<?xml version="1.0" encoding="utf-8"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns="http://purl.org/rss/1.0/" xmlns:dc="http://purl.org/dc/elements/1.1/"><channel rdf:about="http://www.atmos-chem-phys.net/xml/rss1_0.xml"><title>ACP - Latest Articles</title><link>http://www.atmos-chem-phys.net/</link><description>Atmospheric Chemistry and Physics Latest Articles</description><items><rdf:Seq><rdf:li resource="http://www.atmos-chem-phys.net/13/5227/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5205/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5189/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5173/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5163/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5151/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5137/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5117/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5103/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5089/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5063/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5049/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5033/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/5017/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4997/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4983/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4963/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4941/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4917/2013/" /><rdf:li resource="http://www.atmos-chem-phys.net/13/4907/2013/" /></rdf:Seq></items></channel><item rdf:about="http://www.atmos-chem-phys.net/13/5227/2013/"><title>Global impact of smoke aerosols from landscape fires on climate and the Hadley circulation</title><link>http://www.atmos-chem-phys.net/13/5227/2013/</link><description>&lt;b&gt;Global impact of smoke aerosols from landscape fires on climate and the Hadley circulation&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5227-5241, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. G. Tosca, J. T. Randerson, and C. S. Zender&lt;br /&gt;&lt;br /&gt;Each year landscape fires across the globe emit black and organic carbon
smoke particles that can last in the atmosphere for days to weeks. We
characterized the climate response to these aerosols using an Earth system
model. We used remote sensing observations of aerosol optical depth (AOD) and
simulations from the Community Atmosphere Model, version 5 (CAM5) to optimize
satellite-derived smoke emissions for high biomass burning regions.
Subsequent global simulations using the adjusted fire emissions produced AODs
that were in closer agreement with surface and space-based measurements. We
then used CAM5, which included radiative aerosol effects, to evaluate the
climate response to the fire-aerosol forcing. We conducted two 52 yr
simulations, one with four sets of monthly cycling 1997–2009 fire emissions
and one without. Fire emissions increased global mean annual AOD by 10%
(+0.02) and decreased net all-sky surface radiation by 1% (1.3 W m&lt;sup&gt;−2&lt;/sup&gt;).
Elevated AODs reduced global surface temperatures by 0.13 &amp;pm; 0.01 &amp;deg;C.
Though global precipitation declined only slightly, patterns of precipitation
changed, with large reductions near the Equator offset by smaller increases
north and south of the intertropical convergence zone (ITCZ). A combination
of increased tropospheric heating and reduced surface temperatures increased
equatorial subsidence and weakened the Hadley circulation. As a consequence,
precipitation decreased over tropical forests in South America, Africa and
equatorial Asia. These results are consistent with the observed correlation
between global temperatures and the strength of the Hadley circulation and
studies linking tropospheric heating from black carbon aerosols with tropical
expansion.</description><dc:date>2013-05-24T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5205/2013/"><title>35 yr of stratospheric aerosol measurements at Garmisch-Partenkirchen: from Fuego to Eyjafjallajökull, and beyond</title><link>http://www.atmos-chem-phys.net/13/5205/2013/</link><description>&lt;b&gt;35 yr of stratospheric aerosol measurements at Garmisch-Partenkirchen: from Fuego to Eyjafjallajökull, and beyond&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5205-5225, 2013&lt;br /&gt;&lt;br /&gt;Author(s): T. Trickl, H. Giehl, H. Jäger, and H. Vogelmann&lt;br /&gt;&lt;br /&gt;Lidar measurements at Garmisch-Partenkirchen (Germany) have almost
continually delivered backscatter coefficients of stratospheric aerosol
since 1976. The time series is dominated by signals from the particles
injected into or formed in the stratosphere due to major volcanic eruptions,
in particular those of El Chichon (Mexico, 1982) and Mt Pinatubo
(Philippines, 1991). Here, we focus more on the long-lasting background
period since the late 1990s and 2006, in view of processes maintaining a
residual lower-stratospheric aerosol layer in absence of major eruptions, as
well as the period of moderate volcanic impact afterwards. During the long
background period the stratospheric backscatter coefficients reached a level
even below that observed in the late 1970s. This suggests that the predicted
potential influence of the strongly growing air traffic on the stratospheric
aerosol loading is very low. Some correlation may be found with single
strong forest-fire events, but the average influence of biomass burning
seems to be quite limited. No positive trend in background aerosol can be
resolved over a period as long as that observed by lidar at Mauna Loa. We
conclude that the increase of our integrated backscatter coefficients
starting in 2008 is mostly due to volcanic eruptions with explosivity index
4, penetrating strongly into the stratosphere. Most of them occurred in the
mid-latitudes. A key observation for judging the role of eruptions just
reaching the tropopause region was that of the plume from the Icelandic
volcano Eyjafjallajökull above Garmisch-Partenkirchen (April 2010) due
to the proximity of that source. The top altitude of the ash above the
volcano was reported just as 9.3 km, but the lidar measurements revealed
enhanced stratospheric aerosol up to 14.3 km. Our analysis suggests for two
or three of the four measurement days the presence of a stratospheric
contribution from Iceland related to quasi-horizontal transport, differing
from the strong descent of the layers entering Central Europe at low
altitudes. The backscatter coefficients within the first 2 km above the
tropopause exceed the stratospheric background by a factor of four to five.
