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采用CCSD(T)//B3LYP/6-311+G(d,p)方法研究了Criegee中间体CH_3CHOO与OH自由基反应的微观机理.结果表明,上述反应存在抽氢、加成-分解和氧化3类反应通道,其中,syn-CH3CHOO+OH以抽β-H为优势通道,表观活化能为-4.88 k J/mol;anti-CH_3CHOO+OH则以加成-分解反应为优势通道,表观活化能为-13.25 k J/mol.在加成-分解和氧化反应通道中,anti-构象的能垒均低于syn-构象,而抽氢反应则是syn-(β-H)的能垒低于anti-构象.速率常数计算表明,anti-构象的加成-分解反应通道具有显著的负温度效应;syn-和anti-构象的氧化通道具有显著的正温度效应.3类反应具有显著不同的温度效应,说明通过改变温度可显著调节3类反应的相对速率. 相似文献
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采用CCSD(T)/aug-cc-p VTZ//B3LYP/6-311+G(2df,2p)方法对Criegee中间体RCHOO(R=H,CH_3)与NCO反应的机理进行了研究,利用经典过渡态理论(TST)并结合Eckart校正模型计算了标题反应在298~500 K范围内优势通道的速率常数.结果表明,上述反应包含亲核加成、氧化和抽氢3类机理,其中每类又包括NCO中N和O分别进攻的两种形式.亲核加成反应中O端进攻为优势通道,氧化和抽氢反应则是N端进攻为优势通道;甲基取代使CH_3CHOO反应活性高于CH2OO;anti-CH_3CHOO的加成及氧化反应活性高于syn-CH_3CHOO,而抽氢反应则是syn-CH_3CHOO的活性高于anti-CH_3CHOO.anti-构象对总速率常数的贡献大于syn-构象,且总速率常数具有显著的负温度效应. 相似文献
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采用密度泛函理论BB1K/6-31+G(d,p)计算了反应CF3CH2CH3+OH各反应通道上驻点的稳定结构和振动频率, 并分别在BMC-CCSD, MC-QCISD和G3(MP2)水平上进行了单点能校正. 运用变分过渡态理论, 在BMC-CCSD//BB1K, MC-QCISD//BB1K, G3(MP2)//BB1K以及BB1K水平上计算了各反应通道的速率常数, 讨论了-CH2和-CH3基团上H提取通道对总反应的贡献, 并与已有实验和理论结果进行了对比. 计算结果表明, BMC-CCSD水平上的速率常数与实验测量值符合得很好, 进而给出了该水平上反应在200~1000 K温度范围内速率常数k(cm3?molecule-1?s-1)的三参数表达式: k=1.90×10-21T3.21exp(-292.62/T). 相似文献
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用密度泛函理论(DFT)的B3LYP方法,在6-311G、6-311+G(d)、6-311++G(d, p) 基组水平上研究了CH3CF2O2与HO2自由基反应机理. 结果表明, CH3CF2O2与HO2自由基反应存在两条可行的通道. 通道CH3CF2O2+HO2→IM1→TS1→CH3CF2OOH+O2的活化能为77.21 kJ•mol-1,活化能较低,为主要反应通道,其产物是O2和CH3CF2OOH. 这与实验结果是一致的;而通道CH3CF2O2+HO2→IM2→TS2→IM3→TS3→IM4+IM5→IM4+TS4→IM4+OH+O2→TS5+OH+O2→CH3+CF2O+OH+O2→CH3OH+CF2O+O2的控制步骤活化能为93.42 kJ•mol-1,其产物是CH3OH、CF2O和O2. 结果表明这条通道也能发生,这与前人的实验结果一致. 相似文献
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在G3B3,CCSD(T)/6-311++G(d,p)//B3LYP/6-311++G(d,p)水平上详细研究了CH3SH与基态NO2的微观反应机理.在B3LYP/6-311++G(d,p)水平得到了反应势能面上所有反应物、过渡态和产物的优化构型,通过振动频率分析和内禀反应坐标(IRC)跟踪验证了过渡态与反应物和产物的连接关系.在CCSD(T)/6-311++G(d,p)和G3B3水平计算了各物种的能量,得到了反应势能面.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200~3000K温度范围内的速率常数kTST,kCVT和kCVT/SCT.研究结果表明,该反应体系共存在5个反应通道,其中N进攻巯基上H原子生成CH3S+HNO2的通道活化势垒较低,为主要反应通道.动力学数据也表明,该通道在200~3000K计算温度范围内占绝对优势,拟合得到的速率常数表达式为k1CVT/SCT=1.93×10-16T0.21exp(-558.2/T)cm3·molecule-1·s-1. 相似文献
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采用双水平直接动力学方法对C2H3与CH3F氢抽提反应进行了研究. 在QCISD(T)/6-311++G(d, p)//B3LYP/6-311G(d, p)水平上, 计算的三个反应通道R1、R2和R3的能垒(ΔE≠)分别为43.2、43.9和44.1 kJ·mol-1, 反应热为-38.2 kJ·mol-1. 此外, 利用传统过渡态理论(TST)、正则变分过渡态理论(CVT)和包含小曲率隧道效应(SCT)的CVT, 分别计算了200-3000 K温度范围内反应的速率常数kTST、kCVT和kCVT/SCT. 结果表明: (1) 三个氢抽提反应通道的速率常数随温度的增加而增大, 其中变分效应的影响可以忽略, 隧道效应则在低温段影响显著; (2) R1反应是主反应通道, 但随着温度的升高, R2反应的竞争力增大, 而R3反应对总速率常数的影响很小. 相似文献
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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)=2.06×10-20T3.045exp(-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. 相似文献
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在6-311+G(2d,2p)水平下, 采用密度泛函理论(DFT)的B3LYP方法, 研究了Criegee 自由基CH2O2与H2O的反应. 结果表明反应存在三个通道: CH2O2+H2O®HOCH2OOH (R1); CH2O2+H2O®HCO+OH+H2O (R2); CH2O2+H2O®HCHO+H2O2 (R3), 各通道的势垒高度分别为43.35, 85.30和125.85 kJ/mol. 298 K下主反应通道(R1)的经典过渡态理论(TST)与变分过渡态理论(CVT)的速率常数kTST与kCVT均为2.47×10-17 cm3•molecule-1•s-1, 而经小曲率隧道效应模型(SCT)校正后的速率常数kCVT/SCT为 5.22×10-17 cm3•molecule-1•s-1. 另外, 还给出了200~2000 K 温度范围内拟合得到的速率常数随温度变化的三参数Arrhenius方程. 相似文献
