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  • New insights into nocturnal nucleation

    Formation of new aerosol particles by nucleation and growth is a significant source of aerosols in the atmosphere. New particle formation events usually take place during daytime, but in some locations they have been observed also at night. In the present study we have combined chamber experiments, quantum chemical calculations and aerosol dynamics models to study nocturnal new particle formation. All our approaches demonstrate, in a consistent manner, that the oxidation products of monoterpenes play an important role in nocturnal nucleation events. By varying the conditions in our chamber experiments, we were able to reproduce the very different types of nocturnal events observed earlier in the atmosphere. The exact strength, duration and shape of the events appears to be sensitive to the type and concentration of reacting monoterpenes, as well as the extent to which the monoterpenes are exposed to ozone and potentially other atmospheric oxidants.
  • Hindcast experiments of tropospheric composition during the summer 2010 fires over western Russia

    The severe wildfires in western Russia during July–August 2010 coincided with a strong heat wave and led to large emissions of aerosols and trace gases such as carbon monoxide (CO), hydrocarbons and nitrogen oxides into the troposphere. This extreme event is used to evaluate the ability of the global MACC (Monitoring Atmospheric Composition and Climate) atmospheric composition forecasting system to provide analyses of large-scale pollution episodes and to test the respective influence of a priori emission information and data assimilation on the results. Daily 4-day hindcasts were conducted using assimilated aerosol optical depth (AOD), CO, nitrogen dioxide (NO<sub>2</sub>) and ozone (O<sub>3</sub>) data from a range of satellite instruments. Daily fire emissions were used from the Global Fire Assimilation System (GFAS) version 1.0, derived from satellite fire radiative power retrievals. <br><br> The impact of accurate wildfire emissions is dominant on the composition in the boundary layer, whereas the assimilation system influences concentrations throughout the troposphere, reflecting the vertical sensitivity of the satellite instruments. The application of the daily fire emissions reduces the area-average mean bias by 63% (for CO), 60% (O<sub>3</sub>) and 75% (NO<sub>2</sub>) during the first 24 h with respect to independent satellite observations, compared to a reference simulation with a multi-annual mean climatology of biomass burning emissions. When initial tracer concentrations are further constrained by data assimilation, biases are reduced by 87, 67 and 90%. The forecast accuracy, quantified by the mean bias up to 96 h lead time, was best for all compounds when using both the GFAS emissions and assimilation. The model simulations suggest an indirect positive impact of O<sub>3</sub> and CO assimilation on hindcasts of NO<sub>2</sub> via changes in the oxidizing capacity. <br><br> However, the quality of local hindcasts was strongly dependent on the assumptions made for forecasted fire emissions. This was well visible from a relatively poor forecast accuracy quantified by the root mean square error, as well as the temporal correlation with respect to ground-based CO total column data and AOD. This calls for a more advanced method to forecast fire emissions than the currently adopted persistency approach. <br><br> The combined analysis of fire radiative power observations, multiple trace gas and aerosol satellite observations, as provided by the MACC system, results in a detailed quantitative description of the impact of major fires on atmospheric composition, and demonstrate the capabilities for the real-time analysis and forecasts of large-scale fire events.
  • Estimation of speciated and total mercury dry deposition at monitoring locations in eastern and central North America

