Morajkar Pranay, Bossolasco Adriana, Schoemaecker Coralie, Fittschen Christa
Université Lille Nord de France, PhysicoChimie des Processus de Combustion et de l'Atmosphère - PC2A, UMR 8522, F-59650 Villeneuve d'Ascq, France.
J Chem Phys. 2014 Jun 7;140(21):214308. doi: 10.1063/1.4878668.
Radical quantum yields have been measured following the 248 nm photolysis of acetaldehyde, CH3CHO. HCO radical and H atom yields have been quantified by time resolved continuous wave Cavity Ring Down Spectroscopy in the near infrared following their conversion to HO2 radicals by reaction with O2. The CH3 radical yield has been determined using the same technique following their conversion into CH3O2. Absolute yields have been deduced for HCO radicals and H atoms through fitting of time resolved HO2 profiles, obtained under various O2 concentrations, to a complex model, while the CH3 yield has been determined relative to the CH3 yield from 248 nm photolysis of CH3I. Time resolved HO2 profiles under very low O2 concentrations suggest that another unknown HO2 forming reaction path exists in this reaction system besides the conversion of HCO radicals and H atoms by reaction with O2. HO2 profiles can be well reproduced under a large range of experimental conditions with the following quantum yields: CH3CHO + hν(248nm) → CH3CHO*, CH3CHO* → CH3 + HCO ϕ(1a) = 0.125 ± 0.03, CH3CHO* → CH3 + H + CO ϕ(1e) = 0.205 ± 0.04, CH3CHO*[Formula: see text]CH3CO + HO2 ϕ(1f) = 0.07 ± 0.01. The CH3O2 quantum yield has been determined in separate experiments as ϕ(CH₃) = 0.33 ± 0.03 and is in excellent agreement with the CH3 yields derived from the HO2 measurements considering that the triple fragmentation (R1e) is an important reaction path in the 248 nm photolysis of CH3CHO. From arithmetic considerations taking into account the HO2 and CH3 measurements we deduce a remaining quantum yield for the molecular pathway: CH3CHO* → CH4 + CO ϕ(1b) = 0.6. All experiments can be consistently explained with absence of the formerly considered pathway: CH3CHO* → CH3CO + H ϕ(1c) = 0.
在248nm光解乙醛(CH₃CHO)后测量了自由基量子产率。通过时间分辨连续波腔衰荡光谱法在近红外区域对HCO自由基和H原子与O₂反应转化为HO₂自由基后的产率进行了定量。在CH₃自由基转化为CH₃O₂后,使用相同技术测定了CH₃自由基产率。通过将在各种O₂浓度下获得的时间分辨HO₂谱拟合到一个复杂模型,推导出了HCO自由基和H原子的绝对产率,而CH₃产率是相对于CH₃I在248nm光解产生的CH₃产率测定的。极低O₂浓度下的时间分辨HO₂谱表明,除了HCO自由基和H原子与O₂反应转化外,该反应体系中还存在另一条未知的HO₂形成反应路径。在以下量子产率下,HO₂谱在大范围实验条件下都能得到很好的重现:CH₃CHO + hν(248nm) → CH₃CHO*,CH₃CHO* → CH₃ + HCO ϕ(1a) = 0.125 ± 0.03,CH₃CHO* → CH₃ + H + CO ϕ(1e) = 0.205 ± 0.04,CH₃CHO*[公式:见正文]CH₃CO + HO₂ ϕ(1f) = 0.07 ± 0.01。在单独实验中测定的CH₃O₂量子产率为ϕ(CH₃) = 0.33 ± 0.03,考虑到三重碎片化(R1e)是CH₃CHO在248nm光解中的重要反应路径,这与从HO₂测量得出的CH₃产率非常一致。从考虑HO₂和CH₃测量的算术计算中,我们推导出分子路径的剩余量子产率:CH₃CHO* → CH₄ + CO ϕ(1b) = 0.6。所有实验都可以通过不存在先前考虑的路径:CH₃CHO* → CH₃CO + H ϕ(1c) = 0来一致地解释。