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Yang Yong Zhang Weijun Gao Xiaoming Pei Shixin Shao Jie Huang Wei Qu Jun 《化学物理学报(中文版)》2005,18(4):515-521
The reaction for CH3CH2+O(3P) was studied by ab initio method. The geometries of the reactants, intermediates, transition states and products were optimized at MP2/6-311+G(d,p) level. The corresponding vibration frequencies were calculated at the same level. The single-point calculations for all the stationary points were carried out at the QCISD(T)/6-311+G(d,p) level using the MP2/6-311+G(d,p) optimized geometries. The results of the theoretical study indicate that the major products are the CH2O+CH3, CH3CHO+H and CH2CH2+OH in the reaction. For the products CH2O+CH3 and CH3CHO+H, the major production channels are A1: (R)→IM1→TS3→(A) and B1: (R)→IM1→TS4→(B), respectively. The majority of the products CH2CH2+OH are formed via the direct abstraction channels C1 and C2: (R)→TS1(TS2)→(C). In addition, the results suggest that the barrier heights to form the CO reaction channels are very high, so the CO is not a major product in the reaction. 相似文献
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On the basis of the computed results got by the Gaussian 94 package at B3LYP/6-311 G** level,the reaction mechanism of CH3O radical with CO has been investiagted thoroughly via the vibrational model analysis ,And the relationships among the reactants,eight transition states,four intermediates and various products involved this multichannel reation are eluci-dated,The vibrational mode anaysis shows that the reaction mechanism is relialbe. 相似文献
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Lü Ling-Ling 《结构化学》2008,27(9):1039-1044
The insertion reaction mechanism of CF2 with CH2O was investigated at the B3LYP/6-311G(d)//MP2/6-311G(d) level. The geometric conformations at each stationary point in reaction potential surface were fully optimized and the transition states were verified by intrinsic reaction coordinate (IRC) and frequency analysis. The energies of all reactants were calculated with CCSD(T)/6-311G(d)//G2MP2 methods. Results indicated that the P1 reaction route with difuoroaldehyde as product is the dominant reaction pathway, which exhibits nucleophilic character. According to NBO analysis, the starting point of insertion reaction is the interaction between carbene LP(C3) and formaldehyde π(Cl-O2). Besides, the thermodynamic and dynamic properties of dominated reaction (1) at different temperature were studied with statistic thermodynamic method and Eyring transition state theory adjusted by Wigner means, from which the proper temperature (500- 1200 K) of reaction (1) could be estimated. Finally, the thermo- dynamic and dynamic properties of insertion reaction mechanisms (CF2, CX2 (X = Cl, Br) with CH2O) were compared and discussed. 相似文献
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Dr. Edmond P. F. Lee Dr. Daniel K. W. Mok Prof. Dudley E. Shallcross Prof. Carl J. Percival Dr. David L. Osborn Prof. Craig A. Taatjes Prof. John M. Dyke 《Chemistry (Weinheim an der Bergstrasse, Germany)》2012,18(39):12411-12423
