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  • Loading-dependent elemental composition of α-pinene SOA particles

    The chemical composition of secondary organic aerosol (SOA) particles, formed by the dark ozonolysis of α-pinene, was characterized by a high-resolution time-of-flight aerosol mass spectrometer. The experiments were conducted using a continuous-flow chamber, allowing the particle mass loading and chemical composition to be maintained for several days. The organic portion of the particle mass loading was varied from 0.5 to >140 μg/m<sup>3</sup> by adjusting the concentration of reacted α-pinene from 0.9 to 91.1 ppbv. The mass spectra of the organic material changed with loading. For loadings below 5 μg/m<sup>3</sup> the unit-mass-resolution <i>m/z</i> 44 (CO<sub>2</sub><sup>+</sup>) signal intensity exceeded that of <i>m/z</i> 43 (predominantly C<sub>2</sub>H<sub>3</sub>O<sup>+</sup>), suggesting more oxygenated organic material at lower loadings. The composition varied more for lower loadings (0.5 to 15 μg/m<sup>3</sup>) compared to higher loadings (15 to >140 μg/m<sup>3</sup>). The high-resolution mass spectra showed that from >140 to 0.5 μg/m<sup>3</sup> the mass percentage of fragments containing carbon and oxygen (C<sub>x</sub>H<sub>y</sub>O<sub>z</sub><sup>+</sup>) monotonically increased from 48% to 54%. Correspondingly, the mass percentage of fragments representing C<sub>x</sub>H<sub>y</sub><sup>+</sup> decreased from 52% to 46%, and the atomic oxygen-to-carbon ratio increased from 0.29 to 0.45. The atomic ratios were accurately parameterized by a four-product basis set of decadal volatility (viz. 0.1, 1.0, 10, 100 μg/m<sup>3</sup>) employing products having empirical formulas of C<sub>1</sub>H<sub>1.32</sub>O<sub>0.48</sub>, C<sub>1</sub>H<sub>1.36</sub>O<sub>0.39</sub>, C<sub>1</sub>H<sub>1.57</sub>O<sub>0.24</sub>, and C<sub>1</sub>H<sub>1.76</sub>O<sub>0.14</sub>. These findings suggest considerable caution is warranted in the extrapolation of laboratory results that were obtained under conditions of relatively high loading (i.e., >15 μg/m<sup>3</sup>) to modeling applications relevant to the atmosphere, for which loadings of 0.1 to 20 μg/m<sup>3</sup> are typical. For the lowest loadings, the particle mass spectra resembled observations reported in the literature for some atmospheric particles.
  • The time dependence of molecular iodine emission from Laminaria digitata

    We present the first in situ detection of molecular iodine emitted from the brown macroalga <i>Laminaria digitata</i> under natural stress conditions. We show that the release of I<sub>2</sub> occurs in short, strong bursts with a complex time signature. The new data indicate that algal control of I<sub>2</sub> release in the form of an oscillatory time-dependence may be based on a nonlinear autocatalytic reaction scheme which is closely linked to the production of H<sub>2</sub>O<sub>2</sub>.
  • Sulfur isotope analysis of individual aerosol particles – a new tool for studying heterogeneous oxidation processes in the marine environment

