<?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-discuss.net/xml/rss1_0.xml"><title>ACPD - Latest Articles</title><link>http://www.atmos-chem-phys-discuss.net/</link><description>Atmospheric Chemistry and Physics Discussions Latest Articles</description><items><rdf:Seq><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13853/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13799/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13773/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13721/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13685/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13653/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13541/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13519/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13495/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13465/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13439/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13323/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13285/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13245/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13191/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13119/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13079/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/13045/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/12991/2013/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/13/12913/2013/" /></rdf:Seq></items></channel><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13853/2013/"><title>A long-term satellite study of aerosol effects on convective clouds in Nordic background air</title><link>http://www.atmos-chem-phys-discuss.net/13/13853/2013/</link><description>&lt;b&gt;A long-term satellite study of aerosol effects on convective clouds in Nordic background air&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13853-13888, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. K. Sporre, E. Swietlicki, P. Glantz, and M. Kulmala&lt;br /&gt;&lt;br /&gt;Aerosol-cloud interactions constitute a~major uncertainty in future
      climate predictions. This study combines 10 yr of ground-based
      aerosol particle measurements from 2 Nordic background stations
      (Vavihill and Hyytiälä) with MODIS (Moderate Resolution
      Imaging Spectroradiometer) satellite data of convective clouds. The
      merged data are used to examine the indirect aerosol effects on
      convective clouds over the Nordic countries. From the satellite
      scenes, vertical profiles of cloud droplet effective radius
      (&lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt;) are created by plotting &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt; against
      cloud top temperature. The profiles have been divided according to
      aerosol loading but also modeled meteorological parameters from the
      ECMWF (European Centre for Medium-Range Forecasts). Furthermore,
      weather radar data from the BALTEX (Baltic Sea Experiment) and ground
      based precipitation measurements from several ground-based
      meteorological measurement stations have been investigated to
      determine whether aerosols affect precipitation intensity and amount.
&lt;br&gt;&lt;br&gt;
      Higher aerosol number concentrations result in smaller
      &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt; throughout the entire profiles at both
      stations. Profiles associated with no or little precipitation have
      smaller droplets than those associated with more
      precipitation. Furthermore, an increase in aerosol loadings results in
      a suppression of precipitation rates, when the vertical extent of the
      clouds has been taken into account. Clouds with greater vertical
      extent have the highest precipitation rates and are most sensitive to
      aerosol perturbations. Nevertheless, meteorological parameters such as
      the vertical extent of the clouds, the atmospheric instability and the
      relative humidity in the lower atmosphere affect the amount of
      precipitation that reaches the ground more than the aerosols do. The
      combination of these ground-based and remote sensing datasets provides
      a unique long-term study of the effects of aerosols on convective
      clouds over the Nordic countries.</description><dc:date>2013-05-24T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13799/2013/"><title>Secondary organic aerosol formation and primary organic aerosol oxidation from biomass burning smoke in a flow reactor during FLAME-3</title><link>http://www.atmos-chem-phys-discuss.net/13/13799/2013/</link><description>&lt;b&gt;Secondary organic aerosol formation and primary organic aerosol oxidation from biomass burning smoke in a flow reactor during FLAME-3&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13799-13851, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. M. Ortega, D. A. Day, M. J. Cubison, W. H. Brune, D. Bon, J. A. de Gouw, and J. L. Jimenez&lt;br /&gt;&lt;br /&gt;We report the physical and chemical effects of photochemically aging
  dilute biomass-burning smoke. A potential aerosol mass &quot;PAM&quot; flow
  reactor was used with analysis by a high-resolution aerosol mass
  spectrometer and a proton-transfer reaction ion-trap mass spectrometer
  during the FLAME-3 campaign. Hydroxyl (OH) radical concentrations in
  the reactor reached up to ~ 1000 times average tropospheric
  levels, producing effective OH exposures equivalent to up to 5 days aging
  in the atmosphere. VOC observations show aromatics and terpenes
  decrease with aging, while formic acid and other unidentified
  oxidation products increase.  Unidentified gas-phase oxidation
  products, previously observed in atmospheric and laboratory
  measurements, were observed here, including evidence of multiple
  generations of photochemistry. Substantial new organic aerosol (OA)
  mass (&quot;net SOA&quot;; secondary OA) was observed from aging
  biomass-burning smoke, resulting in an total OA average of 1.42 &amp;pm; 0.36
  times the initial primary OA (POA) after oxidation. This study
  confirms that the net SOA to POA ratio of biomass burning smoke is
  far lower on average than that observed for urban emissions.
  Although most fuels were very reproducible, significant differences
  were observed among the biomasses, with some fuels resulting in
  a doubling of the OA mass, while for others a very small increase or
  even a decrease was observed. Net SOA formation in the photochemical
  reactor increased with OH exposure (OH&lt;sub&gt;exp&lt;/sub&gt;), typically peaking
  around three days of equivalent atmospheric photochemical age
  (OH&lt;sub&gt;exp&lt;/sub&gt; ~ 3.9 &amp;times;
  10&lt;sup&gt;11&lt;/sup&gt; molecules cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;), then leveling off at
  higher exposures. The amount of additional OA mass added from aging
  is positively correlated with initial POA concentration, but not
  with the total VOC concentration or the concentration of known SOA
  precursors. The mass of SOA formed often exceeds the mass of the
  known VOC precursors, indicating the likely importance of primary
  semivolatile/intermediate volatility species, and possibly of
  unidentified VOCs as SOA precursors in biomass burning
  smoke. Chemical transformations continue even after mass
