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  • Measurements of OH and HO2 concentrations during the MCMA-2006 field campaign – Part 2: Model comparison and radical budget

    Measurements of hydroxyl (OH) and hydroperoxy (HO<sub>2</sub>) radicals were made during the Mexico City Metropolitan Area (MCMA) field campaign as part of the MILAGRO (Megacity Initiative: Local and Global Research Observations) project during March 2006. These measurements provide a unique opportunity to test current models of atmospheric RO<sub>x</sub> (OH + HO<sub>2</sub> + RO<sub>2</sub>) photochemistry under polluted conditions. A zero-dimensional box model based on the Regional Atmospheric Chemical Mechanism (RACM) was constrained by 10-min averages of 24 <i>J</i>-values and the concentrations of 97 chemical species. Several issues related to the RO<sub>x</sub> chemistry under polluted conditions are highlighted in this study: (i) Measured concentrations of both OH and HO<sub>2</sub> were underpredicted during morning hours on a median campaign basis, suggesting a significant source of radicals is missing from current atmospheric models under polluted conditions, consistent with previous urban field campaigns. (ii) The model-predicted HO<sub>2</sub>/OH ratios underestimate the measurements for NO mixing ratios higher than 5 ppb, also consistent with previous urban field campaigns. This suggests that under high NO<sub>x</sub> conditions, the HO<sub>2</sub> to OH propagation rate may be overestimated by the model or a process converting OH into HO<sub>2</sub> may be missing from the chemical mechanism. On a daily basis (08:40 a.m.–06:40 p.m.), an analysis of the radical budget indicates that HONO photolysis, HCHO photolysis, O<sub>3</sub>-alkene reactions and dicarbonyls photolysis are the main radical sources. O<sub>3</sub> photolysis contributes to less than 6% of the total radical production.
  • Intercomparison of integrated IASI and AATSR calibrated radiances at 11 and 12 &mu;m

    The mission objectives of the Infrared Atmospheric Sounding Interferometer (IASI) are driven by the needs of the Numerical Weather Prediction (NWP) and climate monitoring communities. These objectives rely upon the IASI instrument being able to measure top of atmosphere radiances accurately. This paper presents a technique and first results for the validation of the radiometric calibration of radiances for IASI, using a cross-calibration with the Advanced Along Track Scanning Radiometer (AATSR). The AATSR is able to measure Brightness Temperature (BT) to an accuracy of 30 mK, and by applying the AATSR spectral filter functions to the IASI measured radiances we are able to compare AATSR and IASI Brightness Temperatures. By choosing coincident data points that are over the sea and in clear sky conditions, a threshold of homogeneity is derived. It is found that in these homogenous conditions, the IASI BTs agree with those measured by the AATSR to within 0.3 K, with an uncertainty of order 0.1 K. The agreement is particularly good at 11 &mu;m where the difference is less than 0.1 K. These first results indicate that IASI is meeting its target objective of 0.5 K accuracy. It is believed that a refinement of the AATSR spectral filter functions will hopefully permit a tighter error constraint on the quality of the IASI data and hence further assessment of the climate quality of the radiances.
  • Isoprene oxidation by nitrate radical: alkyl nitrate and secondary organic aerosol yields

    Alkyl nitrates and secondary organic aerosol (SOA) produced during the oxidation of isoprene by nitrate radicals has been observed in the SAPHIR (Simulation of Atmospheric PHotochemistry In a large Reaction Chamber) chamber. A 16 h dark experiment was conducted with temperatures at 289–301 K, and maximum concentrations of 11 ppb isoprene, 62.4 ppb O<sub>3</sub> and 31.1 ppb NO<sub>x</sub>. We find the yield of nitrates is 70&plusmn;8% from the isoprene + NO<sub>3</sub> reaction, and the yield for secondary dinitrates produced in the reaction of primary isoprene nitrates with NO<sub>3</sub> is 40&plusmn;20%. We find an effective rate constant for reaction of NO<sub>3</sub> with the group of first generation oxidation products to be 7&times;10<sup>&minus;14</sup> molecule<sup>&minus;1</sup> cm<sup>3</sup> s<sup>&minus;1</sup>. At the low total organic aerosol concentration in the chamber (max=0.52 μg m<sup>&minus;3</sup>) we observed a mass yield (ΔSOA mass/Δisoprene mass) of 2% for the entire 16 h experiment. However a comparison of the timing of the observed SOA production to a box model simulation of first and second generation oxidation products shows that the yield from the first generation products was &lt;0.7% while the further oxidation of the initial products leads to a yield of 14% (defined as ΔSOA/Δisoprene<sup>2x</sup> where Δisoprene<sup>2x</sup> is the mass of isoprene which reacted twice with NO<sub>3</sub>). The SOA yield of 14% is consistent with equilibrium partitioning of highly functionalized C<sub>5</sub> products of isoprene oxidation.
  • Influence of particle size on the ice nucleating ability of mineral dusts