    Understanding the importance of the different oxidation pathways of sulfur dioxide (SO<sub>2</sub>) to sulfate is crucial for an interpretation of the climate effects of sulfate aerosols. Sulfur isotope analysis of atmospheric aerosol is a well established tool for identifying sources of sulfur in the atmosphere and assessment of anthropogenic influence. The power of this tool is enhanced by a new ion microprobe technique that permits isotope analysis of individual aerosol particles as small as 0.5 μm diameter. With this new single particle technique, different types of primary and secondary sulfates are first identified based on their chemical composition, and then their individual isotopic signature is measured. Our samples were collected at Mace Head, Ireland, a remote coastal station on the North Atlantic Ocean. Sea-salt-sulfate (10–60%), ammonium sulfate/sulfuric acid particles (15–65%), and non-sea-salt-sulfate (nss-sulfate) on aged salt particles all contributed significantly to sulfate loadings in our samples. <br><br> The isotopic composition of secondary sulfates depends on the isotopic composition of precursor SO<sub>2</sub> and the oxidation process. The fractionation with respect to the source SO<sub>2</sub> is poorly characterized. In the absence of conclusive laboratory experiments, we consider the kinetic fractionation of &minus;9&permil; during the gas phase oxidation of SO<sub>2</sub> by OH as suggested by Saltzman et al. (1983) and Tanaka et al. (1994) to be the most reasonable estimate for the isotope fractionation during gas phase oxidation of SO<sub>2</sub> (&alpha;<sub>hom</sub>=0.991) and the equilibrium fractionation for the uptake of SO<sub>2</sub>(g) into the aqueous phase and the dissociation to HSO<sub>3</sub><sup>&minus;</sup> of +16.5&permil; measured by Eriksen (1972a) to be the best approximation for the fractionation during oxidation in the aqueous phase (&alpha;<sub>het</sub>=1.0165). The sulfur isotope ratio of secondary sulfate particles can therefore be used to identify the oxidation pathway by which this sulfate was formed. However, the fraction of heterogeneous and homogeneous oxidation pathway calculated is very sensitive to the isotope fractionation assumed for both pathways. Particles with known oxidation pathway (fine mode ammonium sulfate) are used to estimate the isotopic composition of the source SO<sub>2</sub>. It ranged from &delta;<sup>34</sup>S<sub>VCDT</sub>=0&plusmn;3&permil; to &delta;<sup>34</sup>S<sub>VCDT</sub>=(14&plusmn;3)&permil; under clean conditions and &delta;<sup>34</sup>S<sub>VCDT</sub>=(3&plusmn;1)&permil; under polluted condition. Condensation of H<sub>2</sub>SO<sub>4</sub>(g) onto sea salt aerosol produces an isotopic ratio that, when plotted against the sea-salt-sulfate content of the sample, lies on a mixing line between sea salt and ammonium sulfate. The contribution of heterogeneous oxidation is estimated based on the deviation of non-sea-salt-sulfate from this isotopic mixing line. <br><br> The contribution of heterogeneous oxidation to nss-sulfate formation on aged sea salt sodium sulfate, magnesium sulfate gypsum and mixed sulfate particles under clean conditions is on average 10% for coarse and 25% for fine mode particles. Under polluted conditions, the contribution of heterogeneous oxidation to nss-sulfate formation increased to 60% on coarse mode and 75% on fine mode particles. However, large day-to-day variations in the contribution of heterogeneous oxidation to nss-sulfate formation occurred. Our results suggest that a~significant portion of SO<sub>2</sub> in coastal regions is converted to fine mode ammonium sulfate/sulfuric acid particles (40–80% of nss-sulfate) and that condensation of H<sub>2</sub>SO<sub>4</sub>(g) contributes significantly even to the nss-sulfate in aged sea salt particles (20–85%).
  • A global stratospheric bromine monoxide climatology based on the BASCOE chemical transport model

    A new climatology of stratospheric BrO profiles based on a parameterization using dynamical and chemical indicators has been developed, with the aim to apply it to the retrieval of tropospheric BrO columns from space nadir measurements. The adopted parameterization is based on three years of output data from the 3-D chemistry transport model BASCOE. The impact of the atmospheric dynamics on the stratospheric BrO distribution is treated by means of Br<sub>y</sub>/ozone correlations built from 3-D-CTM model results, while photochemical effects are taken into account using stratospheric NO<sub>2</sub> columns as an indicator of the BrO/Br<sub>y</sub> ratio. The model simulations have been optimized for bromine chemistry and budget, and validated through comparisons using an extensive data set of ground-based, balloon-borne and satellite limb (SCIAMACHY) stratospheric BrO observations.
  • Deep-convective vertical transport: what is mass flux?

    Conceptual basis for the convective mass flux that is used in parameterizations is reviewed from a historical perspective. The main idea of the convective mass flux formulation does not purely reside in dividing the grid-box averaged vertical velocity into several mass flux components such as convective updrafts, downdrafts, and environmental subsidence. The main point rather resides on assuming different vertical profiles for transported quantities for different components. From this point of view, the best way to turn off the convective transport of chemical species is to set the vertical profile of chemical species within convective components (both updrafts and downdrafts) equal to that of the environment. This procedure turns out to be equivalent of simply turning off a standard convective chemical transport package.
  • Contribution of atmospheric processes affecting the dynamics of air pollution in South-Western Europe during a typical summertime photochemical episode