  concentration stabilizes. Changes in the biomass-burning tracer
  &lt;i&gt;f&lt;/i&gt;&lt;sub&gt;60&lt;/sub&gt; ranged from substantially decreasing to remaining constant
  with increased aging. With increased OH&lt;sub&gt;exp&lt;/sub&gt;, oxidation was
  always detected (as indicated by &lt;i&gt;f&lt;/i&gt;&lt;sub&gt;44&lt;/sub&gt; and O/C). POA O/C ranged 0.15–0.5,
  while aged OA O/C reached up to 0.87. The rate of oxidation and maximum O/C
  achieved differs for each biomass and appears to increase with the initial
  O/C of the POA.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13773/2013/"><title>Water-soluble organic carbon over the Pearl River Delta region during fall–winter: spatial variations and source apportionment</title><link>http://www.atmos-chem-phys-discuss.net/13/13773/2013/</link><description>&lt;b&gt;Water-soluble organic carbon over the Pearl River Delta region during fall–winter: spatial variations and source apportionment&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13773-13798, 2013&lt;br /&gt;&lt;br /&gt;Author(s): X. Ding, X.-M. Wang, Q.-F. He, X.-X. Fu, and B. Gao&lt;br /&gt;&lt;br /&gt;Water-soluble organic carbon (WSOC) is a major component of
  carbonaceous aerosols.  However, the detailed information of WSOC
  origins is still unclear. In the current study, fine particles
  (PM&lt;sub&gt;2.5&lt;/sub&gt;) were collected at one sub-urban and two rural
  sites in the Pearl River Delta (PRD) region, south China during
  fall–winter 2008 to measure WSOC and organic tracers of biomass
  burning (BB) and secondary organic aerosols (SOA) from isoprene,
  monoterpenes, &amp;beta;-caryophyllene, aromatics and 2-ring
  polycyclic aromatic hydrocarbons (PAHs). WSOC concentrations ranged
  from 7.63 to 11.5 &amp;mu;g C m&lt;sup&gt;&amp;minus;3&lt;/sup&gt; and accounted for
  38.8–57.9% of organic carbon (OC). Both WSOC and
  water-insoluble organic carbon (WIOC) exhibited higher levels at the
  sub-urban site than the rural sites. Subtracting BB-derived WSOC
  (WSOC&lt;sub&gt;BB&lt;/sub&gt;) from measured WSOC, secondary OC (SOC) and
  primary OC (POC) were estimated that POC exhibited dominance over
  SOC and contributed 68–79% to OC. Significant correlation
  between WSOC and EC was observed, suggesting that BB could have
  important contributions to ambient WSOC in the PRD region during
  fall–winter. Organic tracers were applied to do source apportionment
  of WSOC, which further confirmed that BB was the dominant
  contributor, accounting for 42–47% of measured WSOC. SOC
  estimated by SOA tracers totally contributed 22–40% of WSOC,
  among which anthropogenic SOC (sum of aromatics and 2-ring PAHs,
  18–25%) exhibited dominance over biogenic SOC (sum of
  isoprene, monoterpenes and &amp;beta;-caryophyllene, 4–15%). The
  unexplained WSOC (18–31%) showed a positive correlation with
  POC, indicating that this portion might be associated with POC
  aging.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13721/2013/"><title>Comparison of mixed layer heights from airborne high spectral resolution lidar, ground-based measurements, and the WRF-Chem model during CalNex and CARES</title><link>http://www.atmos-chem-phys-discuss.net/13/13721/2013/</link><description>&lt;b&gt;Comparison of mixed layer heights from airborne high spectral resolution lidar, ground-based measurements, and the WRF-Chem model during CalNex and CARES&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13721-13772, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. J. Scarino, M. D. Obland, J. D. Fast, S. P. Burton, R. A. Ferrare, C. A. Hostetler, L. K. Berg, B. Lefer, C. Haman, J. W. Hair, R. R. Rogers, C. Butler, A. L. Cook, and D. B. Harper&lt;br /&gt;&lt;br /&gt;The California Research at the Nexus of Air Quality and Climate
  Change (CalNex) and Carbonaceous Aerosol and Radiative Effects Study
  (CARES) field campaigns during May and June 2010 provided a data set
  appropriate for studying characteristics of the planetary boundary
  layer (PBL). The NASA Langley Research Center (LaRC) airborne High
  Spectral Resolution Lidar (HSRL) was deployed to California onboard
  the NASA LaRC B-200 aircraft to aid in characterizing aerosol
  properties during these two field campaigns.  Measurements of
  aerosol extinction (532 nm), backscatter (532 and
  1064 nm), and depolarization (532 and 1064 nm)
  profiles during 31 flights, many in coordination with other research
  aircraft and ground sites, constitute a diverse data set for use in
  characterizing the spatial and temporal distribution of aerosols, as
  well as the depth and variability of the daytime mixed layer (ML),
  which is a subset within the PBL. This work illustrates the temporal
  and spatial variability of the ML in the vicinity of Los Angeles and
  Sacramento, CA. ML heights derived from HSRL measurements are
  compared to PBL heights derived from radiosonde profiles, ML heights
  measured from ceilometers, and simulated PBL heights from the
  Weather Research and Forecasting Chemistry (WRF-Chem) community
  model. Comparisons between the HSRL ML heights and the radiosonde
  profiles in Sacramento result in a correlation coefficient value (&lt;i&gt;R&lt;/i&gt;)
  of 0.93 (root-mean-square (RMS) difference of 157 m and bias
  difference (HSRL – radiosonde) of 57 m). HSRL ML heights
  compare well with those from the ceilometer in the LA Basin with an
  &lt;i&gt;R&lt;/i&gt; of 0.89 (RMS difference of 108 m and bias difference (HSRL
  – Ceilometer) of −9.7 m) for distances of up to
  30 km between the B-200 flight track and the ceilometer
  site. Simulated PBL heights from WRF-Chem were compared with those
  obtained from all flights for each campaign, producing an &lt;i&gt;R&lt;/i&gt; of 0.58
  (RMS difference of 604 m and a bias difference (WRF-Chem –
  HSRL) of −157 m) for CalNex and 0.59 (RMS difference of
  689 m and a bias difference (WRF-Chem – HSRL) of
  220 m) for CARES. Aerosol backscatter simulations are also
  available from WRF-Chem and are compared to those from HSRL to
  examine differences among the methods used to derive ML heights.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13685/2013/"><title>Evaluating evidence for Cl sources and oxidation chemistry in a coastal, urban environment</title><link>http://www.atmos-chem-phys-discuss.net/13/13685/2013/</link><description>&lt;b&gt;Evaluating evidence for Cl sources and oxidation chemistry in a coastal, urban environment&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13685-13720, 2013&lt;br /&gt;&lt;br /&gt;Author(s): C. J. Young, R. A. Washenfelder, P. M. Edwards, D. D. Parrish, J. B. Gilman, W. C. Kuster, L. H. Mielke, H. D. Osthoff, C. Tsai, O. Pikelnaya, J. Stutz, P. R. Veres, J. M. Roberts, S. Griffith, S. Dusanter, P. S. Stevens, J. Flynn, N. Grossberg, B. Lefer, J. S. Holloway, J. Peischl, T. B. Ryerson, E. L. Atlas, D. R. Blake, and S. S. Brown&lt;br /&gt;&lt;br /&gt;The role of chlorine atoms (Cl) in atmospheric oxidation was traditionally
thought to be limited to the marine boundary layer,
where they are produced through heterogeneous reactions involving sea
salt. However, recent observation of
photolytic Cl precursors (ClNO&lt;sub&gt;2&lt;/sub&gt; and Cl&lt;sub&gt;2&lt;/sub&gt;) formed
from anthropogenic pollution has expanded the potential importance of Cl to
include coastal and continental urban areas.
