Atmos. Chem. Phys., 12, 6489–
6504
, 2012
www.atmos-chem-phys.net/12/6489/2012/
doi:10.5194/acp-12-6489-2012
© Author(s) 2012. CC Attribution 3.0 License.
Atmospheric
Chemistry
and Physics
α
-pinene photooxidation under controlled chemical conditions –
Part 1: Gas-phase composition in low- and high-NO
x
environments
N. C. Eddingsaas
1
, C. L. Loza
1
, L. D. Yee
2
, J. H. Seinfeld
1,2
, and P. O. Wennberg
2,3
1
Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, USA
2
Division of Engineering and Applied Science, California Institute of Technology, Pasadena, CA, USA
3
Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA, USA
Correspondence to:
N. C. Eddingsaas (eddingsa@caltech.edu)
Received: 29 December 2011 – Published in Atmos. Chem. Phys. Discuss.: 1 March 2012
Revised: 21 June 2012 – Accepted: 1 July 2012 – Published: 25 July 2012
Abstract.
The OH oxidation of
α
-pinene under both low-
and high-NO
x
environments was studied in the Caltech atmo-
spheric chambers. Ozone was kept low to ensure OH was the
oxidant. The initial
α
-pinene concentration was 20–50 ppb
to ensure that the dominant peroxy radical pathway under
low-NO
x
conditions is reaction with HO
2
, produced from re-
action of OH with H
2
O
2
, and under high-NO
x
conditions,
reactions with NO. Here we present the gas-phase results ob-
served. Under low-NO
x
conditions the main first generation
oxidation products are a number of
α
-pinene hydroxy hy-
droperoxides and pinonaldehyde, accounting for over 40 %
of the yield. In all, 65–75 % of the carbon can be accounted
for in the gas phase; this excludes first-generation products
that enter the particle phase. We suggest that pinonaldehyde
forms from RO
2
+ HO
2
through an alkoxy radical channel
that regenerates OH, a mechanism typically associated with
acyl peroxy radicals, not alkyl peroxy radicals. The OH oxi-
dation and photolysis of
α
-pinene hydroxy hydroperoxides
leads to further production of pinonaldehyde, resulting in
total pinonaldehyde yield from low-NO
x
OH oxidation of
∼
33 %. The low-NO
x
OH oxidation of pinonaldehyde pro-
duces a number of carboxylic acids and peroxyacids known
to be important secondary organic aerosol components. Un-
der high-NO
x
conditions, pinonaldehyde was also found to
be the major first-generation OH oxidation product. The
high-NO
x
OH oxidation of pinonaldehyde did not produce
carboxylic acids and peroxyacids. A number of organoni-
trates and peroxyacyl nitrates are observed and identified
from
α
-pinene and pinonaldehyde.
1 Introduction
The emissions of biogenic volatile organic compounds
(BVOCs) far outnumber those of anthropogenic VOCs
(
Guenther et al.
,
1995
;
Steinbrecher et al.
,
2009
;
Monks
et al.
,
2009
). Excluding methane, BVOCs are estimated to
account for a flux of
∼
1150 Tg C yr
−
1
, while anthropogenic
VOCs account for only
∼
140 Tg C yr
−
1
(
Guenther et al.
,
1995
;
Goldstein and Galbally
,
2007
). Important BVOCs in-
clude isoprene, (flux of
∼
500 Tg C yr
−
1
) and the monoter-
penes (
∼
127 Tg C yr
−
1
) of which
α
-pinene accounts for
∼
50 Tg C yr
−
1
(
Guenther et al.
,
1995
;
Chung and Seinfeld
,
2002
). Because they are unsaturated, these compounds are
highly reactive towards OH, O
3
, and NO
3
and thus play an
important role in tropospheric chemistry. The atmospheric
oxidation of BVOCs also results in the formation of sec-
ondary organic aerosol (SOA). Monoterpenes are significant
sources of SOA due to their large emission rate and high SOA
yield (
Hoffmann et al.
,
1997
;
Pye et al.
,
2010
).
The gas-phase oxidation of simple alkanes and alkenes
is well understood and most tropospheric chemical mecha-
nisms use laboratory studies of reactions of these species to
inform the parameterization of the atmospheric oxidation of
VOCs. Many BVOCs, including isoprene, which has a conju-
gated double bond system, and
α
-pinene which is a bicyclic
hydrocarbon with an endocyclic double bond, however, have
much more complicated chemistry than the simple alkanes
and alkenes. For example, recent experimental and theoret-
ical studies with isoprene have shown that its atmospheric
chemistry is not well modeled by the reactions of simple
Published by Copernicus Publications on behalf of the European Geosciences Union.
6490
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
Table 1.
Experimental conditions.
Date
Hydrocarbon
Concentration
OH Source
Aerosol
Length of
(ppb)
seed
a
experiment (hours)
5 May 2010
α
-pinene
45
H
2
O
2
No seed
12
6 May 2010
α
-pinene
50
HONO
No seed
10
7 May 2010
α
-pinene
48
H
2
O
2
AS
11
9 May 2010
α
-pinene
52
HONO
AS
8
10 May 2010
α
-pinene
47
H
2
O
2
AS+SA
11
11 May 2010
α
-pinene
46
HONO
AS+SA
10
12 May 2010
α
-pinene
20
H
2
O
2
No seed
19
13 May 2010
α
-pinene
42
CH
3
ONO
No seed
8
14 May 2010
α
-pinene
47
H
2
O
2
AS
12
17 May 2010
α
-pinene
48
CH
3
ONO
AS
8
18 May 2010
α
-pinene
47
H
2
O
2
AS+SA
12
19 May 2010
α
-pinene
44
CH
3
ONO
AS+SA
8
2 June 2010
α
-pinene
45
H
2
O
2
AS
12
3 June 2010
α
-pinene
45
CH
3
ONO
AS
8
4 June 2010
Pinonaldehyde
–
b
H
2
O
2
No Seed
9
8 Feb 2011
α
-pinene
43
H
2
O
2
No seed
8
14 Feb 2011
Pinonaldehyde
–
b
H
2
O
2
No seed
9
16 Feb 2011
α
-pinene
31
CH
3
ONO
No seed
3
17 Feb 2011
Pinonaldehyde
–
b
CH
3
ONO
No seed
4
a
AS: ammonium sulfate, AS+SA: ammonium sulfate and sulfuric acid.