    Dry deposition of speciated mercury, i.e., gaseous oxidized mercury (GOM), particulate-bound mercury (PBM), and gaseous elemental mercury (GEM), was estimated for the year 2008–2009 at 19 monitoring locations in eastern and central North America. Dry deposition estimates were obtained by combining monitored two- to four-hourly speciated ambient concentrations with modeled hourly dry deposition velocities (<i>V</i><sub>d</sub>) calculated using forecasted meteorology. Annual dry deposition of GOM+PBM was estimated to be in the range of 0.4 to 8.1 μg m<sup>−2</sup> at these locations with GOM deposition being mostly five to ten times higher than PBM deposition, due to their different modeled <i>V</i><sub>d</sub> values. Net annual GEM dry deposition was estimated to be in the range of 5 to 26 μg m<sup>−2</sup> at 18 sites and 33 μg m<sup>−2</sup> at one site. The estimated dry deposition agrees very well with limited surrogate-surface dry deposition measurements of GOM and PBM, and also agrees with litterfall mercury measurements conducted at multiple locations in eastern and central North America. This study suggests that GEM contributes much more than GOM+PBM to the total dry deposition at the majority of the sites considered here; the only exception is at locations close to significant point sources where GEM and GOM+PBM contribute equally to the total dry deposition. The relative magnitude of the speciated dry deposition and their good comparisons with litterfall deposition suggest that mercury in litterfall originates primarily from GEM, which is consistent with the limited number of previous field studies. The study also supports previous analyses suggesting that total dry deposition of mercury is equal to, if not more important than, wet deposition of mercury on a regional scale in eastern North America.
  • Atmospheric histories and growth trends of C4F10, C5F12, C6F14, C7F16 and C8F18

    Atmospheric observations and trends are presented for the high molecular weight perfluorocarbons (PFCs): decafluorobutane (C<sub>4</sub>F<sub>10</sub>), dodecafluoropentane (C<sub>5</sub>F<sub>12</sub>), tetradecafluorohexane (C<sub>6</sub>F<sub>14</sub>), hexadecafluoroheptane (C<sub>7</sub>F<sub>16</sub>) and octadecafluorooctane (C<sub>8</sub>F<sub>18</sub>). Their atmospheric histories are based on measurements of 36 Northern Hemisphere and 46 Southern Hemisphere archived air samples collected between 1973 to 2011 using the Advanced Global Atmospheric Gases Experiment (AGAGE) "Medusa" preconcentration gas chromatography-mass spectrometry systems. A new calibration scale was prepared for each PFC, with estimated accuracies of 6.8% for C<sub>4</sub>F<sub>10</sub>, 7.8% for C<sub>5</sub>F<sub>12</sub>, 4.0% for C<sub>6</sub>F<sub>14</sub>, 6.6% for C<sub>7</sub>F<sub>16</sub> and 7.9% for C<sub>8</sub>F<sub>18</sub>. Based on our observations the 2011 globally averaged dry air mole fractions of these heavy PFCs are: 0.17 parts-per-trillion (ppt, i.e., parts per 10<sup>12</sup>) for C<sub>4</sub>F<sub>10</sub>, 0.12 ppt for C<sub>5</sub>F<sub>12</sub>, 0.27 ppt for C<sub>6</sub>F<sub>14</sub>, 0.12 ppt for C<sub>7</sub>F<sub>16</sub> and 0.09 ppt for C<sub>8</sub>F<sub>18</sub>. These atmospheric mole fractions combine to contribute to a global average radiative forcing of 0.35 mW m<sup>−2</sup>, which is 6% of the total anthropogenic PFC radiative forcing (Montzka and Reimann, 2011; Oram et al., 2012). The growth rates of the heavy perfluorocarbons were largest in the late 1990s peaking at 6.2 parts per quadrillion (ppq, i.e., parts per 10<sup>15</sup>) per year (yr) for C<sub>4</sub>F<sub>10</sub>, at 5.0 ppq yr<sup>−1</sup> for C<sub>5</sub>F<sub>12</sub> and 16.6 ppq yr<sup>−1</sup> for C<sub>6</sub>F<sub>14</sub> and in the early 1990s for C<sub>7</sub>F<sub>16</sub> at 4.7 ppq yr<sup>−1</sup> and in the mid 1990s for C<sub>8</sub>F<sub>18</sub> at 4.8 ppq yr<sup>−1</sup>. The 2011 globally averaged mean atmospheric growth rates of these PFCs are subsequently lower at 2.2 ppq yr<sup>−1</sup> for C<sub>4</sub>F<sub>10</sub>, 1.4 ppq yr<sup>−1</sup> for C<sub>5</sub>F<sub>12</sub>, 5.0 ppq yr<sup>−1</sup> for C<sub>6</sub>F<sub>14</sub>, 3.4 ppq yr<sup>−1</sup> for C<sub>7</sub>F<sub>16</sub> and 0.9 ppq yr<sup>−1</sup> for C<sub>8</sub>F<sub>18</sub>. The more recent slowdown in the growth rates suggests that emissions are declining as compared to the 1980s and 1990s.
  • Megacity ozone air quality under four alternative future scenarios