Measurements of ClNO&lt;sub&gt;2&lt;/sub&gt; in Los Angeles during CalNex showed it
to be an important primary (first generation) radical
source. Ratios of volatile organic compounds (VOCs) have
been proposed as a sensitive method to quantify Cl
oxidation, but have shown little evidence for
a significant role of Cl outside of the Arctic. We used
a box model with the Master Chemical Mechanism (MCM v3.2)
chemistry scheme, constrained by observations in Los
Angeles, to examine the
Cl-sensitivity of the most commonly used VOC ratios
(&lt;i&gt;i&lt;/i&gt;-butane, &lt;i&gt;n&lt;/i&gt;-butane, and propane) as
a function of NO&lt;sub&gt;x&lt;/sub&gt; and secondary radical
production. Model results indicated these and faster
reacting VOC tracer ratios could not detect the influence of Cl unless the
sustained ratio of OH to Cl was below 200.
However, the model results also show that secondary
(second generation) OH production resulting from Cl oxidation of VOCs is
strongly influenced by NO&lt;sub&gt;x&lt;/sub&gt;, and that this
effect can obscure the importance of Cl as a primary
oxidant. Calculated concentrations of Cl showed
a maximum in mid-morning due to a photolytic source from
ClNO&lt;sub&gt;2&lt;/sub&gt; and loss primarily to reactions with
VOCs. The OH to Cl ratio was below 200 for approximately
three hours in the morning, but Cl oxidation was not
evident from the measured ratios of VOCs.
Instead, model simulations show that secondary OH
production causes VOC ratios to follow the values expected for OH oxidation
despite the significant input of primary Cl from ClNO&lt;sub&gt;2&lt;/sub&gt;
photolysis in the morning. Despite the prevalence of
secondary OH as an oxidant in Los Angeles, Cl may play
an important role in tropospheric chemistry. The
reactivity of Cl in Los Angeles during CalNex was more than an order of
magnitude larger than that of OH. In
addition, because of its reactivity toward different
classes of VOCs and its greater propensity to participate in chain
propagation rather than sink reactions, Cl atoms have
a different impact on regional atmospheric oxidation than do OH
radicals.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13653/2013/"><title>Diagnosing the average spatio-temporal impact of convective   systems – Part 1: A methodology for evaluating climate models</title><link>http://www.atmos-chem-phys-discuss.net/13/13653/2013/</link><description>&lt;b&gt;Diagnosing the average spatio-temporal impact of convective   systems – Part 1: A methodology for evaluating climate models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13653-13684, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. S. Johnston, P. Eriksson, S. Eliasson, M. D. Zelinka, R. M. Forbes, and K. Wyser&lt;br /&gt;&lt;br /&gt;A~method to determine the mean response of upper tropospheric water
  to localised deep convective (DC) events is improved and applied to
  the EC-Earth climate model. Following Zelinka and Hartmann (2009),
  several fields related to moist processes and radiation are
  composited with respect to local maxima in rain rate to determine
  their spatio-temporal evolution with deep convection in the central
  Pacific Ocean.
&lt;br&gt;&lt;br&gt;
  Major improvements to the above study are the isolation of DC events
  in time so as to prevent multiple sampling of the same event, and
  a revised definition of the mean background state that allows for
  better characterization of the DC-induced anomalies.
&lt;br&gt;&lt;br&gt;
  The DC events observed in this study propagate westward at
  ~ 4 m s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. Both the upper tropospheric relative
  humidity and outgoing longwave radiation are substantially perturbed
  over a broad horizontal extent during peak convection and for long
  periods of time. Cloud fraction anomaly increases throughout the
  upper troposphere, especially in the 200–250 hPa layer,
  reaching peak coverage following deep convection.  Cloud ice water
  content anomaly confined to pressures greater than about
  250 hPa and peaks near 450 hPa within a few hours of
  the DC event but remain enhanced following the DC event. Consistent
  with the large increase in upper tropospheric cloud ice, albedo
  increases dramatically and persists for sometime following the DC
  event.
&lt;br&gt;&lt;br&gt;
  Applying the method to the model demonstrates that it is able to
  capture the large-scale responses to DC events, most notably for
  outgoing longwave radiation, but there are a number of important
  differences. For example, the DC signature of upper tropospheric
  humidity consistently covers a broader horizontal area than what is
  observed. In addition, the DC events move eastward in the model, but
  westward in the observations, and exhibit an unrealistic
  24 h repeat cycle. Moreover, the modeled upper tropospheric
  cloud fraction anomalies – despite being of comparable magnitude
  and exhibiting similar longevity – are confined to a thinner layer
  that is closer to the tropopause and peak earlier than in
  observations.  Finally, the modeled ice water content anomalies at
  pressures greater than about 350 hPa are about twice as
  large as in the observations and do not persist as long after peak
  convection.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13541/2013/"><title>The Arctic Summer Cloud-Ocean Study (ASCOS): overview and experimental design</title><link>http://www.atmos-chem-phys-discuss.net/13/13541/2013/</link><description>&lt;b&gt;The Arctic Summer Cloud-Ocean Study (ASCOS): overview and experimental design&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13541-13652, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Tjernström, C. Leck, C. E. Birch, B. J. Brooks, I. M. Brooks, L. Bäcklin, R. Y.-W. Chang, E. Granath, M. Graus, A. Hansel, J. Heintzenberg, A. Held, A. Hind, S. de la Rosa, P. Johnston, J. Knulst, G. de Leeuw, L. Di Liberto, M. Martin, P. A. Matrai, T. Mauritsen, M. Müller, S. J. Norris, M. V. Orellana, D. A. Orsini, J. Paatero, P. O. G. Persson, Q. Gao, C. Rauschenberg, Z. Ristovski, J. Sedlar, M. D. Shupe, B. Sierau, A. Sirevaag, S. Sjogren, O. Stetzer, E. Swietlicki, M. Szczodrak, P. Vaattovaara, N. Wahlberg, M. Westberg, and C. R. Wheeler&lt;br /&gt;&lt;br /&gt;The climate in the Arctic is changing faster than anywhere else on
 Earth. Poorly understood feedback processes relating to Arctic
 clouds and aerosol-cloud interactions contribute to a poor
 understanding of the present changes in the Arctic climate system,
 and also to a large spread in projections of future climate in the
 Arctic. The problem is exacerbated by the paucity of
 research-quality observations in the central Arctic. Improved
 formulations in climate models require such observations, which can
 only come from measurements in-situ in this difficult to
 reach region with logistically demanding environmental conditions.