b
The initial concentration of pinonaldehyde was not determined.
alkenes, especially under low-NO
x
(NO and NO
2
) condi-
tions (
Paulot et al.
,
2009b
;
Peeters and Muller
,
2010
;
Crounse
et al.
,
2011
).
α
-pinene is a ten-carbon bicyclic hydrocarbon with an en-
docyclic double bond and, therefore, has the potential to re-
act in ways not represented by simple alkenes. In addition,
α
-pinene is highly reactive with both O
3
and OH, reacting in
the atmosphere with
α
-pinene nearly equally, adding to the
richness of its atmospheric photochemistry (
Capouet et al.
,
2008
). Despite a number of studies of OH oxidation of
α
-
pinene, large uncertainties in the identity and yields of its
reaction products remain. For instance, the reported yield of
pinonaldehyde from the photooxidation of
α
-pinene ranges
from 28 to 87 % in the presence of NO
x
and from 3 to
37 % in the absence of NO
x
(
Arey et al.
,
1990
;
Hatakeyama
et al.
,
1991
;
Noziere et al.
,
1999
;
Jaoui and Kamens
,
2001
;
Wisthaler et al.
,
2001
;
Aschmann et al.
,
2002
;
Lee et al.
,
2006
). In addition, the molecular structures of major products
identified by mass (e.g. 184 and 200 daltons) are subject to
debate (
Aschmann et al.
,
2002
;
Vereecken et al.
,
2007
). The
photooxidation product with molecular mass 184 has been
assigned to an unsaturated hydroperoxy carbonyl (
Vereecken
et al.
,
2007
) or a dihydroxy carbonyl (
Aschmann et al.
,
2002
).
A better understanding of
α
-pinene gas-phase chemistry will
increase the accuracy of
α
-pinene atmospheric chemistry
models and provide insight into atmospheric photooxidation
mechanisms in general.
In this study, we isolate the peroxy radical reaction path-
ways to investigate the photochemistry of
α
-pinene. We have
studied these reactions under low-NO
x
conditions similar
to those found in the atmosphere, where RO
2
+ HO
2
is the
dominant peroxy radical reaction, and other reactions are
suppressed (RO
2
+ RO
2
and reactions with O
3
). We contrast
these conditions with results from the gas-phase photoox-
idation of
α
-pinene under high-NO
x
(with varied amounts
of NO
2
to study both RO
2
+ NO and RO
2
+ NO
2
). We fo-
cus our analysis on low-NO
x
rather than high-NO
x
chem-
istry because the low-NO
x
chemistry of
α
-pinene is less well-
characterized yet it is more atmospherically-relevant (
Pye
et al.
,
2010
). In a forthcoming paper, SOA yields and com-
position formed from the controlled chemical conditions de-
scribed here will be presented.
2 Experimental
Photooxidation experiments of
α
-pinene were performed in
the Caltech dual 28 m
3
Teflon chambers. Details of the cham-
ber facilities have been described elsewhere (
Cocker et al.
,
2001
;
Keywood et al.
,
2004
). A few photooxidation experi-
ments were performed in a
∼
1 m
3
bag enclosed in a small,
black walled chamber with UV-lights lining one wall, as de-
scribed by
Crounse et al.
(
2011
). 40 W black lights (Sylvania
F40/350BL) with emission peak emission at 352 nm were
used in both chambers. The light intensity as a function of
wavelength (300–800 nm) was measured using a Licor (LI-
1800) spectroradiometer. Prior to each run, the chamber was
flushed for a minimum of 24 h with dry purified air. While
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
www.atmos-chem-phys.net/12/6489/2012/
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
6491
being flushed, the chamber was irradiated with the chamber
lights for a minimum of six hours. The temperature, relative
humidity (RH), and concentrations of O
3
, and NO
x
(NO and
NO
2
) were continuously monitored. In all experiments the
RH was kept below 10 %. Aerosol size distribution and num-
ber concentration were measured continuously by a differ-
ential mobility analyzer (DMA, TSI model 3081) coupled to
a condensation nucleus counter (TSI model 3760). Informa-
tion on aerosol measurements can be found in part 2, where
aerosol formation, growth, and composition are discussed.
Table
1
shows a list of conditions for all experiments used in
this study. Experiments ran for 3 to 19 h. No gas phase losses
to the chamber walls of either
α
-pinene prior to light irradia-
tion or oxidation products after lights were extinguished was
observed.
Experiments were performed under low- and high-NO
x
conditions. Under low-NO
x
conditions, photolysis of hydro-
gen peroxide (H
2
O
2
) was the OH source, while for the high-
NO
x
experiments the photolysis of nitrous acid (HONO) or
methyl nitrite (CH
3
ONO) produced OH. For low-NO
x
ex-
periments, 280 μL of 50 wt % H
2
O
2
was injected into the
chamber resulting in an H
2
O
2
concentration
∼
4 ppm. The
two different OH sources used during the high-NO
x
experi-
ments provided the mechanism to vary the NO to NO
2
ratio,
with a higher quantity of NO
2
in the CH
3
ONO experiments.
