7 research outputs found
The Interaction of Propionic and Butyric Acids with Ice and HNO<sub>3</sub>‑Doped Ice Surfaces at 195–212 K
The
interaction of propionic and butyric acids on ice and HNO3-doped ice were studied between 195 and 212 K and low concentrations,
using a Knudsen flow reactor coupled with a quadrupole mass spectrometer.
The initial uptake coefficients (γ0) of propionic
and butyric acids on ice as a function of temperature are given by
the expressions: γ0(T) = (7.30 ±
1.0) × 10–10 exp[(3216 ± 478)/T] and γ0(T) = (6.36 ±
0.76) × 10–11 exp[(3810 ± 434)/T], respectively; the quoted error limits are at 95% level
of confidence. Similarly, γ0 of propionic acid on
1.96 wt % (A) and 7.69 wt % (B) HNO3-doped ice with temperature
are given as γ0,A(T) = (2.89 ±
0.26) × 10–8 exp[(2517 ± 266)/T] and γ0,B(T) = (2.77
± 0.29) × 10–7 exp[(2126 ± 206)/T], respectively. The results show that γ0 of C1 to C4 n-carboxylic acids on ice increase
with the alkyl-group length, due to lateral interactions between alkyl-groups
that favor a more perpendicular orientation and well packing of H-bonded
monomers on ice. The high uptakes (>1015 molecules cm–2) and long recovery signals indicate efficient growth
of random multilayers above the first monolayer driven by significant
van der Waals interactions. The heterogeneous loss of both acids on
ice and HNO3-doped ice particles in dense cirrus clouds
is estimated to take a few minutes, signifying rapid local heterogeneous
removal by dense cirrus clouds
Absolute Rate Coefficient Determination and Reaction Mechanism Investigation for the Reaction of Cl Atoms with CH<sub>2</sub>I<sub>2</sub> and the Oxidation Mechanism of CH<sub>2</sub>I Radicals
The gas-phase reaction of atomic chlorine with diiodomethane was studied over the temperature range 273−363 K with the very low-pressure reactor (VLPR) technique. The reaction takes place in a Knudsen reactor
at pressures below 3 mTorr, where the steady-state concentration of both reactants and stable products is
continuously measured by electron-impact mass spectrometry. The absolute rate coefficient as a function of
temperature was given by k = (4.70 ± 0.65) × 10-11 exp[−(241 ± 33)/T] cm3molecule-1s-1, in the low-pressure regime. The quoted uncertainties are given at a 95% level of confidence (2σ) and include systematic
errors. The reaction occurs via two pathways:  the abstraction of a hydrogen atom leading to HCl and the
abstraction of an iodine atom leading to ICl. The HCl yield was measured to be ca. 55 ± 10%. The results
suggest that the reaction proceeds via the intermediate CH2I2−Cl adduct formation, with a I−Cl bond strength
of 51.9 ± 15 kJ mol-1, calculated at the B3P86/aug-cc-pVTZ-PP level of theory. Furthermore, the oxidation
reactions of CHI2 and CH2I radicals were studied by introducing an excess of molecular oxygen in the Knudsen
reactor. HCHO and HCOOH were the primary oxidation products indicating that the reactions with O2 proceed
via the intermediate peroxy radical formation and the subsequent elimination of either IO radical or I atom.
HCHO and HCOOH were also detected by FT-IR, as the reaction products of photolytically generated CH2I
radicals with O2 in a static cell, which supports the proposed oxidation mechanism. Since the photolysis of
CH2I2 is about 3 orders of magnitude faster than its reactive loss by Cl atoms, the title reaction does not
constitute an important tropospheric sink for CH2I2
Water Interactions with Acetic Acid Layers on Ice and Graphite
Adsorbed organic compounds modify
the properties of environmental
interfaces with potential implications for many Earth system processes.
