2pd)//B3LYP/6-311+G(2df, 2p)双水平计算方法构建了HO₂+HS反应体系的单、三重态反应势能面,并对该反应主通道的速率常数进行了研究。研究结果表明,标题反应经历了八条反应通道,其中三重态反应通道R1是标题反应主通道。此通道包含路径Path 1 (R → ³IM1 → ³TS1 → P1(³O₂+H₂S))和Path 1a (R → ³IM1a → ³TS1a → P1(³O₂+H₂S))两条路径。利用经典过渡态理论(TST)与变分过渡态理论(CVT)并结合小曲率隧道效应模型(SCT),分别计算了主路径Path 1和Path 1a在200-800 K温度范围内的速率常数k^TST、k^CVT和k^CVT/SCT,在此温度区间内路径Path 1和Path 1a具有负温度系数效应。速率常数计算结果显示,对主路径Path 1和Path 1a而言,变分效应在计算温度段内有一定影响,与此同时量子力学隧道效应在低温段有显著影响。路径Path 1和Path 1a的CVT/SCT速率常数的三参数表达式分别为k₁^CVT/SCT(200-800 K) = 1.54×10^-5T^-2.70exp(1154/T) cm³ ·molecule^-1·s^-1和k_1a^CVT/SCT(200-800 K) = 5.82×10^-8T^-1.84exp(1388/T) cm³·molecule^-1·s^-1。     

CH3CH2O+HCHO反应机理及主通道速率常数

采用CCSD(T)/cc-pVDZ//B3LYP/6-311++G(d,p)双水平计算方法研究了CH₃CH₂O+HCHO反应的微观反应机理. 结果表明, 标题反应主要存在5个抽氢和3个氢迁移异构化反应通道, 其中抽氢通道R→ IMa(CH₃CH₂O…CH₂O)→TS1→ IM1b→P1(CH₃CH₂OH+CHO)为优势通道, 其表观活化能为14.65 kJ/mol. 利用变分过渡态理论(CVT)并结合小曲率隧道效应模型计算了主通道R1在275~1000 K温度范围内的速率常数k^TST, k^CVT和k^CVT/SCT, 在此温度区间内表观反应速率常数三参数表达式为k^CVT/SCT=2.26×10^-17 T^0.57 exp(-1004/T), 显示具有正温度系数效应.     

氟代乙炔氢迁移反应微正则系综速率常数的计算

以氟代乙炔的氢迁移反应为例, 计算了隧道效应、曲率因子和转动选态对微正则系综单分子反应速率常数的影响。结果表明, 在低能区域, 隧道效应和曲率因子对反应速率有较大影响, 均使反应速率增加, 而在高能区域作用不明显。与此同时还研究了不同对称态下的反应速率常数, 结果表明, 本例中的两对称态(A'态和A"态)的反应速率常数在能量较低时差异较大, 随能量升高, 两者趋于相等。     

HCF(~1A'''')+SO_2反应的动力学研究

用激光光解-激光诱导荧光方法研究了室温下(T=293K)HCF(X%A′)自由基与SO2分子的反应动力学.实验中1HCF(X%A′)自由基是由213nm激光光解HCFBr2产生的,用激光诱导荧光(LIF)检测HCF(X%A′)自由基的相对浓度随着11反应时间的变化,得到此反应的二级反应速率常数为:k=(1.81±0.15)×10-12cm3?molecule-1?s-1,体系总压为1862Pa.高精度理论计算表明,HCF(X%A′)和SO2分子反应的机理是典型的加成-消除反应.我们运用RRKM-TST理论计算了1此二级反应速率常数的温度效应和压力效应,计算结果和室温下测定的二级反应速率常数符合得较好.     

CF_2ClC(O)OCH_2CH_3+OH的反应机理及动力学性质的理论研究

利用双水平直接动力学方法,在MCG3-MPWB//M06-2X/aug-cc-pVDZ水平上研究了CF_2ClC(0)OCH_2CH_3+OH的微观反应机理.得到了反应物CF_2ClC(O)OCH_2CH_3的5种稳定构象(RCl~RC5),并对每一构象考察了发生在-CH_3-和-CH_2-基团上的所有可能氢提取反应通道.利用改进的变分过渡态理论(ICVT)结合小曲率隧道效应校正(SCT)计算了各反应通道的速率常数,分析了各构象反应位点选择性.结果表明,对于构象RCl和RC2,低温时氢提取反应主要发生在-CH_2-基团上;而对于构象RC3RC4和RC5,发生在-CH_3基团上的氢提取反应通道在整个温度区间内占绝对优势.根据Boltzmann配分函数计算总包反应速率常数,在298 K温度下计算的体系总包反应速率常数与实验值相符,进而给出200~1000 K温度范围内拟合了速率常数的三参数Arrhenius表达式:k_(overall)=5.45×10~(25)T~(4.54)exp(-685/T).     