HONO was prepared daily by dropwise addition of 15 mL
of 1 wt % NaNO
2
into 30 mL of 10 wt % H
2
SO
4
in a glass
bulb, and then introduced into the chamber with dry air. This
process produces NO and NO
2
as side products, which are
also introduced to the chamber. CH
3
ONO was synthesized,
purified, and stored according to the procedure outlined by
Taylor et al.
(
1980
). CH
3
ONO was warmed from liquid ni-
trogen temperatures and vaporized into an evacuated 500 mL
glass bulb and introduced into the chamber with an air stream
of 5 L min
−
1
. After addition of CH
3
ONO, 300–400 ppb of
NO was added to the chamber to suppress the formation of
O
3
. Determination of exact NO and NO
2
concentrations us-
ing the commercial NO
x
monitor was precluded due to in-
terferences by both HONO and CH
3
ONO. At the start of all
high-NO
x
experiments the total NO
x
reading (NO, NO
x
, and
interference from HONO or CH
3
ONO) was 800 ppb and NO
concentration throughout the experiments was such that the
concentration of O
3
never exceeded 5 ppb.
α
-pinene was added to the chamber to achieve a concen-
tration of 20–50 ppb by passing dry air through a bulb con-
taining a known volume of
α
-pinene. The mixing ratio of
α
-pinene was monitored by gas chromatography (Agilent
6890N) coupled with a flame ionization detector (GC-FID).
The GC-FID was calibrated using a 55 L Teflon bag contain-
ing a known concentration of pure
α
-pinene. Gas phase pho-
tooxidation products were monitored using triple-quadrupole
chemical ionization mass spectrometry (CIMS) (
St. Clair
et al.
,
2010
).
Details of the operation of the CIMS can be found in
a number of previous reports (
Crounse et al.
,
2006
;
Paulot
et al.
,
2009a
;
St. Clair et al.
,
2010
) and therefore only a brief
description is presented here. The CIMS was operated in neg-
ative ion mode using CF
3
O
−
as the reagent ion, and in the
positive ion mode using H
3
O
+
for proton transfer mass spec-
trometry (PTR-MS). In negative mode, CF
3
O
−
is sensitive to
the detection of polar and acidic compounds by either clus-
tering with the analyte (R) resulting in an ion with a mass-
to-charge ratio (
m/z
) MW+85
(
R
·
CF
3
O
−
)
or via fluorine ion
transfer resulting in
m/z
MW+19
(
HF
·
R
−
−
H
)
. The dominant
ionization mechanism depends mostly on the acidity of the
neutral species; highly acidic species such as nitric acid only
form the fluorine transfer ion, while non-acidic species such
as methyl hydrogen peroxide form only the cluster ion. This
separation aids both in the determination of the structure of
a molecule and in the identification of isomers. In negative
mode, tandem mass spectrometry (MS/MS) was used to help
identify functional groups of an analyte. In brief, a parent ion
selected in the first quadrupole is exposed to an elevated pres-
sure of N
2
resulting in collision-induced dissociation (CID)
in the second quadrupole, and the resulting fragmentation
ions are detected in the third quadrupole. Molecules with dif-
ferent functional groups have been shown to fragment differ-
ently by CID and thus the detection of certain fragment ions
in quadrupole three can aid in the identification of an analyte.
For instance, hydroperoxides form a characteristic fragment
at
m/z
63 (
Paulot et al.
,
2009b
).
Standards are not available for most of the VOCs described
here and thus the sensitivity of the CIMS is related to the
thermal capture rate and the binding energy of the cluster
(
VOC
·
CF
3
O
−
)
. Details on calculating the sensitivity of the
CIMS to a given analyte can be found in previous publica-
tions (
Paulot et al.
,
2009a
,
b
).
3 Results and discussion
The goal of this study is to determine the gas-phase re-
action products and mechanism of the photooxidation of
α
-pinene by OH under both low-NO
x
and high-NO
x
con-
ditions. In both cases, the experiment is designed such
that
α
-pinene only reacts with OH and that a single per-
oxy radical reaction is dominant. Under ambient con-
ditions,
α
-pinene reacts at an approximately equal rate
with O
3
(
k
O
3
=
9
.
0
×
10
−
17
cm
3
molecules
−
1
s
−
1
)
and OH
(
k
OH
=
5
.
3
×
10
−
11
cm
3
molecules
−
1
s
−
1
)
(
Sander et al.
,
2006
;
Atkinson et al.
,
2006
). To isolate the OH chemistry,
the formation of O
3
was suppressed.
Under low-NO
x
conditions, photolysis of H
2
O
2
resulted in
steady state OH concentration of
∼
2
×
10
6
cm
−
3
and an HO
2
concentration
∼
1
×
10
10
cm
−
3
. The OH and HO
2
concentra-
tions were determined from a kinetic molecular model of
α
-
pinene OH reaction which is described in detail in Sect. 3.2
and in the Supplement. In brief, OH is produced by the pho-
tolysis of H
2
O
2
and is primarily consumed by reactions with
VOCs in the chamber and with H
2
O
2
. The reaction of OH
www.atmos-chem-phys.net/12/6489/2012/
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
6492
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
O
H
O
O
O
O
H
O
O
P
i
n
o
n
a
l
d
e
h
y
d
e
m
/
z
=
(
+
)
1
6
9
~
2
0
%
y
i
e
l
d
O
H
,
O
2
,
H
O
2
O
O
H
O
H
O
H
O
-
O
2
,
-
O
H
-
H
O
2
O
H
O
O
H
α
-
p
i
n
e
n
e
h
y
d
r
o
p
e
r
o
x
i
d
e
H
O
2
O
O
O
H
5
%
y
i
e
l
d
H
O
2
O
H
,
O
2
O
2
O
H
O
O
H
I
s
o
m
.
