M7. Kinetics and Atmospheric Implications of Peroxy Radical Cross Reactions Involving the CH3C(O)O2 Radical

 

E. Villenave a, R. Lesclaux a, S. Seefeld b, W. R. Stockwell c

a Laboratoire de Photophysique et Photochimie Moléculaire, Université Bordeaux I, Talence, France

b EAWAG, Swiss Federal Institute for Environmental Science and Technology, Zürich, Switzerland

c Fraunhofer Institute for Atmospheric Environmental Science and Technology, Garmisch, Germany

e-mail: eric.villenave@nist.gov

 

 Organic peroxy radicals (RO2) represent an important class of intermediates formed in the atmospheric oxidation processes of hydrocarbons.1,2 Their tropospheric chemistry involves several competing reactions, depending on the distribution of relevant trace atmospheric constituents. It is now well accepted that for low NOx concentrations, the principal loss process for peroxy radicals in the troposphere is by reaction with HO2.1 However, in hydrocarbon-rich atmospheres such as in the marine boundary layer or forest areas, it has been shown that high concentrations of RO2 radicals can build up, such that RO2 self- and cross reactions may also have to be taken into account, provided such reactions are fast enough.3 The objectives of the present work were to investigate the kinetics of the reactions of selected peroxy radicals with CH3C(O)O2 which, after HO2 and CH3O2, appears to be the most abundant peroxy radical in the remote troposphere.3 Acetylperoxy radicals are known to be formed as a consequence of the photooxidation of higher carbonyl compounds, and are important in many atmospheric processes, as they appear to be a significant contributor to smog formation, as precursor of PAN (peroxyacetylnitrate).4

The kinetics of the cross reactions of c-C6H11O2, sec-C10H21O2, sec-C12H25O2 and t-C4H9O2 with CH3C(O)O2 were investigated in this work using the flash photolysis technique coupled with UV absorption spectrometry. Radicals were generated by photolysis of either molecular chlorine or molecular bromine, in the presence of suitable hydrocarbons and oxygen. All reaction kinetics were investigated at 760 Torr total pressure and at room temperature. Values of (1.0 ± 0.1) x 10-11, (1.1 ± 0.2) x 10-11, (1.0 ± 0.6) x 10-11 and (1.1 ± 0.3) x 10-11 (units of cm3 molecule-1 s-1) have been obtained for the rate constants of the reactions of CH3C(O)O2 radicals with c-C6H11O2, sec-C10H21O2, sec-C12H25O2 and t-C4H9O2 radicals, respectively.

The present results, combined with the results previously reported for primary peroxy radicals CH3O2 and C2H5O2,5-7 (Table 1) show that all cross reactions of CH3C(O)O2 are fast with rate constants around 1.0 x 10-11 cm3 molecule-1 s-1, independent of the RO2 radical structure and of its rate constant for self reaction. This suggests that all acylperoxy radicals (ACO3) present the same high reactivity as CH3C(O)O2 and hence, it is proposed to assign the above rate constant value to all cross reactions of ACO3 radicals. These new rate constant values were implemented in the Regional Atmospheric Chemistry Mechanism (RACM),8 to estimate the importance of the cross reactions in the chemistry of acylperoxy radicals in the troposphere. In the case of a moderately polluted troposphere, under low NOx and high VOC concentrations, the cross reactions of acylperoxy radicals with organic peroxy radicals account for more than 20 % of the acylperoxy loss reactions (Figure 1), and PAN concentrations decrease by more than 4 %, compared with the previous estimates of Kirchner and Stockwell9.


(1) P.D. Lightfoot, R.A. Cox, J.N. Crowley, M. Destriau, G.D. Hayman, M.E. Jenkin, G.K. Moortgat, and F. Zabel, Atmos. Environ., 1992, 26A, 1806.

(2) T.J. Wallington, P. Dagaut, and M.J. Kurylo, Chem. Rev., 1992, 92, 667.

(3) S. Madronich and J.G. Calvert, J. Geophys. Res., 1990, 95, 5697.

(4) H.B. Singh, D. O’Hara, D. Herlth, J.D. Bradshaw, S.T. Sandholm, G.L. Gregory, G.W. Sachse, D.R. Blake, P.J. Crutzen, and M.A. Kanakidou, J. Geophys. Res., 1992, D15, 16511.

(5) E. Villenave and R. Lesclaux, J. Phys. Chem., 1996, 100, 14372.

(6) C.M. Roehl, D. Bauer, and G.K. Moortgat, J. Phys. Chem., 1996, 100, 4038.

(7) M.M. Maricq and J.J. Szente, J. Phys. Chem., 1996, 100, 4507.

(8) W.R. Stockwell, F. Kirchner, M. Kuhn, and S. Seefeld, J. Geophys. Res., 1997, in press.

(9) F. Kirchner and W.R. Stockwell, J. Geophys. Res., 1996, 101 (D15), 21007.

 

TABLE 1. Rate Constants at 298 K (in cm3 molecule-1 s-1) for RO2 + CH3C(O)O2

Cross Reactions; RO2 Self Reactions are Included for Comparison.

RO2 1011 k(RO2 + CH3C(O)O2) 1011 k(RO2 + RO2)
     
CH3C(O)O2 - 1.4
CH3O2 0.95 ± 0.2 0.037
C2H5O2 1.0 ± 0.5 0.0070
CH3C(O)CH2O2 0.5 ± 0.2 0.80
t-C4H9O2 1.1 ± 0.4 0.000003
c-C6H11O2 1.0 ± 0.4 0.0042
sec-C10H21O2 1.1 ± 0.6 0.0082
sec-C12H25O2 1.0 ± 0.8 0.011

 

FIGURE 1. Fraction of ACO3 reaction rates during the 5th day of the Plume case at 298 K with 100 % emissions. The dotted lines shows the NO2 photolysis frequencies and gives a measure of the day-night cycle.