In addition, Asian and Saharan dust layers were identified in the free
troposphere, Asian dust most likely even in the stratosphere.</description><dc:date>2013-05-24T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5189/2013/"><title>High-resolution mapping of combustion processes and implications for CO&lt;sub&gt;2&lt;/sub&gt; emissions</title><link>http://www.atmos-chem-phys.net/13/5189/2013/</link><description>&lt;b&gt;High-resolution mapping of combustion processes and implications for CO&lt;sub&gt;2&lt;/sub&gt; emissions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5189-5203, 2013&lt;br /&gt;&lt;br /&gt;Author(s): R. Wang, S. Tao, P. Ciais, H. Z. Shen, Y. Huang, H. Chen, G. F. Shen, B. Wang, W. Li, Y. Y. Zhang, Y. Lu, D. Zhu, Y. C. Chen, X. P. Liu, W. T. Wang, X. L. Wang, W. X. Liu, B. G. Li, and S. L. Piao&lt;br /&gt;&lt;br /&gt;High-resolution mapping of fuel combustion and CO&lt;sub&gt;2&lt;/sub&gt; emission provides
valuable information for modeling pollutant transport, developing mitigation
policy, and for inverse modeling of CO&lt;sub&gt;2&lt;/sub&gt; fluxes. Previous global emission
maps included only few fuel types, and emissions were estimated on a grid by
distributing national fuel data on an equal per capita basis, using
population density maps. This process distorts the geographical distribution
of emissions within countries. In this study, a sub-national disaggregation
method (SDM) of fuel data is applied to establish a global
0.1&amp;deg; × 0.1&amp;deg; geo-referenced inventory of fuel
combustion (PKU-FUEL) and corresponding CO&lt;sub&gt;2&lt;/sub&gt; emissions (PKU-CO&lt;sub&gt;2&lt;/sub&gt;)
based upon 64 fuel sub-types for the year 2007. Uncertainties of the emission
maps are evaluated using a Monte Carlo method. It is estimated that CO&lt;sub&gt;2&lt;/sub&gt;
emission from combustion sources including fossil fuel, biomass, and solid
wastes in 2007 was 11.2 Pg C yr&lt;sup&gt;−1&lt;/sup&gt; (9.1 Pg C yr&lt;sup&gt;−1&lt;/sup&gt; and 13.3 Pg
C yr&lt;sup&gt;−1&lt;/sup&gt; as 5th and 95th percentiles). Of this, emission from fossil fuel
combustion is 7.83 Pg C yr&lt;sup&gt;−1&lt;/sup&gt;, which is very close to the estimate of
the International Energy Agency (7.87 Pg C yr&lt;sup&gt;−1&lt;/sup&gt;). By replacing
national data disaggregation with sub-national data in this study, the
average 95th minus 5th percentile ranges of CO&lt;sub&gt;2&lt;/sub&gt; emission for all grid
points can be reduced from 417 to 68.2 Mg km&lt;sup&gt;−2&lt;/sup&gt; yr&lt;sup&gt;−1&lt;/sup&gt;. The spread
is reduced because the uneven distribution of per capita fuel consumptions
within countries is better taken into account by using sub-national fuel
consumption data directly. Significant difference in per capita CO&lt;sub&gt;2&lt;/sub&gt;
emissions between urban and rural areas was found in developing countries
(2.08 vs. 0.598 Mg C/(cap. × yr)), but not in developed countries
(3.55 vs. 3.41 Mg C/(cap. × yr)). This implies that rapid
urbanization of developing countries is very likely to drive up their
emissions in the future.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5173/2013/"><title>Source apportionment of fine PM and sub-micron particle number concentrations at a regional background site in the western Mediterranean: a 2.5 year study</title><link>http://www.atmos-chem-phys.net/13/5173/2013/</link><description>&lt;b&gt;Source apportionment of fine PM and sub-micron particle number concentrations at a regional background site in the western Mediterranean: a 2.5 year study&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5173-5187, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Cusack, N. Pérez, J. Pey, A. Alastuey, and X. Querol&lt;br /&gt;&lt;br /&gt;The chemical composition and sources of ambient fine particulate matter
(PM&lt;sub&gt;1&lt;/sub&gt;) over a period of 2.5 years for a regional background site in the
western Mediterranean are presented in this work. Furthermore, sub-micron
particle number concentrations and the sources of these particles are also
presented. The mean PM&lt;sub&gt;1&lt;/sub&gt; concentration for the measurement period was
8.9 μg m&lt;sup&gt;−3&lt;/sup&gt;, with organic matter (OM) and sulphate comprising
most of the mass (3.2 and 1.5 μg m&lt;sup&gt;−3&lt;/sup&gt; respectively). Six sources
were identified in PM&lt;sub&gt;1&lt;/sub&gt; by Positive Matrix Factorisation (PMF): secondary
organic aerosol, secondary nitrate, industrial, traffic + biomass burning,
fuel oil combustion and secondary sulphate. Typically anthropogenic sources
displayed elevated concentrations during the week with reductions at
weekends. Nitrate levels were elevated in winter and negligible in summer,
whereas secondary sulphate levels underwent a contrasting seasonal evolution
with highest concentrations in summer, similar to the fuel oil combustion
source. The SOA source was influenced by episodes of sustained pollution as
a result of anticyclonic conditions occurring during winter, giving rise to
thermal inversions and the accumulation of pollutants in the mixing layer.
Increased levels in summer were owing to higher biogenic emissions and
regional recirculation of air masses. The industrial source decreased in
August due to decreased emissions during the vacation period. Increases in
the traffic + biomass burning source were recorded in January, April and
October, which were attributed to the occurrence of the aforementioned
pollution episodes and local biomass burning emission sources, which include
agriculture and domestic heating systems. Average particle number
concentrations (N&lt;sub&gt;9-825 nm&lt;/sub&gt;) from 5/11/2010 to 01/06/2011 and from
15/10/2011 to 18/12/2011 reached 3097 cm&lt;sup&gt;−3&lt;/sup&gt;. Five emission sources of
particle of sub-micron particles were determined by Principal Component
Analysis (PCA); industrial + traffic + biomass burning, new particle
formation + growth, secondary sulphate + fuel oil combustion, crustal
material and secondary nitrate. The new particle formation + growth source
dominated the particle number concentration (56% of total particle number
concentration), especially for particles &lt; 100 nm, followed by
industrial + traffic + biomass burning (13%). Secondary sulphate +
fuel oil combustion (8%), nitrate (9%) and crustal material (2%)
were dominant for particles of larger diameter (&gt; 100 nm) and
thus did not influence the particle number concentration significantly.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5163/2013/"><title>Extreme winds over Europe in the ENSEMBLES regional climate models</title><link>http://www.atmos-chem-phys.net/13/5163/2013/</link><description>&lt;b&gt;Extreme winds over Europe in the ENSEMBLES regional climate models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5163-5172, 2013&lt;br /&gt;&lt;br /&gt;Author(s): S. D. Outten and I. Esau&lt;br /&gt;&lt;br /&gt;Extreme winds cause vast amounts of damage every year and represent a major
concern for numerous industries including construction, afforestation, wind
energy and many others. Under a changing climate, the intensity and
frequency of extreme events are expected to change, and accurate projections
of these changes will be invaluable to decision makers and society as a
whole. This work examines four regional climate model downscalings over
Europe following the SRES A1B scenario from the &quot;ENSEMBLE-based Predictions
of Climate Changes and their Impacts&quot; project (ENSEMBLES). It investigates
the projected changes in the 50 yr return wind speeds and the associated
uncertainties. This is accomplished by employing the peaks-over-threshold
method with the use of the generalised Pareto distribution. The models show
that, for much of Europe, the 50 yr return wind is projected to change by
less than 2 m s&lt;sup&gt;−1&lt;/sup&gt;, while the uncertainties associated with the
statistical estimates are larger than this. In keeping with previous works
in this field, the largest source of uncertainty is found to be the
inter-model spread, with some locations showing differences in the 50 yr