HNCS与CH2(X2Π)反应微观动力学的理论研究

用量子化学密度泛函理论的UB3LYP/6-311+G**方法和高级电子相关的UQCISD(T)/6-311+G**方法研究了异硫氰酸(HNCS)与乙炔基自由基(C2H(X2Π))反应的微观机理. 采用双水平直接动力学方法IVTST-M, 获取反应的势能面信息, 应用正则变分过渡态理论并考虑小曲率隧道效应, 计算了在250～2500 K温度范围内反应的速率常数. 研究结果表明, HNCS与C2H(X2Π)反应为多通道、多步骤的复杂反应, 共存在三个可能的反应通道, 主反应通道为通过分子间H原子迁移, 生成主要产物NCS+C2H2. 反应速率常数随温度升高而增大, 表现为正温度效应. 速率常数计算中变分效果很小. 在低温区隧道效应对反应速率的贡献较大, 反应为放热反应.     

HNCS与C_2H(X~2Π)反应微观动力学的理论研究

用量子化学密度泛函理论的UB3LYP/6-311 G鄢鄢方法和高级电子相关的UQCISD(T)/6-311 G鄢鄢方法研究了异硫氰酸(HNCS)与乙炔基自由基(C2H(X2Π))反应的微观机理.采用双水平直接动力学方法IVTST-M,获取反应的势能面信息,应用正则变分过渡态理论并考虑小曲率隧道效应,计算了在250～2500K温度范围内反应的速率常数.研究结果表明,HNCS与C2H(X2Π)反应为多通道、多步骤的复杂反应,共存在三个可能的反应通道,主反应通道为通过分子间H原子迁移,生成主要产物NCS C2H2.反应速率常数随温度升高而增大,表现为正温度效应.速率常数计算中变分效果很小.在低温区隧道效应对反应速率的贡献较大,反应为放热反应.     

Theoretical Study on Dissociation Mechanisms of Di-ethyl Berylliums and Di-t-butyl Berylliums

The potential energy surfaces (PES) of unimolecular dissociation reactions for di-ethyl beryl-lium and di-t-butyl beryllium are investigated by B3LYP, CCSD(T), and G3B3 approaches. Possible reaction pathways through either the radical or transition state (TS) of the molecules are considered. The geometries, vibrational frequencies and relative energies for various sta-tionary points are determined. From the study of energetics, the TS pathways arising from concerted molecular eliminations are indicated to be the main dissociation pathways for both molecules. The PES differences of the dissociation reactions are investigated. The activa-tion energies and rate constants will be helpful for investigating the predictive ability of the reaction in further theoretical and experimental research.     

Anharmonic Effect in CH<Subscript>3</Subscript>CH<Subscript>2</Subscript>C(=O)OCH<Subscript>2</Subscript>CH<Subscript>3</Subscript> Decomposition

In this paper, using the B3LYP functional and CCSD(T) method with 6-311++G** basis set, the harmonic and anharmonic rate constants in the unimolecular dissociation of ethyl propanoate have been calculated using Rice–Ramsperger–Kassel–Marcus theory. The anharmonic rate constants of the title reaction have also been examined, the comparison shows that, the anharmonic effect especially in the case of high total energies and temperature for channels 3 to 6 is significant, so that the anharmonic effect cannot be neglected for unimolecular dissociation reaction of CH₃CH₂C(=O)OCH₂CH₃ both in microcanonical and canonical systems.     

Anharmonic Effect of the Unimolecular Dissociation of Ethyl Radical

The anharmonic and harmonic rate constants have been calculated for the unimolecular dissociation of ethyl radical using the method proposed by Yao and Lin (YL method) at both B3LYP/6‐311++G** and MP2/6‐311++G** levels. The different rate constants indicate that the results obtained from B3LYP and MP2 method are very close. The anharmonic and tunneling effect of the title reaction has also been examined. The comparison shows that, both in microcanonical and canonical systems, the anharmonic rate constants are higher than those for harmonic cases, especially in the case of high total energies and temperatures, which indicates that anharmonic effect of the unimolecular dissociation of ethyl into C₂H₄ and H is so significant that cannot be neglected. The tunneling effect is very small for the decomposition of C₂H₅ radical.     

Ab initio study of the SN1Ar and SN2Ar reactions of benzenediazonium ion with water. On the conception of "unimolecular dediazoniation" in solvolysis reactions