    The recently developed Zurich Ice Nucleation Chamber (ZINC) was used to explore ice nucleation of size-selected mineral dust particles at temperatures between &minus;20&deg;C and &minus;55&deg;C. Four different mineral dust species have been tested: montmorillonite, kaolinite, illite and Arizona test dust (ATD). The selected particle diameters are 100 nm, 200 nm, 400 nm and 800 nm. Relative humidities with respect to ice (RH<sub>i</sub>) required to activate 1% of the dust particles as ice nuclei (IN) are reported as a function of temperature. An explicit size dependence of the ice formation efficiency has been observed for all dust types. 800 nm particles required the lowest RH<sub>i</sub> to activate. Deposition nucleation below water saturation was found only below &minus;30&deg;C or &minus;35&deg;C dependent on particle size. Minimum RH<sub>i</sub> for 1% activation were 105% for illite, kaolinite and montmorillonite at &minus;40&deg;C, respectively 110% for ATD at &minus;45&deg;C. In addition, a possible parameterisation for the measured activation spectra is proposed, which could be used in modeling studies.
  • Variability of residence time in the Tropical Tropopause Layer during Northern Hemisphere winter

    For the first time the long-term interannual and spatial variability of residence time (τ) is presented for the TTL between 360 K and 400 K potential temperature (~14 to 18 km altitude). The analysis is based on a Lagrangian approach using offline calculated diabatic heating rates as vertical velocities, covering Northern Hemisphere (NH) winters from 1962–2004. <br><br> The residence time &tau;<sub>LCP&ndash;400 K</sub>, being the duration time of air parcels in the layer between the Lagrangian Cold Point (LCP) and 400 K, varies spatially and is longer (&gt;50 days) over the maritime continent as the LCP is lowest there (&lt;370 K). Comparing three theta layers within the TTL reveals the vertical dependence of τ. We derive a mean duration time of 34 days for 360–380 K (lower TTL), 38 days for 380–400 K (upper TTL) and 70 days for 360–400 K theta layers for the 1962–2001 period. A case analysis reveals that τ is positively skewed for 360–380 K and 380–400 K during La Niña and El Niño Southern Oscillation (ENSO) neutral years. For these cases, ~60% of air parcels travel from 360 K to 380 K within 25 days. There is large interannual variability for τ varying up to &plusmn;20% from the long-term mean, with strongest variability seen in the lower part of the TTL. Statistical analysis reveals a significant anti-correlation between the residence time and the extratropical and subtropical wave driving in the lowermost stratosphere.
  • Factors determining the effect of aerosols on cloud mass and the dependence of these factors on liquid-water path

    Increasing aerosols decreases the size of droplets and thus their collection efficiencies, leading to an inefficient conversion of droplets to precipitable raindrops. This, in turn, increases the mass of droplets suspended in the air by decreasing the removal of cloud mass by sedimentation and has been known to be a main mechanism which determines the effect of aerosols on cloud mass. However, a recent study showed that this mechanism played a negligible role in the determination of the cloud mass as compared to aerosol-induced feedbacks between microphysics and dynamics in thin stratocumulus clouds with LWP of ~50 g m<sup&minus;2</suP> or less. This is contrary to studies which have shown that the mechanism associated with the aerosol-induced inefficient conversion plays an important role in the determination of the effect of aerosols on cloud mass. These studies are generally based on clouds with LWP &gt;50 g m<sup>&minus;2</sup>. Hence, it is important to understand whether the role of aerosol-induced feedbacks in the effect of aerosols on cloud mass depends on the level of LWP. This study examines the dependence of the role of the conversion of droplets to raindrops and their sedimentation in the determination of the effect of aerosols on cloud mass on the level of LWP. Pairs of numerical experiments for high and low aerosol cases are run for four cases of stratiform clouds with different LWPs. Comparisons among these cases show that the role of the conversion and sedimentation becomes less important as the level of LWP decreases. Instead, the role of the feedbacks between microphysics and dynamics become more important with the lowering level of LWP. The results of this study indicate that the traditional approach to the understanding of the aerosol-cloud interactions and its application to the parameterization of these interactions in climate models can be misleading. The understanding of feedbacks between microphysics and dynamics induced by aerosol changes and their parameterization can be critical to the correct assessment of the effect of aerosols on clouds and climate.
  • What can we learn about ship emission inventories from measurements of air pollutants over the Mediterranean Sea?