&lt;br&gt;&lt;br&gt;
 The Arctic Summer Cloud-Ocean Study (ASCOS) was the most extensive
 central Arctic Ocean expedition with an atmospheric focus during the
 International Polar Year (IPY) 2007–2008. ASCOS focused on the
 study of the formation and life cycle of low-level Arctic
 clouds. ASCOS departed from Longyearbyen on Svalbard on 2 August and
 returned on 9 September 2008. In transit into and out of the pack
 ice, four short research stations were undertaken in the Fram
 Strait; two in open water and two in the marginal ice zone. After
 traversing the pack-ice northward an ice camp was set up on 12
 August at 87&amp;deg;21' N 01&amp;deg;29' W
 and remained in operation through 1 September, drifting with the
 ice. During this time extensive measurements were taken of
 atmospheric gas and particle chemistry and physics, mesoscale and
 boundary-layer meteorology, marine biology and chemistry, and upper
 ocean physics.
&lt;br&gt;&lt;br&gt;
 ASCOS provides a unique interdisciplinary data set for development
 and testing of new hypotheses on cloud processes, their interactions
 with the sea ice and ocean and associated physical, chemical, and
 biological processes and interactions. For example, the first ever
 quantitative observation of bubbles in Arctic leads, combined with
 the unique discovery of marine organic material, polymer gels with
 an origin in the ocean, inside cloud droplets suggest the
 possibility of primary marine organically derived cloud condensation nuclei in Arctic
 stratocumulus clouds. Direct observations of surface fluxes of
 aerosols could, however, not explain observed variability in aerosol
 concentrations and the balance between local and remote aerosols
 sources remains open. Lack of CCN was at times a controlling factor
 in low-level cloud formation, and hence for the impact of clouds on
 the surface energy budget. ASCOS provided detailed measurements of
 the surface energy balance from late summer melt into the initial
 autumn freeze-up, and documented the effects of clouds and storms on
 the surface energy balance during this transition. In addition to
 such process-level studies, the unique, independent ASCOS data set
 can and is being used for validation of satellite retrievals,
 operational models, and reanalysis data sets.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13519/2013/"><title>Estimating neutral nanoparticle steady state size distribution and growth according to measurements of intermediate air ions</title><link>http://www.atmos-chem-phys-discuss.net/13/13519/2013/</link><description>&lt;b&gt;Estimating neutral nanoparticle steady state size distribution and growth according to measurements of intermediate air ions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13519-13540, 2013&lt;br /&gt;&lt;br /&gt;Author(s): H. Tammet, K. Komsaare, and U. Hõrrak&lt;br /&gt;&lt;br /&gt;The concentration of nanometer aerosol particles in atmospheric air
  during quiet periods of new particle formation is low and direct
  measuring is difficult. We study what information about neutral
  particles can be drawn from measurements of intermediate ions, which
  are the electrically charged particles between 1.5–7.5 nm
  in diameter. If the coagulation sink of nanoparticles and the growth
  rate of charged particles are known, then the steady state equations
  allow us to calculate the size distribution of neutral
  nanoparticles. Variations in the trial value of the growth rate have
  a minor effect on the estimates of the concentrations and size
  distributions. There exists a value of the constant growth rate of
  charged nanoparticles that leads to a minimum deviation of the
  estimated growth rate of neutral nanoparticles from the growth rate
  of charged nanoparticles. Rough estimates of the growth rate and
  size distribution of neutral nanoparticles are derived despite the
  fact that the sample data of intermediate ion measurements is not
  accompanied by simultaneous measurements of the background aerosol
  and ionization rate. In the case of a near-median intermediate ion
  concentration of 21 &amp;pm; 2 cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; in the urban air of
  a small town, the growth rate of nanoparticles is estimated to be
  about 2 nm h&lt;sup&gt;&amp;minus;1&lt;/sup&gt;, while the growth flux or apparent
  nucleation rate is about 0.5 cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt; at 3 nm
  and about 0.08 cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt; at 7 nm. The results
  suggest that the process of new particle formation is not
  interrupted during the quiet periods between events of intensive
  nucleation of atmospheric aerosols.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13495/2013/"><title>Net influence of an internally-generated QBO on modelled stratospheric climate and chemistry</title><link>http://www.atmos-chem-phys-discuss.net/13/13495/2013/</link><description>&lt;b&gt;Net influence of an internally-generated QBO on modelled stratospheric climate and chemistry&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13495-13518, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. M. Hurwitz, L. D. Oman, P. A. Newman, and I.-S. Song&lt;br /&gt;&lt;br /&gt;A Goddard Earth Observing System Chemistry–Climate Model (GEOSCCM)
  simulation with strong tropical non-orographic gravity wave drag
  (GWD) is compared to an otherwise identical simulation with
  near-zero tropical non-orographic GWD. The GEOSCCM generates
  a quasi-biennial oscillation (QBO) zonal wind signal in response to
  strong, quasi-realistic tropical GWD. The modelled QBO has
  a frequency and amplitude that closely resembles observations. In
  the annual mean, the modelled QBO improves the simulation of
  tropical zonal winds and enhances tropical and sub-tropical
  stratospheric variability. Also, inclusion of the QBO slows the
  meridional overturning circulation, resulting in a generally older
  stratospheric mean age-of-air.  Slowing of the overturning
  circulation, changes in stratospheric temperature and enhanced
  sub-tropical mixing all affect the mean distributions of ozone,
  methane and nitrous oxide. Furthermore, the modelled QBO enhances
  polar stratospheric variability in winter.  Because tropical zonal
  winds are easterly in the simulation without a QBO, there is
  a relative increase in tropical zonal winds in the simulation with
  a QBO. Extra-tropical differences between the simulations with and
  without a QBO thus reflect a bias toward the westerly phase of the
  QBO: a relative strengthening of the polar stratospheric jet, polar
  stratospheric cooling and a weak reduction in Arctic lower
  stratospheric ozone.</description><dc:date>2013-05-23T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13465/2013/"><title>Cross-validation of inferred daytime airborne CO&lt;sub&gt;2&lt;/sub&gt; urban-regional scale surface fluxes with eddy-covariance observations and emissions inventories in Greater London</title><link>http://www.atmos-chem-phys-discuss.net/13/13465/2013/</link><description>&lt;b&gt;Cross-validation of inferred daytime airborne CO&lt;sub&gt;2&lt;/sub&gt; urban-regional scale surface fluxes with eddy-covariance observations and emissions inventories in Greater London&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13465-13493, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Font, C. S. B. Grimmond, J.-A. Morguí, S. Kotthaus, M. Priestman, and B. Barratt&lt;br /&gt;&lt;br /&gt;Data obtained from eleven flight surveys on six days during October 2011 were used to characterize the urban CO&lt;sub&gt;2&lt;/sub&gt; dome in