return wind of over 20 m s&lt;sup&gt;−1&lt;/sup&gt; between two different downscalings.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5151/2013/"><title>The temporal evolution of three-dimensional lightning parameters and their suitability for thunderstorm tracking and nowcasting</title><link>http://www.atmos-chem-phys.net/13/5151/2013/</link><description>&lt;b&gt;The temporal evolution of three-dimensional lightning parameters and their suitability for thunderstorm tracking and nowcasting&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5151-5161, 2013&lt;br /&gt;&lt;br /&gt;Author(s): V. K. Meyer, H. Höller, and H. D. Betz&lt;br /&gt;&lt;br /&gt;Total lightning (TL) data have been found to provide valuable information
       about the internal dynamics of a thunderstorm allowing
      conclusions about its further development as well as indicating potential
      of thunderstorm-related severe weather at the
      ground. This paper investigates electrical discharge correlations of strokes and
       flashes with respect to the temporal evolution
      of thunderstorms in case studies as well as by statistical means. The recently
      developed algorithm li-TRAM  (tracking and monitoring of lightning cells, 
Meyer et al., 2013)  has been employed to track and monitor
       thunderstorms based on three-dimensionally
      resolved TL data provided as stroke events by the European lightning
      location network LINET. From statistical investigation of 
863 suited thunderstorm life cycles, the cell area turned out
       to correlate well with (a) the total discharge
      rate, (b) the in-cloud (IC) discharge rate, and (c) the mean IC discharge height
       per lightning cell as identified by
      li-TRAM. All three parameter correlations consistently show an abrupt change in
       discharge characteristics around a cell area of
      170 km&lt;sup&gt;2&lt;/sup&gt;. Statistical investigations supported by the comparison of
      three case studies – selected to represent
      a single storm, a multi-cell and a supercell – strongly suggest that the
      correlation functions include the temporal evolution
      as well as the storm type. With the help of volumetric radar data, it can
      also be suggested that the well-defined break
      observed at 170 km&lt;sup&gt;2&lt;/sup&gt; marks the region where the transition occurs
       from short-lived and rather simple structured
      single storm cells to better organized, more persistent, and more complex
      structured thunderstorm forms, e.g. multi-cells and
      supercells. All three storm types experience similar discharge characteristics
       during their growing and dissipating
      phases. However, while the poorly organized and short-lived cells preferentially
       remain small during a short mature phase,
      mainly the more persistent thunderstorm types develop to sizes above
170 km&lt;sup&gt;2&lt;/sup&gt; during a pronounced mature stage. At
      that stage they exhibit on average higher discharge rates at higher altitudes as
       compared with matured single cells. With the
      maximum stroke distance set to 10 km and a flash duration set to
      1 s, the parameterization functions found
      for the stroke rate as a function of the cell area have been transformed to a flash
       rate. The presented study suggests that, with
      respect to the storm type, stroke and flash correlations can be parameterized.
      There is also strong evidence that
      parameterization functions include the time parameter, so that altogether TL
      stroke information has good potential to pre-estimate the further evolution (nowcast) of a currently observed storm in
       an object-oriented thunderstorm nowcasting approach.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5137/2013/"><title>Automated thunderstorm tracking: utilization of three-dimensional lightning and radar data</title><link>http://www.atmos-chem-phys.net/13/5137/2013/</link><description>&lt;b&gt;Automated thunderstorm tracking: utilization of three-dimensional lightning and radar data&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5137-5150, 2013&lt;br /&gt;&lt;br /&gt;Author(s): V. K. Meyer, H. Höller, and H. D. Betz&lt;br /&gt;&lt;br /&gt;This paper presents a new hybrid method for automated thunderstorm
observation by tracking and monitoring of electrically charged cells
(ec-TRAM). The developed algorithm combines information about intense ground
precipitation derived from low-level radar-reflectivity scans with
three-dimensionally resolved lightning data, which are provided by the
European VLF/LF lightning detection network LINET. Based on the already
existing automated radar tracker rad-TRAM  (Kober and Tafferner, 2009), the new method
li-TRAM identifies and tracks electrically active regions in thunderclouds
using lightning data only. The algorithm ec-TRAM uses the output of the two
autonomously operating routines rad-TRAM and li-TRAM in order to assess,
track, and monitor a more comprehensive picture of thunderstorms. The main
motivation of this work is to assess the benefit of three-dimensionally
resolved total lightning (TL) information for thunderstorm tracking and
monitoring. The focus is laid on the temporal development whereby TL is
characterized by an effective in-cloud (IC) and cloud-to-ground (CG)
event discrimination. It is found that the algorithms li-TRAM and ec-TRAM are
both feasible methods for thunderstorm monitoring with potential for
nowcasting. The tracking performance of li-TRAM turns out to be comparable to
that of rad-TRAM, a result that strongly encourages utilization of lightning
data as independent data source for thunderstorm tracking. It is found that
lightning data allow an accurate and close monitoring of storm regions with
intense internal dynamics as soon as convection induces electrical activity.
A case study shows that the current short-term storm dynamics are clearly
reflected in the amount of strokes, change of stroke rates and IC/CG ratio.
The hybrid method ec-TRAM outperforms rad-TRAM and li-TRAM regarding
reliability and continuous assessment of storm tracks especially in more
complexly developing storms, where the use of discharge information
contributes to more detailed information about storm stage and storm
evolution.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5117/2013/"><title>Dissolved organic carbon (DOC) and select aldehydes in cloud and fog water: the role of the aqueous phase in impacting trace gas budgets</title><link>http://www.atmos-chem-phys.net/13/5117/2013/</link><description>&lt;b&gt;Dissolved organic carbon (DOC) and select aldehydes in cloud and fog water: the role of the aqueous phase in impacting trace gas budgets&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5117-5135, 2013&lt;br /&gt;&lt;br /&gt;Author(s): B. Ervens, Y. Wang, J. Eagar, W. R. Leaitch, A. M. Macdonald, K. T. Valsaraj, and P. Herckes&lt;br /&gt;&lt;br /&gt;Cloud and fog droplets efficiently scavenge and process water-soluble
compounds and, thus, modify the chemical composition of the gas and particle
phases. The concentrations of dissolved organic carbon (DOC) in the aqueous
phase reach concentrations on the order of ~ 10 mgC L&lt;sup&gt;−1&lt;/sup&gt;
which is typically on the same order of magnitude as the sum of inorganic
anions. Aldehydes and carboxylic acids typically comprise a large fraction
of DOC because of their high solubility. The dissolution of species in the
aqueous phase can lead to (i) the removal of species from the gas phase
preventing their processing by gas phase reactions (e.g., photolysis of
aldehydes) and (ii) the formation of unique products that do not have any
efficient gas phase sources (e.g., dicarboxylic acids).
&lt;br&gt;&lt;br&gt;
We present measurements of DOC and select aldehydes in fog water at high
elevation and intercepted clouds at a biogenically-impacted location
(Whistler, Canada) and in fog water in a more polluted area (Davis, CA).
Concentrations of formaldehyde, glyoxal and methylglyoxal were in the
micromolar range and comprised &amp;le; 2% each individually of the DOC.