    The impact of the megacities of the world on global tropospheric ozone, and conversely, the extent to which megacities are influenced by emissions of ozone precursors from outside of the megacities is examined under the four alternative RCP ("Representative Concentration Pathway") emissions scenarios. Despite accounting for about 6% of present-day anthropogenic emissions of ozone precursor species, the contribution of emissions from megacities to global tropospheric ozone is calculated to be 0.84%. By 2100 this contribution falls to between 0.18% and 0.62% depending on the scenario, with the lower value being for the most-polluting of the four future emissions scenarios due to stringent controls on ozone precursor emissions from highly populated areas combined with a stronger tropospheric background ozone field. The higher end of this range is from the least-polluting of the four emissions scenarios, due to lower background tropospheric ozone combined with the use of a simpler downscaling methodology in the construction of the scenario, which results in higher emissions from megacities. Although the absolute impact of megacities on global ozone is small, an important result of this study is that under all future scenarios, future air quality in megacities is expected to be less influenced by local emissions within the cities, but instead more influenced by emission sources outside of the cities, with mixing ratios of background ozone projected to play an increasing role in megacity air quality throughout the 21st century. Assumptions made when downscaling the emissions scenarios onto the grids used in such modelling studies can have a large influence on these results; future generations of emissions scenarios should include spatially explicit representations or urban development suitable for air quality studies using global chemical transport models.
  • Sulfuric acid nucleation: power dependencies, variation with relative humidity, and effect of bases

    Nucleation of particles composed of sulfuric acid, water, and nitrogen base molecules was studied using a continuous flow reactor. The particles formed from these vapors were detected with an ultrafine condensation particle counter, while vapors of sulfuric acid and nitrogen bases were detected by chemical ionization mass spectrometry. Variation of particle numbers with sulfuric acid concentration yielded a power dependency on sulfuric acid of 5 ± 1 for relative humidities of 14–68% at 296 K; similar experiments with varying water content yielded power dependencies on H<sub>2</sub>O of ~7. The critical cluster contains about 5 H<sub>2</sub>SO<sub>4</sub> molecules and a new treatment of the power dependency for H<sub>2</sub>O suggests about 12 H<sub>2</sub>O molecules for these conditions. Addition of 2-to-45 pptv of ammonia or methyl amine resulted in up to millions of times more particles than in the absence of these compounds. Particle detection capabilities, sulfuric acid and nitrogen base detection, wall losses, and the extent of particle growth are discussed. Results are compared to previous laboratory nucleation studies and they are also discussed in terms of atmospheric nucleation scenarios.
  • The isotopic record of Northern Hemisphere atmospheric carbon monoxide since 1950: implications for the CO budget