R
i
n
g
C
l
o
s
u
r
e
3
%
y
i
e
l
d
O
α
-
p
i
n
e
n
e
o
x
i
d
e
m
/
z
=
(
+
)
1
5
3
,
1
7
1
O
O
H
O
H
O
H
O
H
O
2
-
H
2
O
α
-
p
i
n
e
n
e
h
y
d
r
o
x
y
h
y
d
r
o
p
e
r
o
x
i
d
e
2
3
%
y
i
e
l
d
α
-
p
i
n
e
n
e
O
O
O
H
O
O
O
H
H
O
2
H
O
2
-
O
2
,
-
O
H
H
O
2
O
O
H
O
2
O
H
,
O
2
,
H
O
2
-
H
O
2
O
O
H
O
H
O
O
H
m/z
= (-) 253, ~6% yield
m/z
= (-) 303
m/z
= (-) 271
m/z
= (-) 271
m/z
= (-) 271
m/z
= (-) 303
m/z
= (-) 269
+O
2
/-HO
2
+O
2
, HO
2
-O
2
Fig. 1.
Pathway of photooxidation of
α
-pinene under low-NO
x
conditions. Species that were observed are labeled in red. The
m/z
of all
species observed in the negative mode are of the complex with CF
3
O
−
(molecular mass + 85). Pinonaldehyde is observed at molecular mass
+ 1 in the positive mode and
α
-pinene oxide is observed at molecular mass + 1 and + 19. The observed percent yield for first-generation
products is also indicated.
and H
2
O
2
produces HO
2
. The photolysis rate of H
2
O
2
used
in the model and the OH concentration determined by the
model were confirmed by comparison of the gas-phase con-
centrations of H
2
O
2
and
α
-pinene from the experiment and
the model (Fig. S1). These OH concentrations are similar to
those observed in the troposphere; however, the HO
2
concen-
trations are about an order of magnitude greater than levels
typically observed in rural or remote areas (
Lelieveld et al.
,
2008
;
Ren et al.
,
2008
;
Wolfe et al.
,
2011
). The O
3
concen-
tration at the start of each experiment was
<
4 ppb and typi-
cally did not exceed 12 ppb over the course of an experiment
(in one experiment, conducted for 20 h, the O
3
concentra-
tion increased nearly linearly from 4 to 25 ppb). Modeling of
these oxidant concentrations indicated that reaction with O
3
accounted for
<
3 % of the
α
-pinene loss.
In the oxidation of
α
-pinene by OH, OH adds predomi-
nantly to the endocyclic double bond, followed by addition
of O
2
to the resulting
β
-hydroxy alkyl radicals producing a
number of hydroxy peroxy radicals. OH abstraction of a hy-
drogen from
α
-pinene occurs with a yield of
∼
12 %, result-
ing in a peroxy radical when O
2
reacts with the alkyl rad-
ical (
Capouet et al.
,
2004
). Under low-NO
x
conditions the
peroxy radicals can react with either HO
2
or with another
RO
2
(self or cross-reactions). Here we seek to emulate atmo-
spheric conditions where RO
2
+ HO
2
dominates. To confirm
that the RO
2
+ HO
2
pathway dominated in our experiments, a
kinetic model was constructed, as described in Sect. 3.2 and
the Supplement. For the experimental conditions (with initial
concentration of
α
-pinene of 20–50 ppb), the kinetic model
indicates that less than 1 % of the peroxy radical reactions
proceed via RO
2
+ RO
2
.
For high-NO
x
photooxidation experiments, OH is gener-
ated from the photolysis of either HONO or methyl nitrite.
When HONO is synthesized, NO and NO
2
are produced as
side products, which are also introduced to the chamber when
HONO is injected. Methyl nitrite is synthesized pure and
upon photolysis eventually produces OH and NO
2
:
CH
3
ONO
+
hν
→
CH
3
O
q
+
NO
(R1)
CH
3
O
q
+
O
2
→
CH
2
O
+
HO
q
2
(R2)
HO
q
2
+
NO
→
OH
q
+
NO
2
(R3)
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
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N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
6493
O
H
,
O
2
O
O
O
O
H
O
2
O
O
O
H
O
O
O
O
H
O
O
O
H
O
2
H
O
2
-
O
3
O
O
H
O
O
2
H
O
2
-
O
H
,
-
C
O
2
O
O
Pinonic peroxyacid
m/z
= (-) 285, 265, 219
H-abstraction could produce
pinonic hydroperoxide (
m/z
(-) 285)
Pinonic acid
m/z
= (-) 203, 269
Pinonaldehyde
m/z
= (+) 169
Norpinonaldehyde
m/z
= (+) 155
m/z
= (-) 257
Fig. 2.
Pathway of photooxidation of pinonaldehyde under low-NO
x
conditions. Species that were observed are labeled in red. Pinonic acid
and pinonic peracid were observed in the negative mode as both the transfer ion (molecular mass + 19) and the complex (molecular mass
+ 85), pinonic peracid is also observed as the complex minus HF (molecular mass + 65), norpinonaldehyde hydroperoxide was observed as
the complex ion, pinonaldehyde and norpinonaldehyde are observed in the positive mode at their molecular mass +1.