Comparison of the DOC and aldehyde concentrations to those at other
locations shows good agreement and reveals highest levels for both in
anthropogenically impacted regions. Based on this overview, we conclude that
the fraction of organic carbon (dissolved and insoluble inclusions) in the
aqueous phase of clouds or fogs, respectively, comprises 2–~ 40%
of total organic carbon. Higher values are observed to be associated
with aged air masses where organics are expected to be more highly oxidised
and, thus, more soluble. Accordingly, the aqueous/gas partitioning ratio
expressed here as an effective Henry's law constant for DOC
(&lt;i&gt;K&lt;/i&gt;&lt;sub&gt;H&lt;/sub&gt;*&lt;sup&gt;DOC&lt;/sup&gt;) increases by an order of magnitude from
7 × 10&lt;sup&gt;3&lt;/sup&gt; M atm&lt;sup&gt;−1&lt;/sup&gt; to 7 × 10&lt;sup&gt;4&lt;/sup&gt; M atm&lt;sup&gt;−1&lt;/sup&gt; during the
ageing of air masses.
&lt;br&gt;&lt;br&gt;
The measurements are accompanied by photochemical box model simulations.
These simulations are used to contrast two scenarios, i.e., an
anthropogenically vs. a more biogenically impacted one as being
representative for Davis and Whistler, respectively. Since the simplicity of
the box model prevents a fully quantitative prediction of the observed
aldehyde concentrations, we rather use the model results to compare trends
in aldehyde partitioning and ratios.  They suggest that the scavenging of
aldehydes by the aqueous phase can reduce HO&lt;sub&gt;2&lt;/sub&gt; gas phase levels
significantly by two orders of magnitude due to a weaker net source of
HO&lt;sub&gt;2&lt;/sub&gt; production from aldehyde photolysis in the gas phase. Despite the
high solubility of dicarbonyl compounds (glyoxal, methylglyoxal), their
impact on the HO&lt;sub&gt;2&lt;/sub&gt; budget by scavenging is &lt; 10% of that of
formaldehyde. The overview of DOC and aldehyde measurements presented here
reveals that clouds and fogs can be efficient sinks for organics, with
increasing importance in aged air masses. Even though aldehydes,
specifically formaldehyde, only comprise ~ 1% of DOC, their
scavenging and processing in the aqueous phase might translate into
significant effects in the oxidation capacity of the atmosphere.</description><dc:date>2013-05-21T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5103/2013/"><title>Evaluation of seasonal atmosphere–biosphere exchange estimations with TCCON measurements</title><link>http://www.atmos-chem-phys.net/13/5103/2013/</link><description>&lt;b&gt;Evaluation of seasonal atmosphere–biosphere exchange estimations with TCCON measurements&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5103-5115, 2013&lt;br /&gt;&lt;br /&gt;Author(s): J. Messerschmidt, N. Parazoo, D. Wunch, N. M. Deutscher, C. Roehl, T. Warneke, and P. O. Wennberg&lt;br /&gt;&lt;br /&gt;We evaluate three estimates of the atmosphere-biosphere exchange against
total column CO&lt;sub&gt;2&lt;/sub&gt; observations from the Total Carbon Column Observing
Network (TCCON). Using the GEOS-Chem transport model, we produce forward
simulations of atmospheric CO&lt;sub&gt;2&lt;/sub&gt; concentrations for the 2006–2010 time
period using the Carnegie-Ames-Stanford Approach (CASA), the Simple Biosphere
(SiB) and the GBiome-BGC models. Large differences in the CO&lt;sub&gt;2&lt;/sub&gt;
simulations result from the choice of the atmosphere-biosphere model. We
evaluate the seasonal cycle phase, amplitude and shape of the simulations.
The version of CASA currently used as the a priori model by the GEOS-Chem
carbon cycle community poorly represents the season cycle in total column
CO&lt;sub&gt;2&lt;/sub&gt;. Consistent with earlier studies, enhancing the CO&lt;sub&gt;2&lt;/sub&gt; uptake in
the boreal forest and shifting the onset of the growing season earlier
significantly improve the simulated seasonal CO&lt;sub&gt;2&lt;/sub&gt; cycle using CASA
estimates. The SiB model gives a better representation of the seasonal cycle
dynamics. The difference in the seasonality of net ecosystem exchange (NEE)
between these models is not the absolute gross primary productivity (GPP),
but rather the differential phasing of ecosystem respiration (RE) with
respect to GPP between these models.</description><dc:date>2013-05-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5089/2013/"><title>Effects of internal mixing and aggregate morphology on optical properties of black carbon using a discrete dipole approximation model</title><link>http://www.atmos-chem-phys.net/13/5089/2013/</link><description>&lt;b&gt;Effects of internal mixing and aggregate morphology on optical properties of black carbon using a discrete dipole approximation model&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5089-5101, 2013&lt;br /&gt;&lt;br /&gt;Author(s): B. V. Scarnato, S. Vahidinia, D. T. Richard, and T. W. Kirchstetter&lt;br /&gt;&lt;br /&gt;According to recent studies, internal mixing of black carbon (BC) with other
aerosol materials in the atmosphere alters its aggregate shape, absorption of
solar radiation, and radiative forcing. These mixing state effects are not
yet fully understood. In this study, we characterize the morphology and
mixing state of bare BC and BC internally mixed with sodium chloride (NaCl)
using electron microscopy and examine the sensitivity of optical properties
to BC mixing state and aggregate morphology using a discrete dipole
approximation model (DDSCAT). DDSCAT is flexible in simulating the geometry
and refractive index of particle aggregates. DDSCAT predicts a higher mass
absorption coefficient (MAC), lower single scattering albedo (SSA), and
higher absorption Angstrom exponent (AAE) for bare BC aggregates that are
lacy rather than compact. Predicted values of SSA at 550 nm range between
0.16 and 0.27 for lacy and compact aggregates, respectively, in agreement
with reported experimental values of 0.25 ± 0.05. The variation in
absorption with wavelength does not adhere precisely to a power law
relationship over the 200 to 1000 nm range. Consequently, AAE values depend
on the wavelength region over which they are computed. The MAC of BC
(averaged over the 200–1000 nm range) is amplified when internally mixed
with NaCl (100–300 nm in radius) by factors ranging from 1.0 for lacy BC
aggregates partially immersed in NaCl to 2.2 for compact BC aggregates fully
immersed in NaCl. The SSA of BC internally mixed with NaCl is higher than for
bare BC and increases with the embedding in the NaCl. Internally mixed BC SSA
values decrease in the 200–400 nm wavelength range, a feature also common
to the optical properties of dust and organics. Linear polarization features
are also predicted in DDSCAT and are dependent on particle size and
morphology.