CH2OO, the simplest Criegee intermediate, and ozone are isoelectronic. They both play very important roles in atmospheric chemistry. Whilst extensive experimental studies have been made on ozone, there were no direct gas‐phase studies on CH2OO until very recently when its photoionization spectrum was recorded and kinetics studies were made of some reactions of CH2OO with a number of molecules of atmospheric importance, using photoionization mass spectrometry to monitor CH2OO. In order to encourage more direct studies on CH2OO and other Criegee intermediates, the electronic and photoelectron spectra of CH2OO have been simulated using high level electronic structure calculations and Franck–Condon factor calculations, and the results are presented here. Adiabatic and vertical excitation energies of CH2OO were calculated with TDDFT, EOM‐CCSD, and CASSCF methods. Also, DFT, QCISD and CASSCF calculations were performed on neutral and low‐lying ionic states, with single energy calculations being carried out at higher levels to obtain more reliable ionization energies. The results show that the most intense band in the electronic spectrum of CH2OO corresponds to the ${{\rm{\tilde B}}}$ 1A′ ← ${{\rm{\tilde X}}}$ 1A′ absorption. It is a broad band in the region 250–450 nm showing extensive structure in vibrational modes involving O–O stretching and C‐O‐O bending. Evidence is presented to show that the electronic absorption spectrum of CH2OO has probably been recorded in earlier work, albeit at low resolution. We suggest that CH2OO was prepared in this earlier work from the reaction of CH2I with O2 and that the assignment of the observed spectrum solely to CH2IOO is incorrect. The low ionization energy region of the photoelectron spectrum of CH2OO consists of two overlapping vibrationally structured bands corresponding to one‐electron ionizations from the highest two occupied molecular orbitals of the neutral molecule. In each case, the adiabatic component is the most intense and the adiabatic ionization energies of these bands are expected to be very close, at 9.971 and 9.974 eV at the highest level of theory used. 相似文献
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The potential energy surface (PES) of CH3SO radical with NO reaction has been studied at MP2/6-311G(2df, p) and QCISD/6-311G(2df, p) levels. Geometries of the reactants, transition states (TS) and products were optimized at B3LYP/6-311G (d,p) level. The geometries of the transition states were found for the first time. The calculated results show that the reaction can proceed via singlet-state or triplet-state PES. Because of the high energy barrier of triplet surface, the singlet surface reactions are dominant. The topological analysis of electron density shows that there are two kinds of structaral transition states (the bifurcation-type ring structure transition state and the T-shaped conflict structure transition state) in the titled reaction. The total electronic density of the reactants, TS and products and the spin electronic density on the triplet surface were also discussed in this paper. 相似文献