When methyl nitrite was used as the OH source, 300 to
400 ppb of NO was added to suppress O
3
production. Un-
der the conditions used, the peroxy radicals formed from the
OH reaction of
α
-pinene react with NO and not RO
2
or HO
2
.
This is confirmed by the lack of RO
2
+ HO
2
or RO
2
+ RO
2
reaction products during high-NO
x
photooxidation. The ex-
act ratio of NO to NO
2
is not known as both HONO and
methyl nitrite interfere with the signals from the chemilumi-
nescence NO
x
instrument; however, it was determined that a
higher NO
2
concentration exists during methyl nitrite pho-
tolysis due to the increased production of peroxyacyl nitrates
(PANs), as detected by CIMS in the negative mode, which
result from the RO
2
+ NO
2
reaction. More details on the de-
tection of, as well as the specific PANs detected will be dis-
cussed in Sect. 3.3.
3.1 Gas phase composition from low-NO
x
photooxidation of
α
-pinene
The principal first-generation oxidation products observed
from the low-NO
x
photooxidation of
α
-pinene were a num-
ber of
α
-pinene hydroxy hydroperoxides and pinonaldehyde.
Production of
α
-pinene hydroperoxide from H-abstraction
and
α
-pinene oxide are also observed (see Fig.
1
for proposed
reaction mechanism for
α
-pinene and Fig.
2
for pinonalde-
hyde). The time traces from the CIMS are shown in Fig.
3
along with those from a number of the minor oxidation prod-
ucts. The identification of each of these signals is discussed
below.
The
α
-pinene hydroxy hydroperoxides are observed at
m/z
(
−
)271 (molecular weight + CF
3
O
−
) by the CIMS. They
are expected to be a major products of the reaction channel of
RO
2
+ HO
2
. Three different
α
-pinene hydroxy hydroperox-
ide isomers are formed; two
β
-hydroxy hydroperoxides and
one ring opened hydroxy hydroperoxide containing a double
bond (see Fig.
1
). The subsequent reaction pathways of these
three
α
-pinene hydroxy hydroperoxides are expected to be
different and will lead to distinct reaction products, as dis-
cussed in Sect. 3.2. The overall estimated initial yield of the
α
-pinene hydroxy hydroperoxides is
∼
23 %. This estimate
accounts for the small yield of pinic acid, which has the same
molecular weight as these peroxides (MW
=
186). Similar to
other carboxylic acids, ionization of pinic acid by CF
3
O
−
yields approximately equal amounts of signal at
m/z
(
−
)271
and 205 (MW
−
H
+ HF). This allows us to use the signal at
m/z
(
−
)205 to insure that the pinic acid concentration does
not significantly impact the hydroperoxide yield estimate.
Pinonaldehyde is neither acidic nor is the complex with
CF
3
O
−
significantly strong to be detected in the negative
mode and thus is observed only in the positive mode of the
CIMS. Pinonaldehyde was synthesized to directly observe
its OH oxidation; however, the synthesized sample was not
of sufficient purity to calibrate the CIMS response. While
we cannot report an absolute yield for pinonaldehyde, we
observe that the yield under low-NO
x
conditions is 2/3 of
that under high-NO
x
conditions. As pinonaldehyde is one
of the main products of
α
-pinene oxidation by any atmo-
spheric oxidant, it has been widely studied. Although the
reported yield of pinonaldehyde under high-NO
x
conditions
varies widely from 27–87 % (
Arey et al.
,
1990
;
Hatakeyama
et al.
,
1991
;
Noziere et al.
,
1999
;
Wisthaler et al.
,
2001
;
Jaoui
and Kamens
,
2001
;
Aschmann et al.
,
2002
;
Lee et al.
,
2006
),
www.atmos-chem-phys.net/12/6489/2012/
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
6494
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
0
2
4
6
8
1
0
1
2
1
4
1
6
0
0
.
5
1
.
0
1
.
5
2
.
0
2
.
5
3
.
0
C
I
M
S
s
i
g
n
a
l
(
a
u
)
1
8
A
0
2
4
6
8
1
0
1
2
1
4
1
6
1
8
0
0
.
2
0
.
4
0
.
6
0
.
8
T
i
m
e
(
h
o
u
r
s
)
B
C
I
M
S
s
i
g
n
a
l
(
a
u
)
Fig. 3.
CIMS time traces of a number of important low-NO
x
photooxidation products of
α
-pinene.
(A
) Main first generation
products,
m/z
(
−
)271
α
-pinene hydroxy hydroperoxide (black),
m/z
(+)169 pinonaldehyde (red),
m/z
(
−
)253
α
-pinene hydroperox-
ide (blue)
(B)
Signals of species that are formed in multiple gener-
ations
m/z
(
−
)285 (black),
m/z
(
−
)269 (red),
m/z
(
−
)303 (green),
m/z
(
−
)301 (orange), and purely second-generation
m/z
(
−
)203
pinonic acid (blue). The signal from
m/z
(+)169 is the only signal
shown from the positive mode and the intensity was divided by 2
for clarity.
most of the measured yields are between 27–35 %. The very
high yields were measured by FTIR which may be biased
by interference from other carbonyls (
Noziere et al.
,
1999
;
Hatakeyama et al.
,
1991
). Assuming that under high-NO
x
conditions the pinonaldehyde yield is between 27–35 %, we
estimate that the low-NO
x
yield is about 20 %.
Pinonaldehyde has been observed from the low-NO
x
pho-
tooxidation of
α
-pinene previously; however, it is typically
assigned as a product of RO
2
+ RO
2
chemistry (
Noziere
et al.