    The southern Mediterranean region frequently experiences critical levels of photochemical pollutants during summertime. In order to account for the contribution of different atmospheric processes during this type of episodes, the WRF-ARW/HERMES/CMAQ modelling system was applied with high resolution (1 km<sup>2</sup>, 33 sigma vertical layers, 1 h) to assess the different dynamics in a coastal environment and an inland-continental zone: the North-Eastern and Central Iberian Peninsula (NEIP and CIP, respectively). The former is characterized by a very complex terrain, while the latter behaves as a flat area, which clearly affects the pattern of local flows. A representative type of photochemical pollution episode (occurring over 78% of summer days) which occurred during 17–18 June, 2004 is selected as the study period. The CMAQ Integrated Process Rate provides the hourly contributions of atmospheric processes to net O<sub>3</sub>, NO<sub>x</sub> and NMVOCs concentrations. The O<sub>3</sub> photochemical formation occurs mainly in downwind areas from the main NO<sub>x</sub> emission sources during midday. At surface level it accounts for 50 to 75 μg m<sup>&minus;3</sup> h<sup>&minus;1</sup>. The urban areas and main roads, as main sources of NO<sub>x</sub> emissions, act as O<sub>3</sub> sinks, quenching up to &minus;200 μg m<sup>&minus;3</sup> per hour during the traffic circulation peaks. The O<sub>3</sub> concentration gradient generated, larger during daytime, increases the contribution of diffusion processes to ground-level O<sub>3</sub> (up to 200 μg m<sup>&minus;3</sup> h<sup>&minus;1</sup> fluxes, mainly from upper vertical layers). The maximum positive contributions of gas-phase chemistry to O<sub>3</sub> occur in the coastal domain at high levels (around 500 to 1500 m a.g.l.), while in the continental domain they take place in the whole atmospheric column under the PBL. The transport of ozone precursors by advective flows determines the location of the maximum O<sub>3</sub> surface concentrations. The O<sub>3</sub> chemical formation involves the oxidation of less NMVOCs in the NEIP than in the CIP domains, due to differences in chemical sensitivity between these areas. The dry deposition is an important sink in the lowest layer of the model, together with vertical diffusion flows. Finally, the contributions from cloud processes, wet deposition and heterogeneous chemistry are negligible during the whole episode, characterized by a high solar radiation and neither precipitation nor cloudiness. This process analysis provides new quantitative information about the origin of the peaks of O<sub>3</sub> and its precursors, aiding the design of abatement strategies in South-Western Europe.
  • Quantification of the impact of climate uncertainty on regional air quality

    Uncertainties in calculated impacts of climate forecasts on future regional air quality are investigated using downscaled MM5 meteorological fields from the NASA GISS and MIT IGSM global models and the CMAQ model in 2050 in the continental US. Differences between three future scenarios: high-extreme, low-extreme and base case, are used for quantifying effects of climate uncertainty on regional air quality. GISS, with the IPCC A1B scenario, is used for the base case simulations. IGSM results, in the form of probabilistic distributions, are used to perturb the base case climate to provide the high- and low-extreme scenarios. Impacts of the extreme climate scenarios on concentrations of summertime fourth-highest daily maximum 8-h average ozone are predicted to be up to 10 ppbV (about one-seventh of the current US ozone standard of 75 ppbV) in urban areas of the Northeast, Midwest and Texas due to impacts of meteorological changes, especially temperature and humidity, on the photochemistry of tropospheric ozone formation and increases in biogenic VOC emissions, though the differences in average peak ozone concentrations are about 1–2 ppbV on a regional basis. Differences between the extreme and base scenarios in annualized PM<sub>2.5</sub> levels are very location dependent and predicted to range between &minus;1.0 and +1.5 &mu;g m<sup>&minus;3</sup>. Future annualized PM<sub>2.5</sub> is less sensitive to the extreme climate scenarios than summertime peak ozone since precipitation scavenging is only slightly affected by the extreme climate scenarios examined. Relative abundances of biogenic VOC and anthropogenic NO<sub>x</sub> lead to the areas that are most responsive to climate change. Overall, planned controls for decreasing regional ozone and PM<sub>2.5</sub> levels will continue to be effective in the future under the extreme climate scenarios. However, the impact of climate uncertainties may be substantial in some urban areas and should be included in assessing future regional air quality and emission control requirements.
  • Particle number emissions of motor traffic derived from street canyon measurements in a Central European city