  Greater London (GL) and to calculate CO&lt;sub&gt;2&lt;/sub&gt; fluxes at the city scale. Flights crossed GL along two transects (SW-NE and SSE-NNW)
  at an altitude of 360 m. Increments as high as 23 ppmv were measured. The maximum CO&lt;sub&gt;2&lt;/sub&gt; mixing ratios were localized
  over GL under low wind speeds, whereas a displacement of the urban plume downwind from the centre of the urban area occurred during
  high wind speeds. The urban-regional surface CO&lt;sub&gt;2&lt;/sub&gt; flux was calculated for four days by the Integrative Mass Boundary Layer
  (IMBL) method. The diurnal CO&lt;sub&gt;2&lt;/sub&gt; flux in GL obtained from the aircraft observations ranged from 46 to 104 &amp;mu;mol
  CO&lt;sub&gt;2&lt;/sub&gt; m&lt;sup&gt;&amp;minus;2&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt; during the day time. The mean CO&lt;sub&gt;2&lt;/sub&gt;
fluxes estimated from the IMBL method were statistically
  similar to those observed by eddy-covariance systems located in central London and a spatially integrated emissions inventory for
  GL. This study provides an important cross-validation of two independent measurement-based methods to infer the contribution of urban
  areas to climate change in terms of CO&lt;sub&gt;2&lt;/sub&gt; surface fluxes, both of which complement bottom-up emissions inventories. The
  uncertainties of fluxes estimated by the IMBL method are considered and the limits of implementation of atmospheric methods to infer
  city-scale fluxes are discussed.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13439/2013/"><title>Simulation of the dispersion of the Eyjafjallajökull plume over Europe with COSMO-ART in the operational mode</title><link>http://www.atmos-chem-phys-discuss.net/13/13439/2013/</link><description>&lt;b&gt;Simulation of the dispersion of the Eyjafjallajökull plume over Europe with COSMO-ART in the operational mode&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13439-13463, 2013&lt;br /&gt;&lt;br /&gt;Author(s): H. Vogel, J. Förstner, B. Vogel, T. Hanisch, B. Mühr, U. Schättler, and T. Schad&lt;br /&gt;&lt;br /&gt;An extended version of the German operational weather forecast model was
used to simulate the ash dispersion during the eruption of the
Eyjafjallajökull. Sensitivity runs show the ability of the model to
simulate thin ash layers when an increased vertical resolution is used.
Calibration of the model results with measured data allows for a
quantitative forecast of the ash concentration. An independent comparison of
the simulated number concentration of 3 μm particles and observations
reveals nearly perfect agreement. However, this perfect agreement could only
be reached after modification of the emissions. As an operational forecast
was launched every six hours, a time-lagged ensemble was obtained. Hence,
the probability of violation of a certain threshold can be calculated. This
is valuable information for the forecasters advising the organizations
responsible for the closing of the airspace.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13323/2013/"><title>Asymmetric and axisymmetric dynamics of tropical cyclones</title><link>http://www.atmos-chem-phys-discuss.net/13/13323/2013/</link><description>&lt;b&gt;Asymmetric and axisymmetric dynamics of tropical cyclones&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13323-13438, 2013&lt;br /&gt;&lt;br /&gt;Author(s): J. Persing, M. T. Montgomery, J. C. McWilliams, and R. K. Smith&lt;br /&gt;&lt;br /&gt;We present the results of idealized numerical experiments to examine
the difference between tropical cyclone evolution in
three-dimensional (3-D) and axisymmetric (AX) model
configurations. We focus on the prototype problem for
intensification, which considers the evolution of an initially
unsaturated AX vortex in gradient-wind balance on an
&lt;i&gt;f&lt;/i&gt;-plane. Consistent with findings of previous work, the mature
intensity in the 3-D model is reduced relative to that in the AX
model. In contrast with previous interpretations invoking barotropic
instability and related horizontal mixing processes as a mechanism
detrimental to the spin-up process, the results indicate that 3-D
eddy processes associated with vortical plume structures can assist
the intensification process by contributing to a radial contraction
of the maximum tangential velocity and to a vertical extension of
tangential winds through the depth of the troposphere. These plumes
contribute significantly also to the azimuthally-averaged heating
rate and the corresponding azimuthal-mean overturning circulation.
&lt;br&gt;&lt;br&gt;
The comparisons show that the resolved 3-D eddy momentum fluxes
above the boundary layer exhibit counter-gradient characteristics
and are generally not represented properly by the subgrid-scale
parameterizations in the AX configuration. The resolved eddy fluxes
act to support the contraction and intensification of the maximum
tangential winds. The comparisons indicate fundamental differences
between convective organization in the 3-D and AX configurations for
meteorologically relevant forecast time scales. While the radial and
vertical gradients of the system-scale angular rotation provide
a hostile environment for deep convection in the 3-D model, with
a corresponding tendency to strain the convective elements in the
tangential direction, deep convection in the AX model does not
suffer this tendency. Also, since during the 3-D intensification
process the convection has not yet organized into annular rings, the
azimuthally-averaged heating rate and radial gradient thereof is
considerably less than that in the AX model. This lack of
organization results broadly in a slower intensification rate in the
3-D model and leads ultimately to a weaker mature vortex after 12
days of model integration. While axisymmetric heating rates in the
3-D model are weaker than those in the AX model, local heating rates
in the 3-D model exceed those in the AX model and at times the
vortex in the 3-D model intensifies more rapidly than AX. Analyses
of the 3-D model output do not support a recent hypothesis
concerning the key role of small-scale vertical mixing processes in
the upper-tropospheric outflow in controlling the intensification
process.
&lt;br&gt;&lt;br&gt;
In the 3-D model, surface drag plays a particularly important role
in the intensification process for the prototype intensification
problem on meteorologically relevant time scales by helping foster
the organization of convection in azimuth. There is a radical
difference in the behaviour of the 3-D and AX simulations when the
surface drag is reduced or increased from realistic
values. Borrowing from ideas developed in a recent paper, we give
a partial explanation for this difference in behaviour.