Here, we describe experimental studies of water interactions with
acetic acid (AcOH) layers on ice and graphite surfaces at temperatures
from 186 to 200 K. Hyperthermal D<sub>2</sub>O water molecules are
efficiently trapped on all of the investigated surfaces, with only
a minor fraction that scatters inelastically after an 80% loss of
kinetic energy to surface modes. Trapped molecules desorb rapidly
from both μm-thick solid AcOH and AcOH monolayers on graphite,
indicating that water has limited opportunities to form hydrogen bonds
with these surfaces. In contrast, trapped water molecules bind efficiently
to AcOH-covered ice and remain on the surface on the observational
time scale of the experiments (60 ms). Thus, adsorbed AcOH is observed
to have a significant impact on water–ice surface properties
and to enhance the water accommodation coefficient compared to bare
ice surfaces. The mechanism for increased water uptake and the implications
for atmospheric cloud processes are discussed
Uptake Measurements of Acetic Acid on Ice and Nitric Acid-Doped Thin Ice Films over Upper Troposphere/Lower Stratosphere Temperatures
The adsorption of gaseous acetic acid (CH<sub>3</sub>CÂ(O)ÂOH) on
thin ice films and on ice doped with nitric acid (1.96 and 7.69 wt
%) was investigated over upper troposphere and lower stratosphere
(UT/LS) temperatures (198–208 K), and at low gas concentrations.
Experiments were performed in a Knudsen flow reactor coupled to a
quadrupole mass spectrometer. The initial uptake coefficients, γ<sub>0</sub>, on thin ice films or HNO<sub>3</sub>-doped ice films were
measured at low surface coverage. In all cases, γ<sub>0</sub> showed an inverse temperature dependence, and for pure thin ice
films, it was given by the expression<i> </i>γ<sub>0</sub>(<i>T</i>) = (4.73 ± 1.13) × 10<sup>–17</sup> exp[(6496 ± 1798)/<i>T</i>]; the quoted errors are the 2σ precision of the linear fit,
and the estimated systematic uncertainties are included in the pre-exponential
factor. The inverse temperature dependence suggests that the adsorption
process occurs via the formation of an intermediate precursor state.
Uptakes were well represented by the Langmuir adsorption model, and
the saturation surface coverage, <i>N</i><sub>max</sub>,
on pure thin ice films was (2.11 ± 0.16) × 10<sup>14</sup> molecules cm<sup>–2</sup>, independent of temperature in
the range 198–206 K. Light nitration (1.96 and 7.69 wt %) of
ice films resulted in more efficient CH<sub>3</sub>CÂ(O)ÂOH uptakes
and larger <i>N</i><sub>max</sub> values that may be attributed
to in-bulk diffusion or change in nature of the gas–ice surface
interaction. Finally, it was estimated that the rate of adsorption
of acetic acid on high-density cirrus clouds in the UT/LS is fast,
and this is reflected in the short atmospheric lifetimes (2–8
min) of acetic acid; however, the extent of this uptake is minor resulting
in at most a 5% removal of acetic acid in UT/LS cirrus clouds
Water Accommodation on Ice and Organic Surfaces: Insights from Environmental Molecular Beam Experiments
Water uptake on aerosol and cloud
particles in the atmosphere modifies
their chemistry and microphysics with important implications for climate
on Earth. Here, we apply an environmental molecular beam (EMB) method
to characterize water accommodation on ice and organic surfaces. The
adsorption of surface-active compounds including short-chain alcohols,
nitric acid, and acetic acid significantly affects accommodation of
D<sub>2</sub>O on ice. <i>n</i>-Hexanol and <i>n</i>-butanol adlayers reduce water uptake by facilitating rapid desorption
and function as inefficient barriers for accommodation as well as
desorption of water, while the effect of adsorbed methanol is small.
Water accommodation is close to unity on nitric-acid- and acetic-acid-covered
ice, and accommodation is significantly more efficient than that on
the bare ice surface. Water uptake is inefficient on solid alcohols
and acetic acid but strongly enhanced on liquid phases including a
quasi-liquid layer on solid <i>n</i>-butanol. The EMB method
provides unique information on accommodation and rapid kinetics on
volatile surfaces, and these studies suggest that adsorbed organic
and acidic compounds need to be taken into account when describing
water at environmental interfaces
Kinetic Study of the Reactions of Cl Atoms with CF<sub>3</sub>CH<sub>2</sub>CH<sub>2</sub>OH, CF<sub>3</sub>CF<sub>2</sub>CH<sub>2</sub>OH, CHF<sub>2</sub>CF<sub>2</sub>CH<sub>2</sub>OH, and CF<sub>3</sub>CHFCF<sub>2</sub>CH<sub>2</sub>OH
The reaction kinetics of chlorine atoms with a series of partially fluorinated straight-chain alcohols, CF3CH2CH2OH (1), CF3CF2CH2OH (2), CHF2CF2CH2OH (3), and CF3CHFCF2CH2OH (4), were studied in the
gas phase over the temperature range of 273−363 K by using very low-pressure reactor mass spectrometry.