,
1999
;
Larsen et al.
,
2001
). In the present set of ex-
periments, the chemistry is overwhelmingly dominated by
RO
2
+ HO
2
(i.e. low
α
-pinene concentration and relatively
high HO
2
concentration). This is confirmed by the photoox-
idation products observed. The two main reaction channels
for alkyl peroxy radicals with other RO
2
are:
RO
q
2
+
RO
′
q
2
→
R=O
+
R
′
OH
+
O
2
(R4)
RO
q
2
+
RO
′
q
2
→
RO
q
+
RO
′
q
+
O
2
(R5)
resulting in the formation of alcohols and carbonyls from
Reaction (R4) and alkoxy radicals from Reaction (R5). In
the case of
α
-pinene, these would be
β
-diols,
β
-hydroxy
carbonyl, and hydroxy alkoxy radicals. The six membered
ring of the hydroxy alkoxy radical will then open forming
pinonaldehyde. There is no indication of either
β
-diols or
β
-hydroxyl carbonyl being formed during the present experi-
ments. In the case of alkyl peroxy radicals reacting with HO
2
,
the main reaction channel is:
RO
q
2
+
HO
q
2
→
ROOH
+
O
2
(R6)
which forms hydroperoxides. For
α
-pinene, Reaction (R6)
will produce the observed
α
-pinene hydroxy hydroperoxides.
For many small alkyl peroxy radicals it has been shown to be
the only channel (
Hasson et al.
,
2004
;
Raventos-Duran et al.
,
2007
;
Noell et al.
,
2010
).
If Reaction (R6) was the only channel, there would be
no route to pinonaldehyde production. One possible route to
pinonaldehyde is a radical channel (see Fig.
1
):
RO
q
2
+
HO
q
2
→
RO
q
+
O
2
+
OH
q
(R7)
similar to those known to be important for acetyl peroxy rad-
icals (
Hasson et al.
,
2004
;
Dillon and Crowley
,
2008
) and
possibly for the reaction of OH with toluene (
Birdsall et al.
,
2010
). If this is the route to pinonaldehyde formation, an OH
recycling channel would also be of importance in the reaction
of OH with
α
-pinene under low-NO
x
conditions.
α
-pinene hydroperoxide and
α
-pinene oxide are also ob-
served products of the OH oxidation of
α
-pinene under
low-NO
x
conditions.
α
-pinene hydroperoxide can be formed
from H-abstraction by OH, which is estimated to account for
about 12 % of the OH reaction with
α
-pinene (
Capouet et al.
,
2004
). Assuming similar CIMS sensitivity to
α
-pinene hy-
droperoxide and
α
-pinene hydroxy hydroperoxide, the yield
of
α
-pinene hydroperoxide is estimated to be
∼
6 %. The re-
mainder of the H-abstraction branching ratio cannot be ac-
counted for at this time.
α
-pinene oxide is neither acidic nor
is the complex with CF
3
O
−
significantly strong to be de-
tected in the negative mode and thus is observed only in the
positive mode at
m/z
(
+
)153 and 171 as confirmed by di-
rect injection of
α
-pinene oxide into the chamber. Further
evidence of
α
-pinene oxide formation is presented in part 2
of this series of paper where SOA composition is discussed.
α
-pinene oxide appears to be a minor product, and the mech-
anism for its formation by OH oxidation is not known. The
mechanism for the formation from O
3
oxidation is known
and yields of a few percent have been reported (
Alvarado
et al.
,
1998
;
Berndt et al.
,
2003
); however, in the present ex-
periments O
3
accounts for less than 3 % of the oxidation of
α
-pinene.
The oxidation products of pinonaldehyde have been shown
to be important in the formation of SOA from the pho-
tooxidation of
α
-pinene. Specifically, pinonic acid, 10-
hydroxypinonic acid, and pinic acid have been observed
in ambient SOA samples (
Kavouras et al.
,
1998
,
1999
;
Yu
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
www.atmos-chem-phys.net/12/6489/2012/
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
6495
et al.
,
1999
;
Laaksonen et al.
,
2008
;
Zhang et al.
,
2010
)
and in laboratory studies of
α
-pinene photooxidation (
Larsen
et al.
,
2001
;
Jaoui and Kamens
,
2001
;
Librando and Tringali
,
2005
). The low-NO
x
photooxidation of pinonaldehyde was
carried out to determine the contribution of pinonaldehyde
oxidation products to the gas and particle phases of
α
-pinene
photooxidation.
Photooxidation of pinonaldehyde accounts for a number
of the products observed from
α
-pinene photooxidation. OH
oxidation of pinonaldehyde occurs by H-abstraction, typi-
cally from the aldehydic group (59–86 %) (
Kwok and Atkin-
son
,
1995
;
Vereecken and Peeters
,
2002
) forming an acyl per-
oxy radical after the addition of O
2
. The reaction of HO
2
with an acyl peroxy radical produces carboxylic acids, per-
oxyacids, and acetoxy radicals that will decompose to pro-
duce CO
2
and an alkyl radical.
Hasson et al.
(
2004
) have
shown that these three pathways occur in roughly equal
yields. The reaction pathways and products from pinonalde-
hyde are shown in Fig.
2
. Pinonic acid is observed by the
CIMS mostly by its transfer product ion (ratio of
m/z
(
−
)203
to
m/z
(
−
)269 is
∼
9:1), typical of acidic species, while the
peroxyacid is observed more by its complex ion (ratio of
m/z
(
−
)219 to
m/z
(
−
)285 is
∼
1:4) (Fig.