&lt;br&gt;&lt;br&gt;
Our results provide new qualitative and quantitative insight into
the differences between the asymmetric and symmetric dynamics of
tropical cyclones and would appear to have important consequences
for the formulation of a fluid dynamical theory of tropical cyclone
intensification and mature intensity. In particular, the results
point to some fundamental limitations of strict axisymmetric theory
and modelling for representing the azimuthally-averaged behaviour of
tropical cyclones in three dimensions.</description><dc:date>2013-05-22T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13285/2013/"><title>Air/sea DMS gas transfer in the North Atlantic: evidence for limited interfacial gas exchange at high wind speed</title><link>http://www.atmos-chem-phys-discuss.net/13/13285/2013/</link><description>&lt;b&gt;Air/sea DMS gas transfer in the North Atlantic: evidence for limited interfacial gas exchange at high wind speed&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13285-13322, 2013&lt;br /&gt;&lt;br /&gt;Author(s): T. G. Bell, W. De Bruyn, S. D. Miller, B. Ward, K. Christensen, and E. S. Saltzman&lt;br /&gt;&lt;br /&gt;Shipboard measurements of eddy covariance DMS air/sea fluxes and
  seawater concentration were carried out in the North Atlantic bloom
  region in June/July 2011. Gas transfer coefficients (&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;660&lt;/sub&gt;) show
  a linear dependence on mean horizontal wind speed at wind speeds up
  to 11 m s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. At higher wind speeds the relationship
  between &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;660&lt;/sub&gt; and wind speed weakens. At high winds, measured
  DMS fluxes were lower than predicted based on the linear
  relationship between wind speed and interfacial stress extrapolated
  from low to intermediate wind speeds. In contrast, the transfer
  coefficient for sensible heat did not exhibit this effect. The
  apparent suppression of air/sea gas flux at higher wind speeds
  appears to be related to sea state, as determined from shipboard
  wave measurements. These observations are consistent with the idea
  that long waves suppress near surface water side turbulence, and
  decrease interfacial gas transfer. This effect may be more easily
  observed for DMS than for less soluble gases, such as
  CO&lt;sub&gt;2&lt;/sub&gt;, because the air/sea exchange of DMS is controlled
  by interfacial rather than bubble-mediated gas transfer under high
  wind speed conditions.</description><dc:date>2013-05-21T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13245/2013/"><title>Quantifying tracer transport in the tropical lower stratosphere using WACCM</title><link>http://www.atmos-chem-phys-discuss.net/13/13245/2013/</link><description>&lt;b&gt;Quantifying tracer transport in the tropical lower stratosphere using WACCM&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13245-13283, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Abalos, W. J. Randel, D. E. Kinnison, and E. Serrano&lt;br /&gt;&lt;br /&gt;The zonal mean transport of ozone and carbon monoxide (CO) near the
  tropical tropopause is investigated using the Whole-Atmosphere
  Community Climate Model version 4 (WACCM4). The variability in
  temperature, ozone and CO in the model shows good agreement with
  satellite and balloon observations. Modeled temperature and tracers
  exhibit large and closely coupled annual cycles in the tropical
  lower stratosphere, as in the observations. The thermodynamic and
  tracer budgets in the model are analyzed based on the Transformed
  Eulerian Mean (TEM) framework on log-pressure coordinates and also
  using the isentropic formulation. Results show that the coupled
  seasonal cycles are mainly forced by tropical upwelling over
  altitudes with large vertical tracer gradients, in agreement with
  previous observational studies. The model also allows explicit
  calculation of eddy transport terms, which make an important
  contribution to ozone tendencies in the tropical lower
  stratosphere. The character of the eddy fluxes changes with
  altitude. At higher levels (~2 km above the cold
  point tropopause), isentropic eddy transport occurs during winter
  and spring in each hemisphere in the sub-tropics, associated with
  transient Rossby waves acting on strong background latitudinal
  gradients. At lower altitudes, close to the tropical tropopause,
  there is a maximum in horizontal eddy transport during boreal summer
  associated with the Asian monsoon anticyclone. Sub-seasonal
  variability in ozone and CO, tied to fluctuations in temperature, is
  primarily driven by transient tropical upwelling. In isentropic
  coordinates, the overall tracer budgets are similar to the
  log-pressure results, highlighting cross-isentropic mean advection
  as the main term in the balance. However, in isentropic coordinates
  the tracer variability is largely reduced on both seasonal and
  sub-seasonal timescales, because the tracer and temperature
  fluctuations are highly correlated (as a response to upwelling).</description><dc:date>2013-05-21T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13191/2013/"><title>Cloud and boundary layer interactions over the Arctic sea-ice in late summer</title><link>http://www.atmos-chem-phys-discuss.net/13/13191/2013/</link><description>&lt;b&gt;Cloud and boundary layer interactions over the Arctic sea-ice in late summer&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13191-13244, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. D. Shupe, P. O. G. Persson, I. M. Brooks, M. Tjernström, J. Sedlar, T. Mauritsen, S. Sjogren, and C. Leck&lt;br /&gt;&lt;br /&gt;Observations from the Arctic Summer Cloud Ocean Study (ASCOS), in
  the central Arctic sea-ice pack in late summer 2008, provide
  a detailed view of cloud-atmosphere-surface interactions and
  vertical mixing processes over the sea–ice environment. Measurements
  from a suite of ground-based remote sensors, near surface
  meteorological and aerosol instruments, and profiles from
  radiosondes and a helicopter are combined to characterize
  a week-long period dominated by low-level, mixed-phase,
  stratocumulus clouds. Detailed case studies and statistical analyses
  are used to develop a conceptual model for the cloud and atmosphere
  structure and their interactions in this environment.