The absolute rate coefficients were given by the expressions (in cm3 molecule-1 s-1):  k1 = (4.42 ± 0.48) ×
10-11 exp(−255 ± 20/T); k1(303) = (1.90 ± 0.17) × 10-11, k2 = (2.23 ± 0.31) × 10-11 exp(−1065 ± 106/
T); k2(303) = (6.78 ± 0.63) × 10-13, k3 = (8.51 ± 0.62) × 10-12 exp(−681 ± 72/T); k3(303) = (9.00 ±
0.82) × 10-13 and k4 = (6.18 ± 0.84) × 10-12 exp(−736 ± 42/T); k4(303) = (5.36 ± 0.51) × 10-13. The
quoted 2σ uncertainties include the systematic errors. All title reactions proceed via a hydrogen atom metathesis
mechanism leading to HCl. Moreover, the oxidation of the primarily produced radicals was investigated, and
the end products were the corresponding aldehydes (RF−CHO; RF = −CH2CF3, −CF2CF3, −CF2CHF2,
and −CF2CHFCF3), providing a strong experimental indication that the primary reactions proceed mainly
via the abstraction of a methylenic hydrogen adjacent to a hydroxyl group. Finally, the bond strengths and
ionization potentials for the title compounds were determined by density functional theory calculations, which
also suggest that the α-methylenic hydrogen is mainly under abstraction by Cl atoms. The correlation of
room-temperature rate coefficients with ionization potentials for a set of 27 molecules, comprising fluorinated
C2−C5 ethers and C2−C4 alcohols, is good with an average deviation of a factor of 2, and is given by the
expression log(k) (in cm3 molecule-1 s-1) = (5.8 ± 1.4) − (1.56 ± 0.13) × (ionization potential (in eV))
Kinetic Study of the Reactions of Cl Atoms with CF<sub>3</sub>CH<sub>2</sub>CH<sub>2</sub>OH, CF<sub>3</sub>CF<sub>2</sub>CH<sub>2</sub>OH, CHF<sub>2</sub>CF<sub>2</sub>CH<sub>2</sub>OH, and CF<sub>3</sub>CHFCF<sub>2</sub>CH<sub>2</sub>OH
The reaction kinetics of chlorine atoms with a series of partially fluorinated straight-chain alcohols, CF3CH2CH2OH (1), CF3CF2CH2OH (2), CHF2CF2CH2OH (3), and CF3CHFCF2CH2OH (4), were studied in the
gas phase over the temperature range of 273−363 K by using very low-pressure reactor mass spectrometry.
The absolute rate coefficients were given by the expressions (in cm3 molecule-1 s-1):  k1 = (4.42 ± 0.48) ×
10-11 exp(−255 ± 20/T); k1(303) = (1.90 ± 0.17) × 10-11, k2 = (2.23 ± 0.31) × 10-11 exp(−1065 ± 106/
T); k2(303) = (6.78 ± 0.63) × 10-13, k3 = (8.51 ± 0.62) × 10-12 exp(−681 ± 72/T); k3(303) = (9.00 ±
0.82) × 10-13 and k4 = (6.18 ± 0.84) × 10-12 exp(−736 ± 42/T); k4(303) = (5.36 ± 0.51) × 10-13. The
quoted 2σ uncertainties include the systematic errors. All title reactions proceed via a hydrogen atom metathesis
mechanism leading to HCl. Moreover, the oxidation of the primarily produced radicals was investigated, and
the end products were the corresponding aldehydes (RF−CHO; RF = −CH2CF3, −CF2CF3, −CF2CHF2,
and −CF2CHFCF3), providing a strong experimental indication that the primary reactions proceed mainly
via the abstraction of a methylenic hydrogen adjacent to a hydroxyl group. Finally, the bond strengths and
ionization potentials for the title compounds were determined by density functional theory calculations, which
also suggest that the α-methylenic hydrogen is mainly under abstraction by Cl atoms. The correlation of
room-temperature rate coefficients with ionization potentials for a set of 27 molecules, comprising fluorinated
C2−C5 ethers and C2−C4 alcohols, is good with an average deviation of a factor of 2, and is given by the
expression log(k) (in cm3 molecule-1 s-1) = (5.8 ± 1.4) − (1.56 ± 0.13) × (ionization potential (in eV))