    Ship emission estimates diverge widely for all chemical compounds for several reasons: use of different methodologies (bottom-up or top-down), activity data and emission factors can easily result in a difference ranging from a factor of 1.5 to even an order of magnitude. Combining three sets of observational data – ozone and black carbon measurements sampled at three coastal sites and on board of a Mediterranean cruise ship, as well as satellite observations of atmospheric NO<sub>2</sub> column concentration over the same area – we assess the accuracy of the three most commonly used ship emission inventories, EDGAR FT (Olivier et al., 2005), emissions described by Eyring et al. (2005) and emissions reported by EMEP (Vestreng et al., 2007). Our tool is a global atmospheric chemistry transport model which simulates the chemical state of the Mediterranean atmosphere applying different ship emission inventories. The simulated contributions of ships to air pollutant levels in the Mediterranean atmosphere are significant but strongly depend on the inventory applied. Close to the major shipping routes relative contributions vary from 10 to 50% for black carbon and from 2 to 12% for ozone in the surface layer, as well as from 5 to 20% for nitrogen dioxide atmospheric column burden. The relative contributions are still significant over the North African coast, but less so over the South European coast because densely populated regions with significant human activity contribute relatively more to air pollution than ships, even if these regions attract a lot of ship traffic. The observations poorly constrain the ship emission inventories in the Eastern Mediterranean where the influence of uncertain land based emissions, the model transport and wet deposition are at least as important as the signal from ships. In the Western Mediterranean, the regional EMEP emission inventory gives the best match with most measurements, followed by Eyring for NO<sub>2</sub> and ozone and by EDGAR for black carbon. Given the uncertainty of the measurements and the model, each of the three emission inventories could actually be right, implying that large uncertainties in ship emissions need to be considered for future scenario analysis.
  • Evidence for ice particles in the tropical stratosphere from in-situ measurements

    In-situ ice crystal size distribution measurements are presented within the tropical troposphere and lower stratosphere. The measurements were performed using a combination of a Forward Scattering Spectrometer Probe (FSSP-100) and a Cloud Imaging Probe (CIP), which were installed on the Russian high altitude research aircraft M55 "Geophysica" during the SCOUT-O<sub>3</sub> campaign in Darwin, Australia. One of the objectives of the campaign was to characterise the Hector convective system, which appears on an almost daily basis during the pre-monsoon season over the Tiwi Islands, north of Darwin. In total 90 encounters with ice clouds, between 10 and 19 km altitude were selected from the dataset and were analysed. Six of these encounters were observed in the lower stratosphere, up to 1.4 km above the local tropopause. Concurrent lidar measurements on board "Geophysica" indicate that these ice clouds were a result of overshooting convection. Large ice crystals, with a maximum dimension up to 400 μm, were observed in the stratosphere. The stratospheric ice clouds included an ice water content ranging from 7.7&times;10<sup>&minus;5</sup> to 8.5&times;10<sup>&minus;4</sup> g m<sup>&minus;3</sup> and were observed at ambient relative humidities (with respect to ice) between 75 and 157%. Three modal lognormal size distributions were fitted to the average size distributions for different potential temperature intervals, showing that the shape of the size distribution of the stratospheric ice clouds are similar to those observed in the upper troposphere. <br><br> In the tropical troposphere the effective radius of the ice cloud particles decreases from 100 μm at about 10 km altitude, to 3 μm at the tropopause, while the ice water content decreases from 0.04 to 10<sup>&minus;5</sup> g m<sup>&minus;3</sup>. No clear trend in the number concentration was observed with altitude, due to the thin and inhomogeneous characteristics of the observed cirrus clouds. <br><br> The ice water content calculated from the observed ice crystal size distribution is compared to the ice water content derived from two hygrometer instruments. This independent measurement of the ice water content agrees within the combined uncertainty of the instruments for ice water contents exceeding 3&times;10<sup>&minus;4</sup>g m<sup>&minus;3</sup>. <br><br> Stratospheric residence times, calculated based on gravitational settling, and evaporation rates show that the ice crystals observed in the stratosphere over the Hector storm system had a high potential of humidifying the stratosphere locally. <br><br> Utilizing total aerosol number concentration measurements from a four channel condensation particle counter during two separate campaigns, it can be shown that the fraction of ice particles to the number of aerosol particles remaining ranges from 1:300 to 1:30 000 for tropical upper tropospheric ice clouds with ambient temperatures below &minus;75&deg;C.
  • A comparison study of regional atmospheric simulations with an elastic backscattering Lidar and sunphotometry in an urban area

