Sengupta Sumana, Indulkar Yogesh, Kumar Awadhesh, Dhanya Suresh, Naik Prakash Dattatray, Bajaj Parma Nand
Radiation and Photochemistry Division, Bhabha Atomic Research Center, Mumbai 400 085, India.
J Phys Chem A. 2008 Dec 11;112(49):12572-81. doi: 10.1021/jp806965p.
Dynamics of formation of electronically excited NO2 and formation of OH fragment, during photo dissociation of 2-nitropropane (NP) and 2-methyl-2-nitropropane (MNP), were investigated at 193 and 248 nm. The radiative lifetime of the electronically excited NO2 fragment, observed at 193 nm, was measured to be 1.2 ( 0.1 micros and the rate coefficient of quenching of its emission by MNP was measured as (2.7 ( 0.1) x 10(-10) molecule(-1) cm3 s(-1). Formation of the ground electronic state of OH was confirmed in both molecules. State selective laser induced fluorescence technique was used to detect the nascent OH (X 2Pi, v'', J'') fragments in different ro-vibrational states, and to obtain information on energy partitioning. Though MNP and NP differ in the types of the available H atoms, the dynamics of OH formation is found to be the same in both. The relative population in different rotational states does not follow Boltzmann equilibrium distribution in both the molecules at 193 and 248 nm. The translational energies of the OH fragments, calculated from the Doppler width, are 21.2 ( 7.2 and 25.0 ( 2.5 kcal mol-1 for NP at 248 and 193 nm, respectively. The translational energies of the OH fragments, in the case of MNP, are found to be lower, 17.5 ( 4.1 and 22.0 ( 3.2 kcal mol-1,respectively, at 248 nm 193 nm. These results are compared with the earlier reports on photodissociation of nitromethane (NM), nitroethane (NE), and other nitroalkanes. All possible dissociation pathways of these molecules--NM, NE, NP, and MNPs leading to the formation of the OH fragment were investigated computationally, with geometry optimization at the B3LYP/6-311+G(d,p) level and energy calculation at the MP4(SDQ)/6-311+G (d,p) level. The results suggest that in NM, OH is formed after isomerization to CH2N(OH)O, whereas in all other cases OH is formed from HONO, a primary product of molecular elimination of nitroalkanes, formed with sufficient internal energy.
研究了2-硝基丙烷(NP)和2-甲基-2-硝基丙烷(MNP)在193和248nm光解离过程中电子激发态NO2的形成动力学以及OH碎片的形成。在193nm处观测到的电子激发态NO2碎片的辐射寿命经测量为1.2(±0.1)微秒,其发射被MNP猝灭的速率系数经测量为(2.7(±0.1)×10^(-10)分子^(-1)厘米^3秒^(-1)。在这两种分子中均证实了基态OH的形成。采用态选择性激光诱导荧光技术检测处于不同转动-振动状态的新生OH(X 2Pi,v'',J'')碎片,并获取能量分配信息。尽管MNP和NP在可用H原子类型上存在差异,但发现二者OH的形成动力学相同。在193和248nm时,这两种分子中不同转动状态的相对丰度均不符合玻尔兹曼平衡分布。由多普勒宽度计算得出,NP在248和193nm时OH碎片的平动能分别为21.2(±7.2)和25.0(±2.5)千卡/摩尔。在MNP的情况下,OH碎片的平动能在248nm和193nm时分别较低,为17.5(±4.1)和22.0(±3.2)千卡/摩尔。将这些结果与早期关于硝基甲烷(NM)、硝基乙烷(NE)及其他硝基烷烃光解离的报道进行了比较。对这些分子(NM、NE、NP和MNP)导致OH碎片形成的所有可能解离途径进行了计算研究,在B3LYP/6-311+G(d,p)水平进行几何优化,在MP4(SDQ)/6-311+G(d,p)水平进行能量计算。结果表明,在NM中,OH是在异构化为CH2N(OH)O后形成的,而在所有其他情况下,OH是由硝基烷烃分子消除的主要产物HONO形成的,且HONO形成时具有足够的内能。