of catechol.14 Generally, catechol formation can be described
starting from the OH/phenol adduct (ortho-position) assum-
ing H-abstraction by O2 :13
zoquinone) were obtained by flushing out the gas phase over
the solid sample by the carrier gas over a time period of 1.5–
23 h. During this period, FT-IR spectra of the resulting gas
mixture were measured in different intervals and in the end
of that the mass differences of the solid sample was deter-
mined. Under conditions of nearly constant sublimation in
the whole time period (Dm/m is small, surface of the solid
stays nearly unchanged, constant temperature), from the
mass difference and the total volume of the gas stream an
averaged concentration of the sublimated substance can be
calculated setting the FT-IR spectra on an absolute scale.
Using this approach, the reproducibility of the results was
found to be reasonable and determined absorption cross sec-
tions for the strongest absorption bands were (base 10, unit:
10ꢂ19 cm2 moleculeꢂ1); catechol: 4.0 ꢀ 0.3 at 1273 cmꢂ1, o-
nitrophenol: 3.9 ꢀ 0.4 at 1342 cmꢂ1 and p-benzoquinone:
9.1 ꢀ 3.2 at 1680 cmꢂ1. Error limits represent two standard
deviations. Because of too low sublimation vapour pressure,
for p-nitrophenol this procedure did not work. Appropriate
cross sections given in the literature13 were measured with
an instrumental resolution of 1 cmꢂ1 making an reasonable
comparison with the data of this study (instrumental resolu-
tion: 8 cmꢂ1) impossible.
For on-line GC-MS analysis (HP 5890 with HP MSD 5971),
a smaller part of the gas stream was pumped continuously
through a GC loop connected with the flow tube by means
of a heated transfer line. For product separation, a 30 m,
0.25 mm id column (HP 5MS) was chosen. Using the corre-
sponding ion traces, o-nitrophenol (m/z ¼ 139 u) and p-ben-
zoquinone (m/z ¼ 108 u) were detected efficiently allowing
the analysis of both substances down to flow-tube concentra-
tions of approximately 1010 molecule cmꢂ3. For signal calibra-
tion, GC-MS chromatograms and FT-IR spectra from the
same sample were measured simultaneously using the deter-
mined concentration from the FT-IR measurement as the
reference value (see the paragraph above). Because of probably
effective wall loss in the sampling device, the determination of
catechol was not successful using this GC method. Also for
the GC-MS analysis of o-nitrophenol and p-benzoquinone,
wall processes affecting the determined concentrations under
reaction conditions (presence of NOx) can not fully be ruled
out.
ð3aÞ
The formation of o-nitrophenol is attributed to the reaction of
phenoxy radicals with NO2 .7
ð7aÞ
Note that the given pathway represents an overall reaction
only. At least an intramolecular H-atom transfer step is needed
to produce a phenol-type substance starting from phenoxy
radicals.
The aim of the present study was to determine the products
of the reaction of OH radicals with phenol in dependence on
gas composition (O2 , NO and NO2 concentration) and tem-
perature. The experimental finding that k1 , kꢂ1 , k2 and k3
are pressure independent above 30–50 mbar (Ar as dilution
gas)10 justifies the use of a total pressure of 100 mbar and
allows the application of the results to atmospheric pressure.
The measurement of newly formed particles should clarify
the possible formation of condensable substances not detect-
able in the gas phase. From the sum of all experimental find-
ings under different conditions more insight into the
mechanism of the reaction of OH radicals with phenol is
expected. Additionally, for the evaluation of a possible com-
peting process under the applied reaction conditions, the rate
constant for the reaction of H-atoms with phenol was
measured.
Experimental
Furthermore, few runs were performed with particle mea-
surements or with cryo-trapping of the reaction products.
For particle measurements, a modified CPC (condensation
particle counter, TSI 7610) was used operating with FC 43
(perfluorotributylamine) as working fluid.15 The CPC was
directly attached to the flow tube approximately 45 cm down-
stream the mixing point of the reactants resulting in a resi-
The experiments were carried out at a pressure of 100 mbar
in a quartz glass flow tube (4.0 cm id, total length: 100 cm)
surrounded with a thermo-jacket allowing operation in the
temperature range of 266–364 K. In the presence of sufficient
O2 in the reaction gas ([O2] ¼ 1.68 ꢁ 1018 molecule cmꢂ3
)
OH radicals were produced via the reaction sequence:.
dence time of 0.63
s before particle counting. Before
H þ O2 þ M ! HO2 þ M
HO2 þ NO ! OH þ NO2
In these experiments NO additions were in the range (9.8–
ð9Þ
ð10Þ
measurements, the counting efficiency of the CPC at 100 mbar
was determined using an aerosol electrometer in a low-pressure
calibration set-up.16,17 For cryo-trapping, for a time period of
1 h the whole gas stream was pumped through a gas trap held
at liquid argon temperature. After disconnecting the trap from
the flow tube, the frozen material was immediately dissolved in
methanol and analysed by GC-MS (HP 6890 with HP MSD
5973). For product separation, an identical column as used
for the on-line GC-MS analysis was chosen.
244) ꢁ 1012 molecule cmꢂ3. In the absence of O2 ([O2] < 2 ꢁ
1013 molecule cmꢂ3, [NO2] ¼ (1.8–17.2) ꢁ 1013 molecule cmꢂ3
OH radicals were produced via:
)
H þ NO2 ! OH þ NO
ð11Þ
Approximately 50 cm downstream of the point for the
entrance of phenol and the additions diluted in the carrier
gas, in a side-arm H-atoms were generated in a commercial
microwave discharge (SAIREM GMP 03 K/SM) using a mix-
ture of 0.012–0.023 vol% H2 in He.
The main part of the reaction gas was pumped continu-
ously through a White cell (volume: 2050 cm3, optical path
length: 10 m) for FT-IR analysis (Nicolet Magna 750) using
an instrumental resolution of 8 cmꢂ1 averaging 200–2000
scans. At 100 mbar and 295 K, calibrated reference spectra
of the reaction products (catechol, o-nitrophenol and p-ben-
For the metering of phenol into the flow tube the same
approach was used as described for the signal calibration of
the reaction products. The resulting phenol concentration in
the tube was permanently controlled by FT-IR measure-
ments. The phenol source was found to be stable over a time
period of days.
The gas flows were set by calibrated mass flow controllers
(MKS 1259) and the pressure in the tube and in the gas cell
was measured using capacitive manometers (Baratron). The
total gas flow was set at 5000 standard cm3 minꢂ1 resulting
in a bulk residence time in the reaction zone of the flow tube
Phys. Chem. Chem. Phys., 2003, 5, 342–350
343