cm- NO was added to the chamber, and the reactant
3
to suppress the formation of O
3
and hence of NO
3
radicals
(
29). Because HCHO is the major product from the photolysis
mixtures monitored for 60 min. Because 1,3-butadiene reacts
of methyl nitrite in air, HCHO formation yields from the
reaction of the OH radical with 1,3-butadiene were measured
in experiments using ethyl nitrite photolysis as the source of
OH radicals (30).
slowly with NO
carried out to investigate this reaction by FT-IR spectroscopy
2
in the dark (20), an experiment was also
with initial concentrations of NO
2
and 1,3-butadiene of 1.8
1
4
14
-3
× 10 and 2.46 × 10 molecule cm , respectively.
Teflon Cham ber with Analysis by API-MS. In the experi-
ments with API-MS analyses, the chamber contents were
sampled through a 25 mm diameter × 75 cm length Pyrex
NO
tion of N
3
radicals were generated by the thermal decomposi-
in the presence of NO (31, 32):
2
O
5
2
-
1
N O f NO + NO
2
(4)
tube at ∼20 L min directly into the API mass spectrometer
source. The operation of the API-MS in the MS (scanning)
and MS/ MS [with collision activated dissociation (CAD)]
modes has been described elsewhere (35). Use of the MS/
MS mode with CAD allows the “daughter ion” or “parent
ion” spectrum of a given ion peak observed in the MS
scanning mode to be obtained (35). The positive ion mode
2
5
3
Teflon Cham ber Experim ents with GC-FID and GC-
MS Analysis. For the OH radical reactions carried out in the
7
500-L Teflon chamber (at ∼5% relative humidity), OH
radicals were generated by the photolysis of methyl nitrite
in air, and the initial reactant concentrations (in molecule
cm units) were as follows: CH
-
3
14
was used in these API-MS and API-MS/ MS analyses with
protonated water hydrates (H
3
ONO, 2.0 × 10 ; NO, 1.9 ×
+
1
4
13
3
O (H
2
O)
n
) generated by the
1
0 ; and 1,3-butadiene, (5.7-6.2) × 10 . Irradiations were
corona discharge in the chamber diluent gas being respon-
sible for the protonation of analytes. Ions are drawn by an
electric potential from the ion source through the sampling
orifice into the mass-analyzing first or third quadrupole. For
these experiments, the API-MS instrument was operated
under conditions that favored the formation of dimer ions
in the ion source region (35). Neutral molecules and particles
are prevented from entering the orifice by a flow of high-
purity nitrogen (curtain gas), and as a result of the declustering
action of the curtain gas on the hydrated ions, the ions that
are mass-analyzed are mainly protonated molecular ions
carried out at 20% of the maximum light intensity for 2-7
min, resulting in up to 53% reaction of the initial 1,3-
butadiene. The concentrations of 1,3-butadiene and selected
products were measured during the experiments by GC-FID.
The concentrations of 1,3-butadiene were measured as
described previously (33). For the analyses of reaction
3
products, gas samples of 100 cm volume were collected from
the chamber onto Tenax-TA solid adsorbent with subsequent
thermal desorption at ∼225 °C onto a DB-1701 megabore
column in a Hewlett-Packard (HP) 5710 GC, initially held at
-
40 °C and then temperature programmed to 200 °C at 8 °C
+
-
1
([M + H] ) and their protonated homo- and heterodimers
min . In addition, an Entech 7000 preconcentrator (Entech
Instruments, Inc.) with a cold trap dehydration method was
used to transfer gas samples collected from the chamber
onto Tenax-TA solid adsorbent to a 30-m DB-1701 fused
silica capillary column in an HP 5890 GC interfaced to a HP
(
35).
For the OH radical reactions, the initial concentrations of
ONO, NO, and 1,3-butadiene (or 1,3-butadiene-d ) were
4.8 ×10 molecule cm each, and irradiations were carried
out for 2 min at 20% of the maximum light intensity. For the
NO radical reactions, the initial 1,3-butadiene (or 1,3-
butadiene-d
CH
∼
3
6
1
3
-3
5
971A mass selective detector operating in the scanning mode
3
for GC-MS analyses. GC-FID response factors were deter-
mined as previously described (34).