&lt;br&gt;&lt;br&gt;
This study shows that DDSCAT predicts complex morphology and mixing state
dependent aerosol optical properties that have been reported previously and
are relevant to radiative transfer, climate modeling, and interpretation of
remote sensing measurements.</description><dc:date>2013-05-16T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5063/2013/"><title>Singular vector decomposition for sensitivity analyses of tropospheric chemical scenarios</title><link>http://www.atmos-chem-phys.net/13/5063/2013/</link><description>&lt;b&gt;Singular vector decomposition for sensitivity analyses of tropospheric chemical scenarios&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5063-5087, 2013&lt;br /&gt;&lt;br /&gt;Author(s): N. Goris and H. Elbern&lt;br /&gt;&lt;br /&gt;Observations of the chemical state of the atmosphere typically provide only
sparse snapshots of the state of the system due to their insufficient
temporal and spatial density. One possibility for optimisation of the state
estimate is to target the observation of those parameters that have the
largest potential of resulting in forecast improvements. In the present work,
the technique of singular vector analysis is applied to atmospheric chemical
modelling in order to identify the most sensitive chemical compounds during a
given time period and prioritise them for measurement. Novel to the current
work is the fact that, in the application of singular vector analysis, not
only the initial values but also the emissions are considered as target
variables for adaptive observation strategies. This specific application of
singular vector analysis is studied in the context of a chemistry box model
allowing for validation of its new features for two chemical regimes. The
time and regime dependence of the ozone (O&lt;sub&gt;3&lt;/sub&gt;) and peroxyacetyl nitrate
(PAN) formation potential of individual volatile organic compounds (VOCs) is
investigated. Results show that the combined sensitivity of O&lt;sub&gt;3&lt;/sub&gt; and PAN to
individual VOCs is strongly dependent on the photochemical scenario and
simulation interval used. Particularly the alkanes show increasing
sensitivities with increasing simulation length. Classifying the VOCs as being of
high, medium, little or negligible importance for the formation of
O&lt;sub&gt;3&lt;/sub&gt; and PAN allows for the identification of those VOCs that may be omitted
from measurement. We find that it is possible to omit 6 out of 18 VOCs
considered for initial value measurement and 4 out of 12 VOCs considered for
emission measurement. The omission of these VOCs is independent of
photochemical regime and simulation length. The VOCs selected for measuring
account for more than 96% and 90% of the O&lt;sub&gt;3&lt;/sub&gt; and PAN sensitivity to
VOCs, respectively.</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5049/2013/"><title>Aerosol mixing state, hygroscopic growth and cloud activation efficiency during MIRAGE 2006</title><link>http://www.atmos-chem-phys.net/13/5049/2013/</link><description>&lt;b&gt;Aerosol mixing state, hygroscopic growth and cloud activation efficiency during MIRAGE 2006&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5049-5062, 2013&lt;br /&gt;&lt;br /&gt;Author(s): S. Lance, T. Raatikainen, T. B. Onasch, D. R. Worsnop, X.-Y. Yu, M. L. Alexander, M. R. Stolzenburg, P. H. McMurry, J. N. Smith, and A. Nenes&lt;br /&gt;&lt;br /&gt;Observations of aerosol hygroscopic growth and CCN activation spectra for
submicron particles are reported for the T1 ground site outside of Mexico
City during the MIRAGE 2006 campaign. &lt;i&gt;κ&lt;/i&gt;-Köhler theory is used to
evaluate the characteristic hygroscopicity parameter, &amp;kappa;*, for the
CCN active aerosol population using both size-resolved HTMDA and
size-resolved CCNc measurements. Organic mass fractions
(&lt;i&gt;f&lt;/i&gt;&lt;sub&gt;org&lt;/sub&gt;) are evaluated from size-resolved aerosol mass
spectrometer (AMS) measurements, from which predictions of the hygroscopicity
parameter are compared against &amp;kappa;*.
&lt;br&gt;&lt;/br&gt;
Strong diurnal changes in aerosol water uptake parameters and aerosol
composition are observed. We find that new particle formation (NPF) events
are correlated with an increased &amp;kappa;* and CCN-active fraction during
the daytime, with greater impact on smaller particles. During NPF events, the
number concentration of 40 nm particles acting as CCN at 0.51% ± 0.06%
supersaturation can surpass by more than a factor of two the corresponding concentrations
of 100 nm particles. We also find that at
06:00–08:00 LT throughout the campaign, fresh traffic emissions
result in substantial changes to the chemical distribution of the aerosol,
with on average 65% externally mixed fraction for 40 nm particles and
30% externally mixed fraction for 100 nm particles, whereas at midday
nearly all particles of both sizes can be described as &quot;internally mixed&quot;.
&lt;br&gt;&lt;/br&gt;
Average activation spectra and growth factor distributions are analyzed for
different time periods characterizing the daytime (with and without NPF
events), the early morning &quot;rush hour&quot; and the entire campaign. We show
that &amp;kappa;* derived from CCNc measurements decreases as a function of
size during all time periods, while the CCN-active fraction increases as a
function of size. Size-resolved AMS measurements do not predict the observed
trend for &amp;kappa;* versus particle size, which can be attributed to
unresolved mixing state and the presence of refractory material not measured
by the AMS. Measured &amp;kappa;* typically ranges from 0.2 to 0.35, and
organics typically make up 60–85 % of the aerosol mass in the size range
studied. We show that &amp;kappa;&lt;sub&gt;AMS&lt;/sub&gt; is able to
describe CCN concentrations reasonably well, provided mixing-state
information is available, especially at the highest CCN concentrations. This
is consistent with other CCN studies carried out in urban environments, and
is partly due to the fact that the highest CCN concentrations occur during
the daytime when the aerosol is internally mixed. During the early
morning rush hour, however, failing to account for the aerosol mixing state results
in systematic overestimation of CCN concentrations by as much as 50–100%
on average.</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5033/2013/"><title>Stratospheric ozone interannual variability (1995–2011) as observed by lidar and satellite at Mauna Loa Observatory, HI and Table Mountain Facility, CA</title><link>http://www.atmos-chem-phys.net/13/5033/2013/</link><description>&lt;b&gt;Stratospheric ozone interannual variability (1995–2011) as observed by lidar and satellite at Mauna Loa Observatory, HI and Table Mountain Facility, CA&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5033-5047, 2013&lt;br /&gt;&lt;br /&gt;Author(s): G. Kirgis, T. Leblanc, I. S. McDermid, and T. D. Walsh&lt;br /&gt;&lt;br /&gt;The Jet Propulsion Laboratory (JPL) lidars, at the Mauna Loa Observatory,
Hawaii (MLO, 19.5° N, 155.6° W) and the JPL Table Mountain
Facility (TMF, California, 34.5° N, 117.7° W), have been
measuring vertical profiles of stratospheric ozone routinely since the early
1990's and late-1980s respectively. Interannual variability of ozone above
these two sites was investigated using a multi-linear regression analysis on
the deseasonalised monthly mean lidar and satellite time-series at 1 km
intervals between 20 and 45 km from January 1995 to April 2011, a period of
low volcanic aerosol loading. Explanatory variables representing the 11 yr
solar cycle, the El Niño Southern Oscillation, the Quasi-Biennial
Oscillation, the Eliassen-Palm flux, and horizontal and vertical transport
were used. A new proxy, the mid-latitude Ozone Depleting Gas Index, which
shows a decrease with time as an outcome of the Montreal Protocol, was
introduced and compared to the more commonly used linear trend method. The
analysis also compares the lidar time-series and a merged time-series
obtained from the space-borne Stratospheric Aerosol and Gas Experiment II,
Halogen Occultation Experiment, and Aura-Microwave Limb Sounder instruments.