    We present a 60-year record of the stable isotopes of atmospheric carbon monoxide (CO) from firn air samples collected under the framework of the North Greenland Eemian Ice Drilling (NEEM) project. CO concentration, &delta;<sup>13</sup>C, and &delta;<sup>18</sup>O of CO were measured by gas chromatography/isotope ratio mass spectrometry (gc-IRMS) from trapped gases in the firn. We applied LGGE-GIPSA firn air models (Witrant et al., 2011) to correlate gas age with firn air depth and then reconstructed the trend of atmospheric CO and its stable isotopic composition at high northern latitudes since 1950. The most probable firn air model scenarios show that &delta;<sup>13</sup>C decreased slightly from −25.8&permil; in 1950 to −26.4&permil; in 2000, then decreased more significantly to −27.2&permil; in 2008. &delta;<sup>18</sup>O decreased more regularly from 9.8&permil; in 1950 to 7.1&permil; in 2008. Those same scenarios show CO concentration increased gradually from 1950 and peaked in the late 1970s, followed by a gradual decrease to present day values (Petrenko et al., 2012). Results from an isotope mass balance model indicate that a slight increase, followed by a large reduction, in CO derived from fossil fuel combustion has occurred since 1950. The reduction of CO emission from fossil fuel combustion after the mid-1970s is the most plausible mechanism for the drop of CO concentration during this time. Fossil fuel CO emissions decreased as a result of the implementation of catalytic converters and the relative growth of diesel engines, in spite of the global vehicle fleet size having grown several fold over the same time period.
  • Growth in NOx emissions from power plants in China: bottom-up estimates and satellite observations

    Using OMI (Ozone Monitoring Instrument) tropospheric NO<sub>2</sub> columns and a nested-grid 3-D global chemical transport model (GEOS-Chem), we investigated the growth in NO<sub>x</sub> emissions from coal-fired power plants and their contributions to the growth in NO<sub>2</sub> columns in 2005–2007 in China. We first developed a unit-based power plant NO<sub>x</sub> emission inventory for 2005–2007 to support this investigation. The total capacities of coal-fired power generation have increased by 48.8% in 2005–2007, with 92.2% of the total capacity additions coming from generator units with size &ge;300 MW. The annual NO<sub>x</sub> emissions from coal-fired power plants were estimated to be 8.11 Tg NO<sub>2</sub> for 2005 and 9.58 Tg NO<sub>2</sub> for 2007, respectively. The modeled summer average tropospheric NO<sub>2</sub> columns were highly correlated (<i>R</i><sup>2</sup> = 0.79–0.82) with OMI measurements over grids dominated by power plant emissions, with only 7–14% low bias, lending support to the high accuracy of the unit-based power plant NO<sub>x</sub> emission inventory. The ratios of OMI-derived annual and summer average tropospheric NO<sub>2</sub> columns between 2007 and 2005 indicated that most of the grids with significant NO<sub>2</sub> increases were related to power plant construction activities. OMI had the capability to trace the changes of NO<sub>x</sub> emissions from individual large power plants in cases where there is less interference from other NO<sub>x</sub> sources. Scenario runs from GEOS-Chem model suggested that the new power plants contributed 18.5% and 10% to the annual average NO<sub>2</sub> columns in 2007 in Inner Mongolia and North China, respectively. The massive new power plant NO<sub>x</sub> emissions significantly changed the local NO<sub>2</sub> profiles, especially in less polluted areas. A sensitivity study found that changes of NO<sub>2</sub> shape factors due to including new power plant emissions increased the summer average OMI tropospheric NO<sub>2</sub> columns by 3.8–17.2% for six selected locations, indicating that the updated emission information could help to improve the satellite retrievals.
  • Assimilation of IASI satellite CO fields into a global chemistry transport model for validation against aircraft measurements

    This work evaluates the IASI CO product against independent in-situ aircraft data from the MOZAIC program and the POLARCAT aircraft campaign. The validation is carried out by analysing the impact of assimilation of eight months of IASI CO columns retrieved for the period of May to December 2008 into the global chemistry transport model LMDz-INCA. A modelling system based on a sub-optimal Kalman filter was developed and a specific treatment that takes into account the representativeness of observations at the scale of the model grid is applied to the IASI CO columns and associated errors before their assimilation in the model. Comparisons of the assimilated CO profiles with in situ CO measurements indicate that the assimilation leads to a considerable improvement of the model simulations in the middle troposphere as compared with a control run with no assimilation. Model biases in the simulation of background values are reduced and improvement in the simulation of very high concentrations is observed. The improvement is due to the transport by the model of the information present in the IASI CO retrievals. Our analysis also shows the impact of assimilation of CO on the representation of transport into the Arctic region during the POLARCAT summer campaign. A considerable increase in CO mixing ratios over the Asian source region was observed when assimilation was used leading to much higher values of CO during the cross-pole transport episode. These higher values are in good agreement with data from the POLARCAT flights that sampled this plume.
  • Size-resolved measurement of the mixing state of soot in the megacity Beijing, China: diurnal cycle, aging and parameterization

