On the heat of formation of carbonyl fluoride, CF2O
J. Chem. Phys. 105, 9781 (1996); doi:10.1063/1.472848
Issue Date: 8 December 1996
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In light of the recent controversy surrounding its heat of formation, CF2O was reexamined by photoionization mass spectrometry. In particular, the CO+ fragment ion yield curve from CF2O was interpreted in terms of a retarded CO++F2 process, and a more facile two-step fragmentation to CO++2F. The former process produces a weak, slowly growing tail region without a clear onset, while the latter occurs at higher energy and causes a pronounced growth with a conspicuous onset, which was found to occur at
20.87+0.03/0.07 eV at 0 K by fitting with a model curve that incorporates ``fluctuations'' associated with second-generation fragments. This onset leads to
H
298(CF2O)
149.1+1.4/0.7 kcal/mol, and indicates that the older experimental values for this quantity are too low by at least 34 kcal/mol. While the F2 elimination is retarded by competition with lower energy processes, the two-step process derives its strength from the FCO+ fragment, which assumes the role of a pseudoparent. Thus, the onset of CO++2F is expected to appear reasonably close to the thermochemical threshold. Such an interpretation indicates that recently calculated ab initio values of 145.3±1.7 kcal/mol and 145.6±1.0 kcal/mol are very likely too high by 34 kcal/mol. In addition, the adiabatic ionization potential of CF2O was refined to 13.024±0.004 eV, while the 0 K appearance potential of the FCO+ fragment was found by fitting to be
14.752±0.005 eV. Together with the suggested value for
H
(CF2O), these two onsets lead to
H
298(CF2O+)=151.2+1.4/0.7 kcal/mol and
H
298(FCO+)=173.5+1.4/0.7 kcal/mol. ©1996 American Institute of Physics.
20.87+0.03/0.07 eV at 0 K by fitting with a model curve that incorporates ``fluctuations'' associated with second-generation fragments. This onset leads to
H
149.1+1.4/0.7 kcal/mol, and indicates that the older experimental values for this quantity are too low by at least 34 kcal/mol. While the F2 elimination is retarded by competition with lower energy processes, the two-step process derives its strength from the FCO+ fragment, which assumes the role of a pseudoparent. Thus, the onset of CO++2F is expected to appear reasonably close to the thermochemical threshold. Such an interpretation indicates that recently calculated ab initio values of 145.3±1.7 kcal/mol and 145.6±1.0 kcal/mol are very likely too high by 34 kcal/mol. In addition, the adiabatic ionization potential of CF2O was refined to 13.024±0.004 eV, while the 0 K appearance potential of the FCO+ fragment was found by fitting to be
14.752±0.005 eV. Together with the suggested value for
H
H
H| History: | Received 19 July 1996; accepted 3 September 1996 |
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KEYWORDS and PACS
ORGANIC FLUORINE COMPOUNDS,
CARBONYL RADICALS,
FORMATION HEAT,
PHOTOIONIZATION,
MASS SPECTROSCOPY,
THERMODYNAMICS,
IONIZATION POTENTIAL,
POTENTIAL ENERGY SURFACES
- 82.60.Cx
Physical Chemistry Chemical thermodynamics Enthalpies of combustion, reaction, and formation - 33.15.Ta
Molecular properties and interactions with photons Properties of molecules and molecular ions Mass spectra - 33.15.Ry
Molecular properties and interactions with photons Properties of molecules and molecular ions Ionization potentials, electron affinities, molecular core binding energy - YEAR: 1996
RELATED DATABASES
PUBLICATION DATA
0021-9606 (print)
1089-7690 (online)
REFERENCES (37)
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- M. W. Chase, C. A. Davies, J. R. Downey, Jr., D. J. Frurip, R. A. Mc-Donald, and A. N. Syverud, JANAF Thermochemical Tables, 3rd ed.;
- J. Phys. Chem. Ref. Data 14, Suppl. 1 (1985).
- J. A. Montgomery, Jr., H. H. Michels, and J. S. Francisco,
Chem. Phys. Lett. 220, 391 (1994 ). - L. A. Curtiss, K. Raghavachari, G. S. Trucks, and J. A. Pople, J. Chem. Phys. 94, 7221 (1991).
- G. A. Petersson, T. G. Tensfeldt, and J. A. Montgomery, Jr., J. Chem. Phys. 94, 6091 (1991).