&lt;br&gt;&lt;br&gt;
The results from both lidar and satellite measurements are consistent with
recent model simulations which propose changes in tropical upwelling.
Additionally, at TMF the Ozone Depleting Gas Index explains as much variance
as the Quasi-Biennial Oscillation in the upper stratosphere. Over the past 17 yr a diminishing downward trend in ozone was observed before 2000 and a net
increase, and sign of ozone recovery, is observed after 2005. Our results
which include dynamical proxies suggest possible coupling between horizontal
transport and the 11 yr solar cycle response, although a dataset spanning a
period longer than one solar cycle is needed to confirm this result.</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/5017/2013/"><title>Modeling organic aerosol from the oxidation of α-pinene in a Potential Aerosol Mass (PAM) chamber</title><link>http://www.atmos-chem-phys.net/13/5017/2013/</link><description>&lt;b&gt;Modeling organic aerosol from the oxidation of α-pinene in a Potential Aerosol Mass (PAM) chamber&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 5017-5031, 2013&lt;br /&gt;&lt;br /&gt;Author(s): S. Chen, W. H. Brune, A. T. Lambe, P. Davidovits, and T. B. Onasch&lt;br /&gt;&lt;br /&gt;A model has been developed to simulate the formation and evolution of
secondary organic aerosol (SOA) and was tested against data produced in a
Potential Aerosol Mass (PAM) flow reactor and a large environmental chamber.
The model framework is based on the two-dimensional volatility basis set
approach (2D-VBS), in which SOA oxidation products in the model are
distributed on the 2-D space of effective saturation concentration
(&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;&lt;i&gt;i&lt;/i&gt;&lt;/sub&gt;*) and oxygen-to-carbon ratio (O : C). The modeled organic
aerosol mass concentrations (&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;OA&lt;/sub&gt;) and O : C agree with laboratory
measurements within estimated uncertainties. However, while both measured
and modeled O : C increase with increasing OH exposure as expected, the
increase of modeled O : C is rapid at low OH exposure and then slows as OH
exposure increases while the increase of measured O : C is initially slow and
then accelerates as OH exposure increases. A global sensitivity analysis
indicates that modeled &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;OA&lt;/sub&gt; values are most sensitive to the assumed
values for the number of &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;&lt;i&gt;i&lt;/i&gt;&lt;/sub&gt;* bins, the heterogeneous OH
reaction rate coefficient, and the yield of first-generation products.
Modeled SOA O : C values are most sensitive to the assumed O : C of
first-generation oxidation products, the number of
&lt;i&gt;C&lt;/i&gt;&lt;sub&gt;&lt;i&gt;i&lt;/i&gt;&lt;/sub&gt;* bins, the heterogeneous OH reaction rate coefficient, and
the number of O : C bins. All these sensitivities vary as a function of OH
exposure. The sensitivity analysis indicates that the 2D-VBS model framework
may require modifications to resolve discrepancies between modeled and
measured O : C as a function of OH exposure.</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4997/2013/"><title>Characterization of urban aerosol in Cork city (Ireland) using aerosol mass spectrometry</title><link>http://www.atmos-chem-phys.net/13/4997/2013/</link><description>&lt;b&gt;Characterization of urban aerosol in Cork city (Ireland) using aerosol mass spectrometry&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4997-5015, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Dall'Osto, J. Ovadnevaite, D. Ceburnis, D. Martin, R. M. Healy, I. P. O'Connor, I. Kourtchev, J. R. Sodeau, J. C. Wenger, and C. O'Dowd&lt;br /&gt;&lt;br /&gt;Ambient wintertime background urban aerosol in Cork city, Ireland, was
characterized using aerosol mass spectrometry. During the three-week
measurement study in 2009, 93% of the ca. 1 350 000 single particles
characterized by an Aerosol Time-of-Flight Mass Spectrometer (TSI ATOFMS)
were classified into five organic-rich particle types, internally mixed to
different proportions with elemental carbon (EC), sulphate and nitrate,
while the remaining 7% was predominantly inorganic in nature.
Non-refractory PM&lt;sub&gt;1&lt;/sub&gt; aerosol was characterized using a High Resolution
Time-of-Flight Aerosol Mass Spectrometer (Aerodyne HR-ToF-AMS) and was also
found to comprise organic aerosol as the most abundant species (62%),
followed by nitrate (15%), sulphate (9%) and ammonium (9%), and
chloride (5%).
&lt;br&gt;&lt;br&gt;
Positive matrix factorization (PMF) was applied to the HR-ToF-AMS organic
matrix, and a five-factor solution was found to describe the variance in the
data well. Specifically, &quot;hydrocarbon-like&quot; organic aerosol (HOA) comprised
20% of the mass, &quot;low-volatility&quot; oxygenated organic aerosol (LV-OOA)
comprised 18%, &quot;biomass burning&quot; organic aerosol (BBOA) comprised
23%, non-wood solid-fuel combustion &quot;peat and coal&quot; organic aerosol
(PCOA) comprised 21%, and finally a species type characterized by primary
\textit{m/z}~peaks at 41 and 55, similar to previously reported &quot;cooking&quot;
organic aerosol (COA), but possessing different diurnal variations to what
would be expected for cooking activities, contributed 18%.
&lt;br&gt;&lt;br&gt;
Correlations between the different particle types obtained by the two
aerosol mass spectrometers are also discussed. Despite wood, coal and peat
being minor fuel types used for domestic space heating in urban areas, their
relatively low combustion efficiencies result in a significant contribution
to PM&lt;sub&gt;1&lt;/sub&gt; aerosol mass (44% and 28% of the total organic aerosol
mass and non-refractory total PM&lt;sub&gt;1&lt;/sub&gt;, respectively).</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4983/2013/"><title>Continuous atmospheric boundary layer observations in the coastal urban area of Barcelona during SAPUSS</title><link>http://www.atmos-chem-phys.net/13/4983/2013/</link><description>&lt;b&gt;Continuous atmospheric boundary layer observations in the coastal urban area of Barcelona during SAPUSS&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4983-4996, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Pandolfi, G. Martucci, X. Querol, A. Alastuey, F. Wilsenack, S. Frey, C. D. O'Dowd, and M. Dall'Osto&lt;br /&gt;&lt;br /&gt;Continuous measurements of surface mixed layer (SML), decoupled
residual/convective layer (DRCL) and aerosol backscatter coefficient were
performed within the Barcelona (Spain) boundary layer from September to
October 2010 (30 days) in the framework of the SAPUSS (Solving Aerosol
Problems by Using Synergistic Strategies) field campaign. Two near-infrared
ceilometers (Jenoptik CHM15K), vertically and horizontally probing (only
vertical profiles are herein discussed), were deployed. Ceilometer-based
DRCLs (1761 ± 363 m a.g.l.) averaged over the campaign duration were twice
as high as the mean SML (904 ± 273 m a.g.l.). Both DRCL and SML showed
a marked SML diurnal cycle. Ceilometer data were compared with potential
temperature profiles measured by daily radiosounding (twice a day, midnight
and midday) to interpret the boundary layer structure in the coastal urban
area of Barcelona. The overall agreement (&lt;i&gt;R&lt;/i&gt;&lt;sup&gt;2&lt;/sup&gt; = 0.80) between the
ceilometer-retrieved and radiosounding-based SML heights (&lt;i&gt;h&lt;/i&gt;) revealed
overestimation of the SML by the ceilometer (&amp;Delta;&lt;i&gt;h&lt;/i&gt;=145 ± 145 m).