    A biennial dataset of ambient particle number size distributions (diameter range 4–800 nm) collected in urban air in Leipzig, Germany, was analysed with respect to the influence of traffic emissions. Size distributions were sampled continuously in 2005 and 2006 inside a street canyon trafficked by ca. 10 000 motor vehicles per day, and at a background reference site distant at 1.5 km. Auto-correlation analysis showed that the impact of fresh traffic emissions could be seen most intensely below particle sizes of 60 nm. The traffic-induced concentration increment at roadside was estimated by subtracting the urban background values from the street canyon measurement. To describe the variable dispersion conditions inside the street canyon, micro-meteorological dilution factors were calculated using the Operational Street Pollution Model (OSPM), driven by above-roof wind speed and wind direction observations. The roadside increment concentrations, dilution factor, and real-time traffic counts were used to calculate vehicle emission factors (aerosol source rates) that are representative of the prevailing driving conditions, i.e. stop-and-go traffic including episodes of fluent traffic flow at speeds up to 40 km h<sup>&minus;1</sup>. The size spectrum of traffic-derived particles was essentially bimodal – with mode diameters around 12 and 100 nm, while statistical analysis suggested that the emitted number concentration varied with time of day, wind direction, particle size and fleet properties. Significantly, the particle number emissions depended on ambient temperature, ranging between 4.8 (&plusmn;1.8) and 7.8 (&plusmn;2.9).10<sup>14</sup> p. veh<sup>&minus;1</sup> km<sup>&minus;1</sup> in summer and winter, respectively. A separation of vehicle types according to vehicle length suggested that lorry-like vehicles emit about 80 times more particle number than passenger car-like vehicles. Using nitrogen oxide (NO<sub>x</sub>) measurements, specific total particle number emissions of 338 p. (pg NO<sub>x</sub>)<sup>&minus;1</sup> were inferred. The calculated traffic emission factors, considering particle number and size, are anticipated to provide useful input for future air quality and particle exposure modelling in densely populated urban areas.
  • Global temperature estimates in the troposphere and stratosphere: a validation study of COSMIC/FORMOSAT-3 measurements

    This paper mainly focuses on the validation of temperature estimates derived with the newly launched Constellation Observing System for Meteorology Ionosphere and Climate (COSMIC)/Formosa Satellite 3 (FORMOSAT-3) system. The analysis is based on the radio occultation (RO) data samples collected during the first year observation from April 2006 to April 2007. For the validation, we have used the operational stratospheric analyses including the National Centers for Environmental Prediction - Reanalysis (NCEP), the Japanese 25-year Reanalysis (JRA-25), and the United Kingdom Met Office (MetO) data sets. Comparisons done in different formats reveal good agreement between the COSMIC and reanalysis outputs. Spatially, the largest deviations are noted in the polar latitudes, and height-wise, the tropical tropopause region noted the maximum differences (2–4 K). We found that among the three reanalysis data sets the NCEP data sets have the best resemblance with the COSMIC measurements.
  • Exploring the relation between aerosol optical depth and PM2.5 at Cabauw, the Netherlands

    Estimates of PM<sub>2.5</sub> distributions based on satellite data depend critically on an established relation between AOD and ground level PM<sub>2.5</sub>. In this study we performed an experiment at Cabauw to establish a relation between AOD and PM<sub>2.5</sub> for the Netherlands. A first inspection of the AERONET L1.5 AOD and PM<sub>2.5</sub> data showed a low correlation between the two properties. The AERONET L1.5 showed relatively many observations of high AOD values paired to low PM<sub>2.5</sub> values, which hinted cloud contamination. Various methods were used to detect cloud contamination in the AERONET data to substantiate this hypothesis. A cloud screening method based on backscatter LIDAR observations was chosen to detect cloud contaminated observations in the AERONET L1.5 AOD. A later evaluation of AERONET L2.0 showed that the most data that are excluded in the update from L1.5 to L2.0 were also excluded by our cloud screening, which provides confidence in both our cloud-screening method as well as the final screening in the AERONET procedure. The use of LIDAR measurements in conjunction with the CIMEL AOD data is regarded highly beneficial. Contra-intuitively, the AOD to PM<sub>2.5</sub> relationship was shown to be insensitive to inclusion of the mixed layer height. The robustness of the relation improves dependent on the time window during the day towards noon. The final relation found for Cabauw is PM<sub>2.5</sub>=124.5&times;AOD&minus;0.34 and is valid for fair weather conditions. The relationship found between bias corrected MODIS AOD and PM<sub>2.5</sub> at Cabauw is very similar to the analysis based on the much larger dataset from ground based data only. We applied the relationship to a MODIS composite map to assess the PM<sub>2.5</sub> distribution over the Netherlands for the first time. The verification of the derived map is difficult because ground level artefact free PM<sub>2.5</sub> data are lacking. The validity and utility of our proposed mapping methodology should be further investigated.
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