4
). In addition, we
have observed, using synthesized peracetic acid, that peroxy-
acids are also observed in the negative mode as its molecular
mass +65 (complex with CF
3
O
−
−
HF) at 10–20 % that of
the complex ion (+85). A signal at
m/z
(
−
)265,
∼
10 % the
intensity of
m/z
(
−
)285, has been assigned to pinonic perox-
yacid providing further evidence of its formation. These two
products are formed in roughly equal yields. H-abstraction
at carbons other than the aldehydic carbon could also form
pinonaldehyde hydroperoxide which would also be detected
at
m/z
(
−
)285, as would 10-hydroxy pinonic acid (product
found in SOA). A signal at
m/z
(
−
)257 that has nine carbons
was observed and has been assigned to the hydroperoxide
formed from the alkyl radical formed from the decomposi-
tion of the acetoxy radical. The formation of norpinaldehyde
was also detected. Pinic acid was observed in equal amounts
at
m/z
(
−
)205 and
m/z
(
−
)271, but is a minor product.
Low-NO
x
photooxidation of
α
-pinene also leads to
the pinonaldehyde oxidation products (Fig.
4
). Ions at
m/z
(
−
)203 and (
−
)219 assigned to the transfer ions of
pinonic acid and pinonic peroxyacid are observed to be sec-
ond generation products from
α
-pinene photooxidation, as
would be expected arising from the oxidation of pinonalde-
hyde. The ion at
m/z
(
−
)257 assigned to the C
9
hydroperox-
ide produced from pinonaldehyde photooxidation is also ob-
served to be second generation. Pinonic acid and pinonic per-
oxyacid are also observed as the complex ion at
m/z
(
−
)269
and (
−
)285 respectively. The time traces for
m/z
(
−
)269 and
m/z
(
−
)285 from the photooxidation of
α
-pinene are not
purely from first or second generation products (see Figs.
3 and 4) but a combination of the two. The second genera-
tion products observed as these two ions are pinonic acid and
pinonic peroxyacid, evident from their transfer ions, while
T
i
m
e
s
i
n
c
e
lights on (hours)
0
5
1
0
1
5
0
0
.
2
0
.
4
0
.
6
0
.
8
α
-
p
i
n
e
n
e
C
I
M
S
s
i
g
n
a
l
(
a
u
)
-
1
0
1
2
3
4
5
6
0
0
.
2
0
.
4
0
.
6
p
i
n
o
n
a
l
d
e
h
y
d
e
A
B
C
I
M
S
s
i
g
n
a
l
(
a
u
)
Fig. 4.
Comparison of CIMS signals from low
−
NO
x
photoox-
idation of
(A)
α
-pinene and
(B)
pinonaldehyde;
m/z
(
−
)285
(black),
m/z
(
−
)269 (red),
m/z
(
−
)257 (orange),
m/z
(
−
)219 (blue),
and
m/z
(
−
)203 (green). Pinonaldehyde photooxidation produces
pinonic peroxyacid observed at both
m/z
(
−
)285 and (
−
)219,
pinonic acid observed at both
m/z
(
−
)269 and (
−
)203, and a C
9
hy-
droperoxide observed at
m/z
(
−
)257. The pinonaldehyde photoox-
idation products are observed from
α
-pinene photooxidation along
with additional first-generation signals at
m/z
(
−
)269 and (
−
)285
from first-generation photooxidation products.
the first generation products arise from the photooxidation
of
α
-pinene. Oxidation products of these molecular mass
(184 and 200) have been observed and theoretically proposed
from the photooxidation of
α
-pinene in the presence of NO
(
Aschmann et al.
,
2002
;
Vereecken et al.
,
2007
). Under high-
NO
x
conditions,
Aschmann et al.
(
2002
) observed molecules
at these masses and assigned them to a dihydroxy carbonyl
and a trihydroxy carbonyl that would be formed by a num-
ber of isomerization steps as well as multiple reactions of
peroxy radicals with NO to form alkoxy radicals.
Vereecken
et al.
(
2007
) indicate that molecules with these molecular
weights could be formed by isomerization reactions after
ring opening, while the molecule with MW
=
200 is pro-
duced from a reaction of NO with the peroxy radical. In both
mechanisms, alkoxy radicals are essential. Alkoxy radicals
appear to form from the reaction of the initially formed
α
-
pinene hydroxy peroxy radical intermediates with HO
2
, and
this is a possible route; however, at this point, the structure
of these molecules is unknown. These are, however, clearly
polyoxygenated species formed from the primary oxidation
www.atmos-chem-phys.net/12/6489/2012/
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
6496
N. C. Eddingsaas et al.:
α
-pinene photooxidation gas-phase composition
of
α
-pinene and their most likely molecular formulas are
C
10
H
16
O
3
and C
10
H
16
O
4
.
Highly oxidized species at
m/z
(
−
)301 and (
−
)303 are also
observed as first generation products (see Fig.
3
). Both sig-
nals decay similarly to the signals at
m/z
(
−
)269 and (
−
)285,
indicating that they are also formed as later generation prod-
ucts. The most likely structure for the first-generation species
at
m/z
(
−
)303 is an
α
-pinene hydroxy hydroperoxide with
a bridging peroxy group that results from the ring closing
channel of the ring opened hydroxy hydroperoxide as shown
in Fig.
1
. This mechanism has been postulated by
Vereecken
et al.