After separating the data in accordance with different atmospheric scenarios,
the lowest SML (736 ± 183 m) and DRCL (1573 ± 428 m) were
recorded during warm North African (NAF) advected air mass. By contrast,
higher SML and DRCL were observed during stagnant Regional (REG)
(911 ± 234 m and 1769 ± 314 m, respectively) and cold Atlantic
(ATL) (965 ± 222 m and 1878 ± 290 m, respectively) air masses.
In addition to being the lowest, the SML during the NAF scenario frequently
showed a flat upper boundary throughout the day possibly because of the
strong winds from the Mediterranean Sea limiting the midday SML convective
growth. The mean backscatter coefficients were calculated at two selected
heights representative of middle and top SML portions, i.e.
&amp;beta;&lt;sub&gt;500&lt;/sub&gt; = 0.59 ± 0.45 Mm&lt;sup&gt;−1&lt;/sup&gt; sr&lt;sup&gt;−1&lt;/sup&gt; and
&amp;beta;&lt;sub&gt;800&lt;/sub&gt; = 0.87 ± 0.68 Mm&lt;sup&gt;−1&lt;/sup&gt; sr&lt;sup&gt;−1&lt;/sup&gt; at 500 m and
800 m a.g.l., respectively. The highest backscatter coefficients were observed during NAF
(&amp;beta;&lt;sub&gt;500&lt;/sub&gt; = 0.77 ± 0.57 Mm&lt;sup&gt;−1&lt;/sup&gt; sr&lt;sup&gt;−1&lt;/sup&gt;) when compared
with ATL (&amp;beta;&lt;sub&gt;500&lt;/sub&gt; = 0.51 ± 0.44 Mm&lt;sup&gt;−1&lt;/sup&gt; sr&lt;sup&gt;−1&lt;/sup&gt;) and REG
(&amp;beta;&lt;sub&gt;500&lt;/sub&gt; = 0.64 ± 0.39 Mm&lt;sup&gt;−1&lt;/sup&gt; sr&lt;sup&gt;−1&lt;/sup&gt;). The relationship
between the vertical change in backscatter coefficient and atmospheric
stability (&amp;part;&amp;theta;/&amp;part;&lt;i&gt;z&lt;/i&gt;) was investigated in the first
3000 m a.g.l., aiming to study how the unstable, stable or neutral
atmospheric conditions of the atmosphere alter the distribution of aerosol
backscatter with height over Barcelona. A positive correlation between
unstable conditions and enhanced backscatter and vice versa was found.</description><dc:date>2013-05-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4963/2013/"><title>Evaluating and constraining ice cloud parameterizations in CAM5 using aircraft measurements from the SPARTICUS campaign</title><link>http://www.atmos-chem-phys.net/13/4963/2013/</link><description>&lt;b&gt;Evaluating and constraining ice cloud parameterizations in CAM5 using aircraft measurements from the SPARTICUS campaign&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4963-4982, 2013&lt;br /&gt;&lt;br /&gt;Author(s): K. Zhang, X. Liu, M. Wang, J. M. Comstock, D. L. Mitchell, S. Mishra, and G. G. Mace&lt;br /&gt;&lt;br /&gt;This study uses aircraft measurements of relative humidity and ice crystal
size distribution collected during the SPARTICUS (Small PARTicles In CirrUS)
field campaign to evaluate and constrain ice cloud parameterizations in the
Community Atmosphere Model version 5. About 200 h of data were collected
during the campaign between January and June 2010, providing the longest
aircraft measurements available so far for cirrus clouds in the
midlatitudes. The probability density function (PDF) of ice crystal number
concentration (&lt;i&gt;N&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;)
derived from the high-frequency (1 Hz)
measurements features a strong dependence on ambient temperature. As
temperature decreases from −35 °C to −62 °C, the peak
in the PDF shifts from 10–20 L&lt;sup&gt;−1&lt;/sup&gt; to 200–1000 L&lt;sup&gt;−1&lt;/sup&gt;,
while &lt;i&gt;N&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt; shows a factor of 6–7 increase.
&lt;br&gt;&lt;br&gt;
Model simulations are performed with two different ice nucleation schemes for
pure ice-phase clouds. One of the schemes can reproduce a clear increase of
&lt;i&gt;N&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt; with decreasing temperature by using either an
observation-based ice nuclei spectrum or a classical-theory-based spectrum with
a relatively low (5–10%) maximum freezing ratio for dust aerosols. The
simulation with the other scheme, which assumes a high maximum freezing ratio
(100%), shows much weaker temperature dependence of &lt;i&gt;N&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;.