- W. F. Schneider and T. J. Wallington,
J. Phys. Chem. 98, 7448 (1994 ). - L. A. Curtiss, K. Raghavachari, and J. A. Pople, J. Chem. Phys. 98, 1293 (1993).
- L. Batt and R. Walsh,
Int. J. Chem. Kinet. 14, 933 (1982 ); - W. F. Schneider and T. J. Wallington,
J. Phys. Chem. 97, 12783 (1993 ). - H. von Wartenberg and G. Riteris, Z. Anorg. Chem. 258, 356 (1949).
- O. Ruff and S.-C. Li, Z. Anorg. Chem. 242, 272 (1939).
- D. R. Stull, E. F. Westrum, Jr., and G. C. Sinke, The Chemical Thermodynamics of Organic Compounds (Wiley, New York, 1969), pp. 8086.
- L. V. Gurvich, I. V. Veyts, and C. B. Alcock, Thermodynamic Properties of Individual Substances, Vol. 2, 4th ed. (Hemisphere, New York, 1991).
- J. C. Amphlett, J. R. Dacey, and G. O. Pritchard, J. Phys. Chem. 7, 3024 (1971).
- H. C. Duus, Ind. Eng. Chem. 47, 1447 (1955).
- Termicheskiye Konstanty Veshchestv: Spravochnik, edited by V. P. Glushko (VINITI, Moscow, 19651973).
- L. A. Curtiss and J. A. Pople (private communication).
- J. D. Cox, D.D. Wagman, and V. A. Medvedev, CODATA Key Values for Thermodynamics (Hemisphere, New York, 1989).
- E. Greenberg and W. N. Hubbard,
J. Phys. Chem. 72, 222 (1968 ). - T. J. Buckley, R. D. Johson III, R. E. Huie, Z. Zhang, S. C. Kuo, and R. B. Klemm,
J. Phys. Chem. 99, 4879 (1995 ). - M. W. Farlow, E. H. Man, and C. W. Tullock, Inorg. Syn. 6, 155 (1960).
- P. M. Guyon, W. A Chupka, and J. Berkowitz, J. Chem. Phys. 64, 1419 (1976).
- B. Ruscic and J. Berkowitz, J. Chem. Phys. 98, 2568 (1993).
- C. R. Brundle, M. B. Robin, N. A. Kuebler, and H. Basch,
J. Am. Chem. Soc. 94, 1451 (1972 ). - R. K. Thomas and H. Thompson,
Proc. R. Soc. London Ser. A 327, 13 (1972 ). - S. G. Lias, J. E. Bartmess, J. F. Liebman, J. L. Holmes, R. D. Levin, and W. G. Mallard, J. Phys. Chem. Ref. Data 17, Suppl. 1 (1988).
- C. E. Theodosiou, M. Inokuti, and S. T. Manson, At. Data 35, 473 (1986).
- (a) B. Ruscic and J. Berkowitz,
J. Phys. Chem. 97, 11451 (1993 );
(b) J. Chem. Phys. 100, 4498 (1994); - P. C. Haarhoff,
Mol. Phys. 7, 101 (1963 ). - P. D. Mallinson, D. C. McKean, J. H. Holloway, and I. A. Oxton,
Spectrochim. Acta A 31, 143 (1975 ). - See, for example, G. N. Lewis and M. Randall, Thermodynamics, 2nd ed. (McGraw Hill, New York, 1961).
- K. P. Huber and G. Herzberg, Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules (Van Nostrand, New York, 1979).
- (a) W. Forst, Theory of Unimolecular Reactions (Academic, New York 1973);
- J. M. Dyke, N. Jonathan, A. Morris, and M. J. Winter,
J. Chem. Soc. Faraday Trans 2 77, 667 (1981 ). - J. M. Dyke, N. B. H. Jonathan, A. Morris, and M. J. Winter,
Mol. Phys. 39, 629 (1980 );
J. M. Dyke, - K. A. G. MacNeil and J. C. J. Thynne,
Int. J. Mass Spectrom. Ion Phys. 3, 35 (1969 ). - C. Blondel, P. Cacciani, C. Delsart, and R. Trainham, Phys. Rev. A 40, 3698 (1989).
- S. W. Benson,
J. Phys. Chem. 98, 2216 (1994 ).
(c) 101, 7795 (1994);
(d) 101, 7975 (1994);
(e) 101, 10936 (1994).
(c) M. B. Wallenstein and M. Krauss, J. Chem. Phys. 34, 929 (1961).