    Soot particles are the most efficient light absorbing aerosol species in the atmosphere, playing an important role as a driver of global warming. Their climate effects strongly depend on their mixing state, which significantly changes their light absorbing capability and cloud condensation nuclei (CCN) activity. Therefore, knowledge about the mixing state of soot and its aging mechanism becomes an important topic in the atmospheric sciences. <br><br> The size-resolved (30–320 nm diameter) mixing state of soot particles in polluted megacity air was measured at a suburban site (Yufa) during the CAREBeijing 2006 campaign in Beijing, using a volatility tandem differential mobility analyzer (VTDMA). Particles in this size range with non-volatile residuals at 300 &deg;C were considered to be soot particles. On average, the number fraction of internally mixed soot in total soot particles (<i>F</i><sub>in</sub>), decreased from 0.80 to 0.57 when initial <i>D</i><sub>p</sub> increased from 30 to 320 nm. Further analysis reveals that: (1) <i>F</i><sub>in</sub> was well correlated with the aerosol hygroscopic mixing state measured by a CCN counter. More externally mixed soot particles were observed when particles showed more heterogeneous features with regard to hygroscopicity. (2) <i>F</i><sub>in</sub> had pronounced diurnal cycles. For particles in the accumulation mode (<i>D</i><sub>p</sub> at 100–320 nm), largest <i>F</i><sub>in</sub> were observed at noon time, with "apparent" turnover rates (<i>k</i><sub>ex &rarr; in</sub>) up to 7.8% h<sup>−1</sup>. (3) <i>F</i><sub>in</sub> was subject to competing effects of both aging and emissions. While aging increases <i>F</i><sub>in</sub> by converting externally mixed soot particles into internally mixed ones, emissions tend to reduce <i>F</i><sub>in</sub> by emitting more fresh and externally mixed soot particles. Similar competing effects were also found with air mass age indicators. (4) Under the estimated emission intensities, actual turnover rates of soot (<i>k</i><sub>ex &rarr; in</sub>) up to 20% h<sup>−1</sup> were derived, which showed a pronounced diurnal cycle peaking around noon time. This result confirms that (soot) particles are undergoing fast aging/coating with the existing high levels of condensable vapors in the megacity Beijing. (5) Diurnal cycles of <i>F</i><sub>in</sub> were different between Aitken and accumulation mode particles, which could be explained by the faster growth of smaller Aitken mode particles into larger size bins. <br><br> To improve the <i>F</i><sub>in</sub> prediction in regional/global models, we suggest parameterizing <i>F</i><sub>in</sub> by an air mass aging indicator, i.e., <i>F</i><sub>in</sub> = <i>a</i> + <i>bx</i>, where <i>a</i> and <i>b</i> are empirical coefficients determined from observations, and <i>x</i> is the value of an air mass age indicator. At the Yufa site in the North China Plain, fitted coefficients (<i>a</i>, <i>b</i>) were determined as (0.57, 0.21), (0.47, 0.21), and (0.52, 0.0088) for <i>x</i> (indicators) as [NO<sub>z</sub>]/[NO<sub>y</sub>], [E]/[X] ([ethylbenzene]/[m,p-xylene]) and ([IM] + [OM])/[EC] ([inorganic + organic matter]/[elemental carbon]), respectively. Such a parameterization consumes little additional computing time, but yields a more realistic description of <i>F</i><sub>in</sub> compared with the simple treatment of soot mixing state in regional/global models.
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