Simulations are also performed to test empirical parameters related to water
vapor deposition and the autoconversion of ice crystals to snow. Results
show that a value between 0.05 and 0.1 for the water vapor deposition
coefficient, and 250 μm for the critical diameter that
distinguishes ice crystals from snow, can produce good agreement between
model simulation and the SPARTICUS measurements in terms of &lt;i&gt;N&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;
and effective radius. The climate impact of perturbing
these parameters is also discussed.</description><dc:date>2013-05-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4941/2013/"><title>CO&lt;sub&gt;2&lt;/sub&gt; dispersion modelling over Paris region within the CO&lt;sub&gt;2&lt;/sub&gt;-MEGAPARIS project</title><link>http://www.atmos-chem-phys.net/13/4941/2013/</link><description>&lt;b&gt;CO&lt;sub&gt;2&lt;/sub&gt; dispersion modelling over Paris region within the CO&lt;sub&gt;2&lt;/sub&gt;-MEGAPARIS project&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4941-4961, 2013&lt;br /&gt;&lt;br /&gt;Author(s): C. Lac, R. P. Donnelly, V. Masson, S. Pal, S. Riette, S. Donier, S. Queguiner, G. Tanguy, L. Ammoura, and I. Xueref-Remy&lt;br /&gt;&lt;br /&gt;Accurate simulation of the spatial and temporal variability of tracer mixing
ratios over urban areas is a challenging and interesting task needed to be
performed in order to utilise CO&lt;sub&gt;2&lt;/sub&gt; measurements in an atmospheric inverse
framework and to better estimate regional CO&lt;sub&gt;2&lt;/sub&gt; fluxes. This study
investigates the ability of a high-resolution model to simulate
meteorological and CO&lt;sub&gt;2&lt;/sub&gt; fields around Paris agglomeration during the March
field campaign of the CO&lt;sub&gt;2&lt;/sub&gt;-MEGAPARIS project. The mesoscale atmospheric
model Meso-NH, running at 2 km horizontal resolution, is coupled with the
Town Energy Balance (TEB) urban canopy scheme and with the Interactions
between Soil, Biosphere and Atmosphere CO&lt;sub&gt;2&lt;/sub&gt;-reactive (ISBA-A-gs) surface
scheme, allowing a full interaction of CO&lt;sub&gt;2&lt;/sub&gt; modelling between the surface
and the atmosphere. Statistical scores show a good representation of the
urban heat island (UHI) with stronger urban–rural contrasts on temperature
at night than during the day by up to 7 °C. Boundary layer heights
(BLH) have been evaluated on urban, suburban and rural sites during the
campaign, and also on a suburban site over 1 yr. The diurnal cycles of the
BLH are well captured, especially the onset time of the BLH increase and its
growth rate in the morning, which are essential for tall tower CO&lt;sub&gt;2&lt;/sub&gt;
observatories. The main discrepancy is a small negative bias over urban and
suburban sites during nighttime (respectively 45 m and 5 m), leading to a
few overestimations of nocturnal CO&lt;sub&gt;2&lt;/sub&gt; mixing ratios at suburban sites and a
bias of +5 ppm. The diurnal CO&lt;sub&gt;2&lt;/sub&gt; cycle is generally well captured for all
the sites. At the Eiffel tower, the observed spikes of CO&lt;sub&gt;2&lt;/sub&gt; maxima occur
every morning exactly at the time at which the atmospheric boundary layer
(ABL) growth reaches the measurement height. At suburban ground stations,
CO&lt;sub&gt;2&lt;/sub&gt; measurements exhibit maxima at the beginning and at the end of each
night, when the ABL is fully contracted, with a strong spatio-temporal
variability. A sensitivity test without urban parameterisation removes the
UHI and underpredicts nighttime BLH over urban and suburban sites, leading to
large overestimation of nocturnal CO&lt;sub&gt;2&lt;/sub&gt; mixing ratio at the suburban sites
(bias of +17 ppm). The agreement between observation and prediction for BLH
and CO&lt;sub&gt;2&lt;/sub&gt; concentrations and urban–rural increments, both day and night,
demonstrates the potential of using the urban mesoscale system in the context
of inverse modelling</description><dc:date>2013-05-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4917/2013/"><title>The mass and number size distributions of black carbon aerosol over Europe</title><link>http://www.atmos-chem-phys.net/13/4917/2013/</link><description>&lt;b&gt;The mass and number size distributions of black carbon aerosol over Europe&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4917-4939, 2013&lt;br /&gt;&lt;br /&gt;Author(s): C. L. Reddington, G. McMeeking, G. W. Mann, H. Coe, M. G. Frontoso, D. Liu, M. Flynn, D. V. Spracklen, and K. S. Carslaw&lt;br /&gt;&lt;br /&gt;Black carbon-containing aerosol particles play an important role in the
direct and indirect radiative forcing of climate. However, the magnitude and
sign of the net radiative effect is strongly dependent on the physical
properties of the black carbon (BC) component of the particles, such as mass
concentration, number size distribution and mixing state. Here we use a
global aerosol model combined with aircraft measurements of BC particle
number and size from the Single Particle Soot Photometer (SP2) to assess the
realism with which these physical properties are predicted by global models.
The comparison reveals a substantial mismatch between the measured and
modelled BC size distribution over the size range of the SP2 instrument
(90–400 nm BC diameter). The model predicts BC particle number
concentrations a factor ~3.5–5.7 higher than measured and a mode
diameter that is ~40–65 nm smaller than observed. More than
~90% of the model particles with dry diameters &amp;gtrsim;260 nm
contain BC, while the observations suggest only 14% on average. These
model–observation biases in the BC properties are considerably greater than
for the overall particle distribution, suggesting that the discrepancy is
associated with model assumptions about the size and mixing state of the
emitted carbonaceous particles. We expect the discrepancy in BC size
distribution to be common among most global aerosol models, with implications
for model estimates of absorption optical depth and direct radiative forcing.</description><dc:date>2013-05-14T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys.net/13/4907/2013/"><title>Linkages between ozone-depleting substances, tropospheric oxidation and aerosols</title><link>http://www.atmos-chem-phys.net/13/4907/2013/</link><description>&lt;b&gt;Linkages between ozone-depleting substances, tropospheric oxidation and aerosols&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics, 13, 4907-4916, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Voulgarakis, D. T. Shindell, and G. Faluvegi&lt;br /&gt;&lt;br /&gt;Coupling between the stratosphere and the troposphere allows changes in
stratospheric ozone abundances to affect tropospheric chemistry. Large-scale
effects from such changes on chemically produced tropospheric aerosols have
not been systematically examined in past studies. We use a
composition-climate model to investigate potential past and future impacts
of changes in stratospheric ozone depleting substances (ODS) on tropospheric
oxidants and sulfate aerosols. In most experiments, we find significant
responses in tropospheric photolysis and oxidants, with small but
significant effects on methane radiative forcing. The response of sulfate
aerosols is sizeable when examining the effect of increasing future nitrous
oxide (N&lt;sub&gt;2&lt;/sub&gt;O) emissions. We also find that without the regulation of
chlorofluorocarbons (CFCs) through the Montreal Protocol, sulfate aerosols
could have increased by 2050 by a comparable amount to the decreases
predicted due to relatively stringent sulfur emissions controls. The
individual historical radiative forcings of CFCs and N&lt;sub&gt;2&lt;/sub&gt;O through their
indirect effects on methane (−22.6 mW m&lt;sup&gt;−2&lt;/sup&gt; for CFCs and −6.7 mW m&lt;sup&gt;−2&lt;/sup&gt;
for N&lt;sub&gt;2&lt;/sub&gt;O) and sulfate aerosols (−3.0 mW m&lt;sup&gt;−2&lt;/sup&gt;
for CFCs and +6.5 mW m&lt;sup&gt;−2&lt;/sup&gt; for N&lt;sub&gt;2&lt;/sub&gt;O when considering the direct aerosol effect)
discussed here are non-negligible when compared to known historical ODS
forcing. Our results stress the importance of accounting for
stratosphere-troposphere, gas-aerosol and composition-climate interactions
when investigating the effects of changing emissions on atmospheric
composition and climate.</description><dc:date>2013-05-14T00:00:00+02:00</dc:date></item></rdf:RDF>