&lt;br&gt;&lt;br&gt;
  Clouds were persistent during the period of study, having qualities
  that suggest they were sustained through a combination of advective
  influences and in-cloud processes, with little contribution from the
  surface. Radiative cooling near cloud top produced buoyancy-driven,
  turbulent eddies that contributed to cloud formation and created
  a cloud-driven mixed layer. The depth of this mixed layer was
  related to the amount of turbulence and condensed cloud
  water. Coupling of this cloud-driven mixed layer to the surface
  boundary layer was primarily determined by proximity. For 75%
  of the period of study, the primary stratocumulus cloud-driven mixed
  layer was decoupled from the surface and typically at a warmer
  potential temperature. Since the near-surface temperature was
  constrained by the ocean–ice mixture, warm temperatures aloft
  suggest that these air masses had not significantly interacted with
  the sea–ice surface. Instead, back trajectory analyses suggest that
  these warm airmasses advected into the central Arctic Basin from
  lower latitudes. Moisture and aerosol particles likely accompanied
  these airmasses, providing necessary support for cloud formation. On
  the occasions when cloud-surface coupling did occur, back
  trajectories indicated that these air masses advected at low levels,
  while mixing processes kept the mixed layer in equilibrium with the
  near-surface environment. Rather than contributing buoyancy forcing
  for the mixed-layer dynamics, the surface instead simply appeared to
  respond to the mixed-layer processes aloft. Clouds in these cases
  often contained slightly higher condensed water amounts, potentially
  due to additional moisture sources from below.</description><dc:date>2013-05-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13119/2013/"><title>The global impact of the transport sectors on atmospheric aerosol: simulations for year 2000 emissions</title><link>http://www.atmos-chem-phys-discuss.net/13/13119/2013/</link><description>&lt;b&gt;The global impact of the transport sectors on atmospheric aerosol: simulations for year 2000 emissions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13119-13189, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Righi, J. Hendricks, and R. Sausen&lt;br /&gt;&lt;br /&gt;We use the EMAC-MADE global aerosol model to quantify the impact of
  transport emissions (land transport, shipping and aviation) on
  global aerosol. We consider a present-day (2000) scenario and the
  CMIP5 emission dataset developed in support of the IPCC Fifth
  Assessment Report. The model takes also into account particle number
  emissions, which are derived from mass emissions under different
  assumptions on the size distribution of particles emitted by the
  three transport sectors. Additional sensitivity experiments are
  performed to quantify the effects of the uncertainties behind such
  assumptions. The model simulations show that the impact of the
  transport sectors closely matches the emission patterns. Land
  transport is the most important source of black carbon pollution in
  USA, Europe and Arabian Peninsula. Shipping strongly contributes to
  aerosol sulfate concentrations along the most-traveled routes of the
  northern Atlantic and northern Pacific oceans, with a significant
  impact along the coastlines. The effect of aviation is mostly
  confined to the upper-troposphere (7–12 km), in the
  northern mid-latitudes, although significant effects are also
  simulated at the ground, due to the emissions from landing and
  take-off cycles. The transport-induced perturbations to particle
  number concentrations are very sensitive to the assumptions on the
  size distribution of emitted particles, with the largest
  uncertainties obtained for the land transport sector. The simulated
  climate impacts, due to aerosol direct and indirect effects, are
  strongest for the shipping sector, as a consequence of the large
  impact of sulfate aerosol on low marine clouds and their optical
  properties.</description><dc:date>2013-05-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13079/2013/"><title>Long term in-situ observations of biomass burning aerosol at a high altitude station in Venezuela – sources, impacts and inter annual variability</title><link>http://www.atmos-chem-phys-discuss.net/13/13079/2013/</link><description>&lt;b&gt;Long term in-situ observations of biomass burning aerosol at a high altitude station in Venezuela – sources, impacts and inter annual variability&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13079-13117, 2013&lt;br /&gt;&lt;br /&gt;Author(s): T. Hamburger, M. Matisāns, P. Tunved, J. Ström, S. Calderon, P. Hoffmann, G. Hochschild, J. Gross, T. Schmeissner, and R. Krejci&lt;br /&gt;&lt;br /&gt;First long-term observations of South American biomass burning
  aerosol within the tropical lower free troposphere are
  presented. The observations were conducted between 2007 and 2009 at
  a high altitude station (4765 m a.s.l.) on the Pico Espejo,
  Venezuela. Sub-micron aerosol volume, number concentrations of
  primary particles and particle absorption were observed. Orographic
  lifting and shallow convection leads to a distinct diurnal cycle at
  the station. It enables measurements within the lower free
  troposphere during night time and observations of boundary layer air
  masses during day time and at their transitional regions. The
  seasonal cycle is defined by a wet rainy season and a dry biomass
  burning season. The particle load of biomass burning aerosol is
  dominated by fires in the Venezuelan savannah. Increases of aerosol
  concentrations could not be linked to long-range transport of
  biomass burning plumes from the Amazon basin or Africa due to
  effective wet scavenging of particles. Highest particle
  concentrations were observed within boundary layer air masses during
  the dry season. Ambient sub-micron aerosol volume reached
  1.4 &amp;plusmn; 1.3 &amp;mu;m&lt;sup&gt;3&lt;/sup&gt; cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt;, heated (300 &amp;deg;C) particle
  number concentrations 510 &amp;plusmn; 420 cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; and the
  absorption coefficient 0.91 &amp;plusmn; 1.2 Mm&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. The
  respective concentrations were lowest within the lower free
  troposphere during the wet season and averaged at 
 0.19 &amp;plusmn; 0.25 &amp;mu;m&lt;sup&gt;3&lt;/sup&gt; cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt;, 150 &amp;plusmn; 94 cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; and
  0.15 &amp;plusmn; 0.26 Mm&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. A decrease of particle
  concentrations during the dry seasons from 2007–2009 could be
  connected to a decrease in fire activity in the wider region of
  Venezuela using MODIS satellite observations. The variability of
  biomass burning is most likely linked to the El Niño-Southern
  Oscillation (ENSO). Low biomass burning activity in the Venezuelan
  savannah was observed to follow La Niña conditions, high biomass
  burning activity followed El Niño conditions.</description><dc:date>2013-05-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/13045/2013/"><title>Ozone weekend effects in the Beijing–Tianjin–Hebei metropolitan area, China</title><link>http://www.atmos-chem-phys-discuss.net/13/13045/2013/</link><description>&lt;b&gt;Ozone weekend effects in the Beijing–Tianjin–Hebei metropolitan area, China&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 13045-13078, 2013&lt;br /&gt;&lt;br /&gt;Author(s): Y. H. Wang, B. Hu, and Y. S. Wang&lt;br /&gt;&lt;br /&gt;The ozone weekend effect (OWE) was first investigated in the metropolitan
area of Beijing–Tianjin–Hebei (BTH), China, using in situ measurements from
the Atmospheric Environment Monitoring Network from July 2009 to August 2011.
The results indicate that there is an obvious weekly periodical variation in
the surface ozone concentration based on 24 h averaged value. There is
a lower ozone concentration from Wednesday to Friday (weekday) and a higher
concentration from Saturday to Monday (weekend) over the entire study area.
NO&lt;sub&gt;x&lt;/sub&gt; also displays weekly cycle, with the maximum level occurring on
weekdays and the minimum level on weekends, especially later on Sunday night
and early Monday morning. This pattern may be responsible for the higher
concentration of ozone on weekends. Additionally, the vertical variations in
O&lt;sub&gt;3&lt;/sub&gt; and NO&lt;sub&gt;x&lt;/sub&gt; from the 8 m  47 m, 120 m
and 280 m observation platforms on the 325 m Beijing
meteorological tower displayed obvious weekly cycles that corresponded to the
surface results.
&lt;br&gt;&lt;br&gt;
A smaller decrease in VOCs (a proxy for CO) and much lower NO&lt;sub&gt;x&lt;/sub&gt;
concentrations on the weekend may lead to higher VOC/NO&lt;sub&gt;x&lt;/sub&gt; ratio, which
can enhance the ozone production efficiency in VOC-regime areas.
