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J. Czarnowski / Journal of Fluorine Chemistry 127 (2006) 736–739
3. Experimental
(16)
The experiments were performed in a grease-free conven-
tional static system allowing pressure measurements at constant
volume and temperature. A spherical quartz bulb with a volume
of 270 cm3 was used as reaction vessel. The pressure was
measured with a quartz spiral gauge. Infrared spectra were
recorded on a Shimadzu IR-435 spectrometer and a Perkin-
Elmer 1600 Series FTIR spectrometer, using 10 cm cells
provided with NaCl and KBr windows, respectively.
CF2BrCFBrOꢀ ! CF2BrCðOÞF þ Brꢀ
CF2BrCFBrOꢀ ! CF2Brꢀ þ CðOÞFBr
(17)
(18)
CF2Brꢀ þ O2 þ M ! CF2BrO2 þ M
(19)
ꢀ
All reactants were purchased commercially. CF3OF (PCR,
97–98%) was washed with 0.1 mol dmꢁ3 NaOH solution and
filtered at 80 K [30]. The CF2CFBr (PCR, 97–98%) contained
CF4, and CF3CF3 as impurities. These impurities are more
volatile than CF2CFBr, but could not be separated by fractional
condensation, distilling together. The CF2CFBr was purified by
intermittent brief evacuation cycles at 153 K, opening and
closing the trap valve. This procedure was repeated several
times until the disappearance of the respective very strong
absorption bands of CF4 [31] and CF3CF3 [32] at 1279 and
1250 cmꢁ1 in the IR spectrum of CF2CFBr. Oxygen (La
Oxigena, 99.99%) was bubbled through 98% analytical-grade
H2SO4, and passed slowly through a Pyrex coil at 153 K.
Fourteen experiments were made in the temperature range
273–218 K. The initial pressure of CF3OF was varied between
0.9 and 2.4 Torr, that of CF2CFBr between 11.5 and 30.7 Torr
and that of O2 between 42.5 and 100.7 Torr.
2CF2BrO2 ! 2CF2BrOꢀ þ O2
(20)
(21)
ꢀ
CF2BrOꢀ ! CðOÞF2 þ Brꢀ
The primary path is the homolytic cleavage of a rather
weak O–F bond in a bimolecular reaction between CF3OF and
CF2CFBr, originating radicals CF3Oꢀ. The radicals CF3Oꢀ
add rapidly to the double bond forming CF3OCF2CFBrꢀ
radical. The lack of formation of CF3OOCF3 confirms that
the addition of CF3Oꢀ to the double bond is faster that any
other reaction of this radical. The values of order
1010 dm3 molꢁ1 sꢁ1 were obtained for the addition of CF3Oꢀ
to the alkenes [22–25].
The radicals CF3OCF2CFBrꢀ react with O2, producing
oxyradicals CF3OCF2CFBrOꢀ through the reacꢀtions (9) and
(10). The equilibrium study of Rꢀ + O2 $ RO2 [26], where
Rꢀ are alkyl radicals, suggests that at the pressure of O2 used
in this work the haloalkyl radicals generated in this reaction
system are almost completely eliminated by O2. It was also
reported [27], that the rate constants for the reactions of
methyl and halomethyl radicals with O2 exceed those for
fluorine-atom abstraction from CF3OF by three to four orders
of magnitude. It indicates that the reaction between radical
CF3OCF2CFBrꢀ and CF3OF to give the corresponding adduct
CF3OCF2CF2Br and CF3Oꢀ can be neglected. The oxyradicals
CF3OCF2CFBrOꢀ decompose eliminating bromine atoms,
which, analogously to the chlorine atoms [4–6,28] add rapidly
to the double bond, initiating the chain reaction and leading to
the formation of radicals CF2BrCFBrOꢀ in presence of O2.
The obtained products point out that the CF3Oꢀ and bromine
atom add to the less bulky CF2 group of the CF2CFBr, which
is consistent with the fact that the steric effects govern the
addition process.
To eliminate the oxygen in excess from the reaction mixture,
the reaction vessel was rapidly cooled down to liquid–air
temperature and O2 evacuated.
Acknowledgments
This work was supported by the Consejo Nacional de
´
´
Investigaciones Cientıficas y Tecnicas, CONICET. The author
thanks Mr. Z. Czarnowski for helpful comments and the Max
Planck Institute for Biophysical Chemistry, Goettingen,
through the Partner Group for Chlorofluorocarbons in the
Atmosphere, for financial support.
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[29].
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The production of CF2BrC(O)F as the main product
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