193 nm photolysis of CHCl3: Probe of the CH product by CRDS

The CH radical production induced by 193 nm two-photon photolysis of CHCl₃ has been measured for the first time via the cavity ring-down absorption spectroscopy of its A–X bands, using a commercial nanosecond pulsed dye laser. The range of pressure and laser intensity, as well as the time window detection, have been carefully chosen to ensure a constant CH number density during the measurement and to avoid post-photolysis reactivity. Internal energy distribution of the CH(X²II) fragment has been derived from population distribution simulations, leading to an average vibrational temperature T_vib = 1900 ± 50 K and rotational temperature T_rot = 300 ± 20 K. Two competing mechanisms can be invoked for the CH production channel: either two-photon absorption via resonant excited states of CHCl₃ leading to dissociation of excited CHCl₃, or two-photon sequential dissociation via the formation of the vibrationally excited CHCl₂ fragment. The latter mechanism is proposed to be the prominent process for CH formation.     

Simultaneous high speed PIV and CH PLIF using R-branch excitation in the C2Σ+-X2Π (0,0) band

Simultaneous particle image velocimetry (PIV) and planar laser-induced fluorescence (PLIF) utilizing R-branch transitions in the C-X (0,0) band were performed at a 10-kHz repetition-rate in a turbulent premixed flame. The CH lines at 310.690?nm (from the R-branch of the C-X band) used here have greater efficiency than A-X and B-X transitions, which allows for high-framerate imaging with low laser pulse energy. Most importantly, the simultaneous imaging of both CH PLIF and PIV is enabled by the use of a custom edge filter, which blocks scattering at the laser wavelength (below ～311?nm) while efficiently transmitting fluorescence at longer wavelengths. The Hi-Pilot Bunsen burner operated with a turbulent Reynolds number of 7900 was used to demonstrate simultaneous PIV and CH PLIF utilizing this filtered detection scheme. Instances where pockets of products were observed well upstream of the mean flame brush are found to be the result of out-of-plane motion of the flame sheet. Such instances can lead to ambiguous results when interpreting the thickness of reaction layers. However, the temporally resolved nature of the present diagnostics facilitate the identification and proper treatment of such situations. The strategy demonstrated here can yield important information in the study of turbulent flames by providing temporally resolved flame dynamics in terms of flame sheet visualization and velocity fields.     

CH(X2∏)+N2O的反应机理研究

在G2(B3LYP/MP2/CC)理论水平上研究了CH(X2∏)自由基与氧化二氮(NNO)分子的反应.计算了反应体系的最低二重态势能面上各驻点的构型参数、振动频率和能量,揭示了此反应存在两种机理和六个通道其中HC和NNO复合,生成中间体HC(N)NO,解离得到产物HCN+NO,这是最主要的通道之一;HC插入NO键,克服38.9 KJ/mol的势垒,产生富能的中间体HC(O)NN,预测了五个反应通道,其中主要反应通道为:NN+HCO.     

CH与H2分子反应动力学及选态反应的理论研究

次甲基作为化学反应源曾引起广泛的兴趣.Schaefer 及其合作者于1977年对反应CH(~4Σ~-)+H_2→CH_2(~3B_1)+H 进行过量子化学研究,但是计算中限制了一些自由度.近年来,由于能量梯度方法的发展,反应途径哈密顿理论和变分过渡态理论的提出,有可能进一步对该反应进行分子反应动力学性质的研究.本文用从头算UHF/6-31G 方法和能量梯度方法首先优化出上述反应(原子编号为CH_a+H_bH_c→H_bCH_a+H_c)的过渡态;再用     

CH(X~2∏)+N_2O的反应机理研究

在G2 (B3LYP/MP2 /CC)理论水平上研究了CH(X2 ∏ )自由基与氧化二氮 (NNO)分子的反应 .计算了反应体系的最低二重态势能面上各驻点的构型参数、振动频率和能量 ,揭示了此反应存在两种机理和六个通道 .其中HC和NNO复合 ,生成中间体HC(N)NO ,解离得到产物HCN +NO ,这是最主要的通道之一 ;HC插入NO键 ,克服 38.9kJ/mol的势垒 ,产生富能的中间体HC(O)NN ,预测了五个反应通道 ,其中主要反应通道为 :NN +HCO .     

CH(X2∏)+N2O的反应机理研究

在G2(B3LYP/MP2/CC)理论水平上研究了CH(X^2Ⅱ)自由基与氧化二氮（NNO）分子的反应。计算了反应体系的最低二重态势能面上各驻点的构型参数、振动频率和能量，揭示了此反应存在的两种机理和六个通道。基中HC和NNO复合，生成中间体HC(N)NO，解离得到产物HCN+NO，这是最主要的通道之一；HC插入NO键，克服38.9kJ/mol的势垒，产生富能的中间体HC(O)NN，预测了五个反应通道，其中主要反应通道为：NN+HCO.