The nucleophilic substitution of N2 in benzenediazonium ion 1 by one H2O molecule to form protonated phenol 2 has been studied with ab initio (RHF, MP2, QCISD(T)//MP2) and hybrid density functional (B3LYP) methods. Three mechanisms were considered: (a) the unimolecular process SN1Ar with steps 1 --> Ph+ + N2 and Ph+ + H2O --> 2, (b) the bimolecular process SN2Ar with precoordination 1 + H2O --> 1 x H2O, SN reaction 1 x H2O --> [TS]++ --> 2 x N2 and dissociation of the postcoordination complex 2 x N2 --> 2 + N2, and (c) the direct bimolecular process SN2Ar that bypasses precoordination and involves just the SN reaction 1 + H2O --> [TS]++ --> 2 + N2. The SN2Ar reactions proceed by way of a Cs symmetric SN2Ar transition state structure that is rather loose, contains essentially a phenyl cation weakly bound to N2 and OH2, and is analogous to the transition state structures of front-side nucleophilic replacement at saturated centers. In solvolysis reactions, all of these processes follow first-order kinetics, and the electronic relaxation is essentially the same. It is argued that "unimolecular dediazoniations" have to proceed by way of SN2Ar transition state structures because strict SN1Ar reactions cannot be realized in solvolyses, despite the fact that the Gibbs free energy profile favors the strict SN1Ar process over the SN2Ar reaction by 6.7 kcal/mol. It is further argued that the direct SN2Ar process is the best model for the solvolysis reaction for dynamic reasons, and its Gibbs free energy of activation is 19.3 kcal/mol and remains higher than the SN1Ar value. Even though the SN1Ar and SN2Ar models provide activation enthalpies and SKIE values that closely match the experimental data, the analysis leads us to the unavoidable conclusion that this agreement is fortuitous. While the experiments do show that the solvent effect on the activation energy is about the same for all solvents, they do not show the absence of a solvent effect. The ab initio results presented here suggest that the solvent effect on the direct SN2Ar dediazoniation is approximately 12 kcal/mol, and computation of solvent effects with the isodensity polarized continuum model (IPCM) support this conclusion.     

Tandem mass spectrometric study of 1,3,5-trinitrobenzene molecular ion: an unusual ortho effect involving a hydrogen atom from the aromatic ring

Unimolecular (metastable) and collision-induced dissociation of 1,3, 5-trinitrobenzene molecular ion was studied using linked scans and mass-analyzed ion kinetic energy spectrometry on a hybrid instrument of EBEqQ geometry. An unusual ortho effect leading to the loss of OH radical from the parent molecular ion is observed as a unimolecular dissociation process only in the first-field free region between the ion source and the electric sector, although corresponding dissociation in the ion source is of negligible abundance (<0.1%). This unimolecular process is taken over by other dissociation pathways when the parent ion is collisionally activated, suggesting that this dissociation process occurs only in a very narrow energy window with a rate constant of the order of 2 x 10(5) s(-1). Copyright 2000 John Wiley & Sons, Ltd.     

水催化2个酯分子相互转化反应的理论研究

从印楝植物内生真菌Phomopsis sp.培养液中分离得到的4-acetoxymultiplolide(1)和1-acetoxymultiplo-lide(2)在室温及水存在下能够相互转化. 提出二者相互转化最可能的4个途径(机理A~D). 在B3LYP/6-311+G(d,p)水平进行气相条件的优化, 结果表明, 无水催化的机理A中TS1和TS2的活化能均显著大于120 kJ/mol, 2个分子水催化的机理D中TS1和TS2的活化能则显著降低. 计算结果显示水的溶剂化效应能进一步降低机理D中TS1和TS2的活化能. 在MP2/6-311++G(2d,2p)//B3LYP/6-311+G(d,p)水平计算了单点能, 得到在水相时机理D中TS1和TS2的活化能分别为106.24和107.37 kJ/mol. 因此, 机理D是化合物1 和2在室温下及水存在时相互转化最可能的途径, 该途径是一种特殊的水催化分子内酯的醇解反应, 也是一种经典的亲核加成反应, 通过一种新的叔醇中间体实现.     

Theoretic studies on the kinetics and mechanism of multi-channel gas-phase unimolecular reactions of 1-chloropropane and 2-chloropropane

The potential energy surfaces of the gas-phase unimolecular decomposition reactions of 1-chloropropane and 2-chloropropane are investigated by various quantum chemical methods including CCSD(T), CCSD, GBS-QB3, C3B3, MP4, MP2, and B3LYP. Modified strong collision/RRKM theory was used to calculate the unimolecular rate constants as a function of pressure and temperature. It is found that the major reaction pathway is the HCl elimination. It is predicted that bond dissociation reactions have negligible contribution to the overall rate constant. The computed rate constants are compared with the available experimental data.     

Increased cytotoxicity and phototoxicity in the methylene blue series via chromophore methylation

The cytotoxic and photodynamic activities of the commercially-available biological stains methylene blue (MB), 1,9-dimethyl MB (Taylor's Blue) and a newly synthesised compound, 1-methyl MB, were measured against the murine mammary tumour cell line, EMT-6 Both 1-methyl MB and 1,9-dimethyl MB exhibited increased dark toxicity with concomitant higher phototoxicity compared to MB at a light dose of 7.2 J cm⁻². While increasing the light dose as a function of the fluence rate increased the photocytotoxicity of MB, this had little effect on the methylated derivatives. In vitro chemical testing proved that successive methylation rendered the phenothiazinium chromophore both more resistant to reduction to its inactive leuco form, and also led to increased levels of singlet-oxygen production, thus providing a possible explanation for the increased toxicities of the methylated derivatives. Comparisons are made with the benzo[a]phenothiazinium photosensitizer, EtNBS.