    We describe a comparison study of Aerosol Optical Thickness (AOT) from numerical simulations using a regional atmospheric model with an elastic backscattering lidar operating at 532 nm and a sunphotometer belonging to the AERONET network at São Paulo (23&deg; S 46&deg; W) city, Brazil, a very populated urban area. The atmospheric model includes an aerosol emission, transport and deposition module coupled to a radiative transfer parameterization, which takes the interaction between aerosol particles and short and long wave radiation into account. A period of one week was taken as case study during the dry season (late August) when intense biomass burning activities occur at remote areas in South America, and meteorological conditions disfavor the pollution dispersion in the city of São Paulo. The situation presented here showed how smoke from biomass burning in remote areas is transported to the south-east part of Brazil and affects the optical atmospheric conditions in São Paulo. The numerical simulations are corroborated by in situ measurements of AOT obtained by lidar and sun photometry.
  • An operational system for the assimilation of the satellite information on wild-land fires for the needs of air quality modelling and forecasting

    This paper investigates a potential of two remotely sensed wild-land fire characteristics: 4-&mu;m Brightness Temperature Anomaly (TA) and Fire Radiative Power (FRP) for the needs of operational chemical transport modelling and short-term forecasting of atmospheric composition and air quality. The treatments of the TA and FRP data are presented and a methodology for evaluating the emission fluxes of primary aerosols (PM<sub>2.5</sub> and total PM) is described. The method does not include the complicated analysis of vegetation state, fuel load, burning efficiency and related factors, which are uncertain but inevitably involved in approaches based on burnt-area scars or similar products. The core of the current methodology is based on the empirical emission factors that are used to convert the observed temperature anomalies and fire radiative powers into emission fluxes. These factors have been derived from the analysis of several fire episodes in Europe (28.4–5.5.2006, 15.8–25.8.2006 and in August 2008). These episodes were characterised by: (i) well-identified FRP and TA values, and (ii) available ground-based observations of aerosol concentrations, and optical thickness for the regions where the contribution of the fire smoke to the concentrations of PM<sub>2.5</sub> was dominant, in comparison with those of other pollution sources. The emission factors were determined separately for the forested and grassland areas; in case of mixed-type land use, an intermediate scaling was assumed. Despite significant differences between the TA and FRP methodologies, an accurate non-linear fitting was found between the predictions of these approaches. The agreement was comparatively weak only for small fires, for which the accuracy of both products is expected to be low. The applications of the Fire Assimilation System (FAS) in combination with the dispersion model SILAM showed that both the TA and FRP products are suitable for the evaluation of the emission fluxes from wild-land fires. The fire-originated concentrations of aerosols (PM<sub>2.5</sub>, PM<sub>10</sub>, sulphates and nitrates) and AOD, as predicted by the SILAM model were mainly within a factor of 2–3 compared with the observations. The main challenges of the FAS improvement include refining of the emission factors globally, determination of the types of fires (smouldering vs flaming), evaluation of the injection heights of the plumes, and predicting the temporal evolution of fires.
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