478
E.A. Wade et al. / Chemical Physics Letters 365 (2002) 473–479
obscured by strong phosgene bands at 1827 and
1837 cmꢁ1. Similarly, the 691 cmꢁ1 band is pre-
dicted to have nearly the same intensity as the
791 cmꢁ1 band, but is very close to a strong
chloropicrin band at 674 cmꢁ1 and would likely
not be observed. The fifth predicted band, at
617 cmꢁ1, is not observed, but is predicted to be
the weakest of these five bands with less than one-
third the intensity of the 1096 cmꢁ1 band. Given
the small observed signal in the most intense fea-
ture of the intermediate spectrum, our failure to
observe this band is not sufficient to disprove our
assignment of the intermediate as Cl3CONO.
partial support by a California State University
Research Fund Grant. Dr. Wade would also like
to thank the Clark Teacher/Scholar Fellowship
for allowing her the opportunity to initiate this
research at SJSU. T. Clemes would like to thank
the Lottery Funds program at SJSU for partial
financial support. K. Reak would like to thank
the Mills College Women’s Studies Program for
financial support. Prof. C.B. Moore and Stacie
Cowan provided many helpful discussions which
led directly to this work. The equipment used in
this work was funded through grants from NSF,
Research Corporation, the William M. Keck
Foundation, and San Jose State University.
5. Conclusion
References
Chloropicrin undergoes photolysis to produce
phosgene and nitrosyl chloride in cryogenic ma-
trices. These products are observed at a wide range
of photolysis wavelengths, and whether or not
oxygen is present. Furthermore, when 18O2 is
present, 18O-labeled photoproducts are not ob-
served in cryogenic matrices.
Based on these observations, the following
mechanism is proposed. Chloropicrin initially un-
dergoes cleavage of the C–N bond to produce NO2
and CCl3 radicals. In the matrix, these radicals are
kept close to each other, and can recombine to
form Cl3CONO, which itself undergoes photolysis.
CCl3 and NO2 eventually react with each other to
form phosgene and NOCl. It is also possible that
some fraction of the chloropicrin photolyzes to
produce phosgene and NOCl directly.
This mechanism would be consistent with
many, but not all, of the previous gas phase ex-
periments [10,11,13]. In particular, we have ob-
served that chloropicrin will dissociate in the
absence of oxygen in cryogenic matrices, contrary
to what was reported by Moilanen et al. [13].
Further, gas-phase studies will be required to
completely explain these results and predict the
atmospheric behavior of chloropicrin.
[1] State of California, Department of Pesticide Regulation,
Summary of Pesticide Use Report Data, 1994.
[2] P. Morse, Chem. Eng. News 76 (1998), Oct 26 (*look up p.
#).
[3] M. Leistra, S.J.H. Crum, Water, Air, Soil Pollut. 50 (1990)
109.
[4] P. Howard, Handbook of Environmental Fate and Expo-
sure Data for Organic Chemistry 3 (1990) 126.
[5] J. Heicklen, Atmos. Environ. 16 (1982) 821.
[6] J.H. Seinfeld, Atmospheric Chemistry and Physics of Air
Pollution, Wiley, New York, 1986.
[7] R. Atkinson, Atmos. Environ. 24A (1990) 1.
[8] R. Atkinson, J. Phys. Chem. Ref. Data, Monograph 2
(1994).
[9] R. Atkinson, W.P.L. Carter, Chem. Rec. 1984 (1984)
437.
[10] W.P.L. Carter, D. Luo, I.L. Malkina, Atmos. Eviron. 31
(1997) 1425.
[11] T.D. Allston, M.L. Fedyk, G.A. Takacs, Chem. Phys. Lett.
60 (1978) 100.
[12] N.S. Bayliss, E.G. McRae, J. Phys. Chem. 58 (1954)
1006.
[13] K.W. Moilanen, D.G. Crosby, J.R. Humphrey, J.W. Giles,
Tetrahedron 34 (1978) 3345.
[14] K. Honda, H. Mikuni, M. Takahasi, M. Bull. Chem. Soc.
Japan 45 (1972) 3534.
[15] S.J. Paszyc, Photochemistry 2 (1973) 183.
[16] W.D. Taylor, T.D. Allston, M.J. Moscato, G.B. Fazekas,
R. Kozlowski, G.A. Takacs, Int. J. Chem. Kinet. 12 (1980)
231.
[17] E. Catalano, K.S. Pitzer, J. Am. Chem. Soc. 80 (1958)
1054.
Acknowledgements
[18] D.E. Tevault, R.R. Smardzewski, J. Phys. Chem. 82 (1978)
375.
We gratefully acknowledge partial support
from the Petroleum Research Fund, as well as
[19] M.E. Jacox, J. Phys. Chem. 88 (1984) 3373.
[20] H.W. Brown, G.C. Pimentel, J. Chem. Phys. 29 (1958) 883.