(
2007
). The addition of one hydroxyl group and two hy-
droperoxyl groups decreases the vapor pressure about eight
orders of magnitude making this product a likely aerosol
phase component (
Capouet and M
̈
uller
,
2006
). The photoox-
idation of
α
-pinene hydroperoxide will produce a hydroxy
dihydroperoxide that will also be observed at
m/z
(
−
)303
thus accounting for the slow decay of the signal. We do
not know the structure of the photooxidation product(s) at
m/z
(
−
)301. Given the molecular weight, the structure po-
tentially includes one carbonyl and two hydroperoxyl groups.
Whatever the structure, the vapor pressure will be greatly re-
duced from that of
α
-pinene, once again making it a potential
SOA component.
Another route to the formation of the low vapor pressure
oxidation products at
m/z
(
−
)301 and (
−
)303 is peroxy rad-
ical isomerization. Peroxy radical isomerization has recently
been extensively studied for the isoprene system both theo-
retically (
Peeters et al.
,
2009
;
da Silva et al.
,
2010
;
Nguyen
et al.
,
2010
) as well as experimentally (
Crounse et al.
,
2011
).
It has been shown that peroxy radical isomerization most of-
ten occurs via a six or seven membered intermediate (
Per-
rin et al.
,
1998
;
Blin-Simiand et al.
,
2001
;
Jorand et al.
,
2003
). When OH adds to the tertiary carbon of the double
bond the peroxy radical on the secondary carbon can form
a seven membered ring with the hydrogen of either the sec-
ondary carbon in the four membered ring or one of primary
carbons attached to the four membered ring. After isomer-
ization, reaction with O
2
and HO
2
will result in the forma-
tion of
α
-pinene hydroxy dihydroperoxide which would be
detected at
m/z
(
−
)303. See Fig. S2 in the Supplement for
proposed mechanism. When OH adds to the secondary car-
bon of the double bond, a seven membered intermediate can
form with the other tertiary carbon of the four membered ring
ultimetly forming
α
-pinene hydroxy dihydroperoxide. Sim-
ilarly, the
α
-pinene hydroxy hydroperoxide peroxy radical
formed from isomerization from the addition of OH to the
secondary carbon can form a six membered ring with the hy-
drogen on the carbon
α
to the hydroxyl group. This isomer-
ization would result in the formation of
α
-pinene carbonyl di-
hydroperoxide which would be observed at
m/z
(
−
)301. For
the species observed at
m/z
(
−
)301 and (
−
)303 to be formed
via isomerization, the rate of peroxy radical isomerization
would have to be competitive with that of RO
2
+ HO
2
. In the
present experiments [HO
2
] is
∼
1
×
10
10
molecules cm
−
3
so
the rate of loss of
α
-pinene hydroxy peroxy radical by reac-
tion with HO
2
is
∼
0.2 s
−
1
. In the atmosphere the HO
2
con-
centration is about an order of magnitude less, so for isomer-
ization to be competitive (10 % of peroxy radical reaction)
the rate would have to be
∼
0.002 s
−
1
. In the isoprene system
the isomerization rate has been found to be 0.002 s
−
1
with
conformer specific rates being much faster (
Crounse et al.
,
2011
). At this time there have been no experimental stud-
ies on the isomerization rate in the
α
-pinene system so it is
unknown what the rate is and therefor its atmospheric rel-
evance. If the rate of isomerization is competitive with re-
action with HO
2
in the atmosphere, more low vapor pres-
sure species capable of partitioning into the aerosol will be
formed than were observed in this study.
3.2 Kinetic model of low-NO
x
photooxidation of
α
-pinene
To gain a better understanding of the low-NO
x
photooxida-
tion of
α
-pinene, a kinetic model was assembled and com-
pared to the time traces of
α
-pinene and the reaction products
measured during the photooxidation of 19.8 ppb
α
-pinene
and 4 ppm H
2
O
2
. The kinetic model was constructed using
Kintecus modeling software (
Ianni
,
2002
). When available,
rate constants from literature were used; however, a major-
ity of the rate constants are not known. In these cases, reac-
tion rates with respect to OH oxidation were estimated us-
ing the structural activity relationship derived by Kwok and
Atkinson (
Kwok and Atkinson
,
1995
). This method has been
shown to predict rate constants to within a factor of two for
most species (see Tables S1 and S2 for lists of photooxidation
products, reactions, and reaction rates used in this model).
The rate constants were then modified slightly to best fit
the data. The rate constants for RO
2
+ HO
2
and RO
2
+ RO
2
were taken from the estimates used for the Master Chemical
Mechanism (
Saunders et al.
,
2003
). Photolysis was included
for hydrogen peroxide, the organic hydroperoxides, and for
pinonaldehyde. The photodissociation frequencies (
j
) were
determined from the spectral radiance measured from the
chamber lights and the absorption cross sections reported in
the literature for hydrogen peroxide and pinonaldehyde and
estimated for the organic hydroperoxides from reported cross
sections of similar hydroperoxides (
Atkinson et al.
,
2006
;
Sander et al.
,
2006
).
For the model to be accurate, the concentration of OH and
HO
2
need to be correct. OH is produced from photolysis of
H
2
O
2
which initially reacts with hydrocarbons in the cham-
ber as well as H
2
O
2
. It is the reaction of OH with H
2
O
2
that
produces HO
2
. The value of
j
H
2
O
2
was confirmed by com-
paring the simulated loss of H
2
O
2
(photolysis and reaction
with OH) to the time trace observed from the CIMS (see SI
Fig. S1). The comparison of the simulated loss of
α
-pinene,
using the recommended rate constant for the reaction of
α
-pinene with OH from the IUPAC database (
Atkinson et al.
,
2006
), with the the observed loss of
α
-pinene also confirms
Atmos. Chem. Phys., 12, 6489–
6504
, 2012
www.atmos-chem-phys.net/12/6489/2012/