1
3
6
-
) and NO
2
concentrations were ∼4.8 × 10
molecule cm each, and one addition of N (corresponding
to an initial concentration of N in the chamber of (2.2-
3
2
O
5
For the NO
by the thermal decomposition of N
3
radical reactions, NO
3
radicals were generated
, and the initial 1,3-
2
O
5
2
O
5
1
3
-3
1
3
3.9) × 10 molecule cm ) was made to the chamber during
butadiene and NO
2
concentrations were (5.7-6.0) × 10 and
1
3
-3
the experiment.
∼
4.8 × 10 molecule cm , respectively. Three additions of
Chem icals. The chemicals used and their stated purities
were as follows: acrolein (99+%), Aldrich Chemical Co.; 1,3-
N
2
O [corresponding to initial concentrations of N O in the
5
2
5
1
3
-3
chamber of (0.82-1.32) × 10 molecule cm ] were made
to the chamber during an experiment. The concentrations
of 1,3-butadiene and selected products were measured as
described above.
butadiene (g99.0%), NO (g99.0%), and NO
Matheson Gas Products; and 1,3-butadiene-d (98%), Cam-
bridge Isotope Laboratories. Methyl nitrite, ethyl nitrite, and
were prepared and stored as described previously (29,
1, 34).
2
(g99.5%),
6
2 5
N O
3
Evacuable Cham ber Experim ents with FT-IR Analysis.
Four OH radical reactions were carried out in the 5870-L
evacuable, Teflon-coated chamber; two irradiations of CH
ONO-NO-1,3-butadiene-air mixtures and two irradiations
of C ONO-NO-1,3-butadiene-air mixtures at 740 Torr
total pressure and a relative humidity of <1%. The initial
3
-
Results
2
H
5
Gas Chrom atographic Analyses. GC-MS and GC-FID analy-
ses showed the formation of acrolein [CH
both the OH and NO
Because acrolein also reacts with the OH radical, the
measured acrolein concentrations in the OH radical-initiated
reactions were corrected to take into account secondary
reactions with the OH radical as described previously (36),
using rate constants for the reactions of the OH radical with
2
dCHCHO] from
3
radical reactions of 1,3-butadiene.
1
4
concentrations of the reactants were 2.46 × 10 molecule
-
3
cm each. The irradiations were carried out intermittently
with illumination periods of 0.5-1.25 min and total irradiation
times of 5-6.5 min. IR spectra were recorded prior to the
start of photolysis and during the intervening dark periods.
Each spectrum was recorded with 64 scans (corresponding
to 2.0-min averaging time), a full-width-at-half-maximum
-
11
1,3-butadiene and acrolein at 298 K of 6.66 × 10 and 1.99
-
1
-11
3
-1 -1
resolution of 0.7 cm , and a path length of 62.9 m (30, 34).
× 10 cm molecule
s , respectively (20-22). Corrections
In one of the CH
3
ONO-NO-1,3-butadiene-air irradiations,
for secondary reactions of acrolein with the OH radical during
1
4
-3
4
.9 × 10 molecule cm NO was added at the end of
the OH radical reactions were <14%. Corrections for the
irradiation and monitored in the dark by FT-IR spectroscopy
for 35 min.
secondary reaction of acrolein with the NO
the NO
formation yields obtained from the OH and NO
3
3
radical during
radical reactions were negligible (<1%). The acrolein
radical-
3
Two NO
3
radical experiments were performed by adding
1
3
13
-3
N
2
O
5
, in aliquots of 2.46 × 10 or 4.92 × 10 molecule cm
initiated reactions by least-squares analyses of the data
obtained are given in Table 1.
Analyses by FT-IR Spectroscopy. Reaction with the OH
Radical. The major products observed during the photolyses
1
4
-3
to 2.46 × 10 molecule cm 1,3-butadiene in 740 Torr total
pressure of air and by monitoring the reactants and products
by FT-IR spectroscopy after each N
of each of these two experiments, (2.5-7.4) × 10 molecule
2 5
O addition. At the end
1
4
of CH
3
2 5
ONO-NO-1,3-butadiene-air and C H ONO-NO-
VOL. 33, NO. 20, 1999 / ENVIRONMENTAL SCIENCE & TECHNOLOGY
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