Additionally, a clear weekly cycle in the fine aerosol concentration
was observed, with maximum values occurring on weekdays and minimum
values occurring on weekends. Higher concentrations of aerosol on
weekdays can reduce the UV radiation flux by absorption or scattering,
which leads to a decrease in the ozone production
efficiency. A significant weekly cycle in UV radiation, in consistent
with the aerosol concentration, was discovered at the BJT site,
validating the assumption.  A comprehensive understanding of the ozone
weekend effect in the BTH area can provide deep insights into
controlling photochemical pollution.</description><dc:date>2013-05-17T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/12991/2013/"><title>Reconstruction of Northern Hemisphere 1950–2010 atmospheric non-methane hydrocarbons</title><link>http://www.atmos-chem-phys-discuss.net/13/12991/2013/</link><description>&lt;b&gt;Reconstruction of Northern Hemisphere 1950–2010 atmospheric non-methane hydrocarbons&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12991-13043, 2013&lt;br /&gt;&lt;br /&gt;Author(s): D. Helmig, V. Petrenko, P. Martinerie, E. Witrant, T. Röckmann, A. Zuiderweg, R. Holzinger, J. Hueber, C. Stephens, J. White, W. Sturges, A. Baker, T. Blunier, D. Etheridge, M. Rubino, and P. Tans&lt;br /&gt;&lt;br /&gt;The short-chain non-methane hydrocarbons (NMHC) are mostly emitted into the
atmosphere by anthropogenic processes. Recent studies have pointed out a
tight linkage between the atmospheric mole fractions of the NMHC ethane to
the atmospheric growth rate of methane. Consequently, atmospheric NMHC are
valuable indicators for tracking changes in anthropogenic emissions,
photochemical ozone production, and greenhouse gases. This study
investigates the 1950–2010 Northern Hemisphere atmospheric C&lt;sub&gt;2&lt;/sub&gt;-C&lt;sub&gt;5&lt;/sub&gt;
NMHC ethane, propane, &lt;i&gt;i&lt;/i&gt;-butane, &lt;i&gt;n&lt;/i&gt;-butane, &lt;i&gt;i&lt;/i&gt;-pentane, and &lt;i&gt;n&lt;/i&gt;-pentane.
Atmospheric mole fractions of these trace gases were constructed from (a) air samples of these trace gases from air
samples extracted from three firn boreholes in 2008 and 2009 at the North
Greenland Eemian Ice Drilling (NEEM) site using state of the art models of
trace gas transport in firn, and by (b) considering eight years of ambient
NMHC monitoring data from five Arctic sites within the NOAA Global
Monitoring Division (GMD) Cooperative Air Sampling Network. Results indicate
that these NMHC increased by ~ 40–120% after 1950, peaked
around 1980 (with the exception of ethane, which peaked approximately 10
years earlier), and have since dramatically decreased to be now back close
to 1950 levels. The earlier peak time of ethane versus the C&lt;sub&gt;3&lt;/sub&gt;-C&lt;sub&gt;5&lt;/sub&gt;
NMHC suggests that different processes and emissions mitigation measures
contributed to the decline in these NMHC. The 60 yr record also
illustrates notable increases in the ratios of the isomeric &lt;i&gt;iso-/n&lt;/i&gt;-butane and
&lt;i&gt;iso-/n&lt;/i&gt;-pentane ratios. Comparison of the reconstructed NMHC histories with
1950–2000 volatile organic compounds (VOC) emissions data and with other
recently published ethane trend analyses from ambient air Pacific transect
data showed (a) better agreement with North America and Western Europe
emissions than with total Northern Hemisphere emissions data, and (b) better
agreement with other Greenland firn air data NMHC history reconstructions
than with the Pacific region trends. These analyses emphasize that for NMHC,
having atmospheric lifetimes on the order of &lt; 2 months, the
Greenland firn air records are primarily a representation of Western Europe
and North America emission histories.</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/13/12913/2013/"><title>The balances of mixing ratios and segregation intensity: a case study from the field (ECHO 2003)</title><link>http://www.atmos-chem-phys-discuss.net/13/12913/2013/</link><description>&lt;b&gt;The balances of mixing ratios and segregation intensity: a case study from the field (ECHO 2003)&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12913-12989, 2013&lt;br /&gt;&lt;br /&gt;Author(s): R. Dlugi, M. Berger, M. Zelger, A. Hofzumahaus, F. Rohrer, F. Holland, K. Lu, and G. Kramm&lt;br /&gt;&lt;br /&gt;An inhomogeneous mixing of reactants causes a reduction of their
  chemical removal compared to the homogeneously mixed case in
  turbulent atmospheric flows.  This can be described by the intensity
  of segregation &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; being the covariance of the mixing
  ratios of two species divided by the product of their means.  Both
  terms appear in the balance equation of the mixing ratio and are
  discussed for the reaction between isoprene and OH for data
  of the field study ECHO 2003 above a deciduous forest.  For most of
  these data, &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; is negatively correlated with the
  fraction of mean OH mixing ratio reacting with isoprene.
  &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; is also negatively correlated with the isoprene
  standard deviation.  Both findings agree with model results
  discussed by Patton et al. (2001) and others.  The correlation
  coefficient between OH and isoprene, and, therefore,
  &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; increases with increasing mean reaction rate.  In
  addition, the balance equation of the covariance between isoprene
  and OH is applied for the analysis of the same field data.
  The storage term is small, and, therefore, a diagnostic equation for
  this covariance can be derived.  The chemical reaction term &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&lt;i&gt;ij&lt;/i&gt;&lt;/sub&gt;
  is dominated by the variance of isoprene times the quotient of
  mixing ratios of OH and isoprene.  In addition a diagnostic
  equation for &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; is formulated.  Comparing different
  terms of this equation, &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; and &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&lt;i&gt;ij&lt;/i&gt;&lt;/sub&gt; show a relation
  also to the normalized isoprene standard deviation.  It is shown
  that not only chemistry, but also turbulent and convective mixing
  and advection – considered in a residual term – influence
  &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt;.  Despite this finding, a detection of the influence
  of coherent eddy transport above the forest according to
  Katul et al. (1997) on &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; fails, but a relation with the
  turbulent transport of isoprene variance is determined.  In
  addition, largest values of &lt;i&gt;I&lt;/i&gt;&lt;sub&gt;S&lt;/sub&gt; are found for most
  unstable conditions with increasing buoyancy. These results are
  compared to model results by Ouwersloot et al. (2011).</description><dc:date>2013-05-15T00:00:00+02:00</dc:date></item></rdf:RDF>