<?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/12/4417/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4373/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4341/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4311/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4279/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4243/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4221/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4185/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4165/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4101/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4073/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/4031/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3983/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3941/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3875/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3781/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3731/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3695/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3655/2012/" /><rdf:li resource="http://www.atmos-chem-phys-discuss.net/12/3619/2012/" /></rdf:Seq></items></channel><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4417/2012/"><title>Long-term monitoring of atmospheric total gaseous mercury (TGM) at a remote site in Mt. Changbai area, northeastern China</title><link>http://www.atmos-chem-phys-discuss.net/12/4417/2012/</link><description>&lt;b&gt;Long-term monitoring of atmospheric total gaseous mercury (TGM) at a remote site in Mt. Changbai area, northeastern China&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4417-4446, 2012&lt;br /&gt;&lt;br /&gt;Author(s): X. W. Fu, X. Feng, L. H. Shang, S. F. Wang, and H. Zhang&lt;br /&gt;&lt;br /&gt;Total gaseous mercury (TGM) was continuously monitored at a remote site
(CBS) in the Mt. Changbai area, northeastern China biennially from 24 October 2008
to 31 October 2010. The overall mean TGM concentration was 1.60 &amp;plusmn; 0.51 ng m&lt;sup&gt;−3&lt;/sup&gt;,
which is lower than those reported from remote sites in eastern,
southwestern and western China, indicating a relatively low regional
anthropogenic mercury (Hg) emission intensity in northeastern China.
Measurements at a site in the vicinity (~1.2 km) of the CBS station during
August 2005 and July 2006 showed a significantly higher mean TGM concentration
of 3.58 &amp;plusmn; 1.78 ng m&lt;sup&gt;−3&lt;/sup&gt;. The divergent result was partially
attributed to fluctuations in the regional surface wind system and moreover
an effect of local emission sources. The temporal variation of TGM at CBS
was obviously influenced by regional sources as well as long-range
transported Hg. Regional sources, frequently contributing to episodical high
TGM concentrations, were pinpointed as a large iron mining district in
northern North Korea and two large power plants and urban areas to the
southwest of the sampling site. Source areas in Beijing, Tianjin, southern
Liaoning, Hebei, northwestern Shanxi and northwestern Shandong were found
to contribute to elevated TGM observations at CBS via long-range transport.
The diurnal pattern of TGM at CBS was mainly regulated by regional sources,
likely as well as intrusion of air masses from the free troposphere during
summer season. There are no discernible seasonal pattern of TGM at CBS,
which mainly showed links with the patterns of regional air movements and
long-range transport.</description><dc:date>2012-02-07T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4373/2012/"><title>Ice nuclei in marine air: bioparticles or dust?</title><link>http://www.atmos-chem-phys-discuss.net/12/4373/2012/</link><description>&lt;b&gt;Ice nuclei in marine air: bioparticles or dust?&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4373-4416, 2012&lt;br /&gt;&lt;br /&gt;Author(s): S. M. Burrows, C. Hoose, U. Pöschl, and M. G. Lawrence&lt;br /&gt;&lt;br /&gt;Ice nuclei can influence the properties of clouds and precipitation, but their sources and
      distribution in the atmosphere are still not well known. Particularly
      little attention has been paid to IN sources in marine environments,
      although anecdotal evidence suggests that IN populations in remote
      marine regions may be dominated by biological particles associated
      with sea spray. In this exploratory model study, we aim to bring
      attention to this long-neglected topic and identify promising target
      regions for future field campaigns. We assess the likely global
      distribution of marine biological ice nuclei using a combination of
      historical observations, satellite data and model output.  By
      comparing simulated marine biological IN distributions and dust IN
      distributions, we predict strong regional differences in the
      importance of marine biological IN relative to dust IN. Our analysis
      suggests that marine biological IN are most likely to play a dominant
      role in determining IN concentrations over the Southern Ocean, so
      future field campaigns aimed at investigating marine biological IN
      should target that region. Climate-related changes in the abundance
      and emission of biological marine IN could affect marine cloud
      properties, thereby introducing previously unconsidered feedbacks that
      influence the hydrological cycle and the Earth's energy
      balance. Furthermore, marine biological IN may be an important aspect
      to consider in proposals for marine cloud brightening by artificial
      sea spray production.</description><dc:date>2012-02-07T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4341/2012/"><title>AERONET and ESR sun direct products comparison performed on Cimel CE318 and Prede POM01 solar radiometers</title><link>http://www.atmos-chem-phys-discuss.net/12/4341/2012/</link><description>&lt;b&gt;AERONET and ESR sun direct products comparison performed on Cimel CE318 and Prede POM01 solar radiometers&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4341-4371, 2012&lt;br /&gt;&lt;br /&gt;Author(s): V. Estellés, M. Campanelli, T. J. Smyth, M. P. Utrillas, and J. A. Martínez-Lozano&lt;br /&gt;&lt;br /&gt;The &lt;i&gt;European Skynet Radiometers&lt;/i&gt; network (EuroSkyRad or ESR) has been
recently established as a research network of European Prede POM sun – sky
radiometers. Moreover, ESR is federated with SKYNET (SKYrad NETwork), an
international network mostly present in East Asia. In contrast to SKYNET, the
European network also integrates users of the Cimel CE318 sunphotometer.
Keeping instrumental duality in mind, a set of open source algorithms has
been developed consisting of two modules for: (1) the retrieval of direct sun
products from the sun extinction measurements; and (2) the inversion of the
sky radiance to derive aerosol optical properties. In this study we evaluate
the ESR direct sun products (spectral aerosol optical depth, Angström
wavelength exponent and columnar content of water vapour) in comparison with
the AERosol RObotic NETwork (AERONET) products. Specifically, we have applied
the ESR algorithm to a Cimel CE318 and Prede POM01L simultaneously for a 4 yr 
database measured at the Burjassot site (Valencia, Spain), and compared
the resultant products with the AERONET direct sun retrievals obtained with
the same Cimel CE318 instrument. The comparison show that aerosol optical
depth differences are mostly within the nominal uncertainty of 0.003 for a
standard calibration instrument, and fall within the nominal AERONET
uncertainty of 0.01–0.02 for a field instrument. Therefore, we present an
open source code that can be used for both radiometers and whose results are
comparable to those of AERONET and SKYNET.</description><dc:date>2012-02-07T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4311/2012/"><title>Quantifying retrieval uncertainties in the CM-SAF cloud physical property algorithm with simulated SEVIRI observations</title><link>http://www.atmos-chem-phys-discuss.net/12/4311/2012/</link><description>&lt;b&gt;Quantifying retrieval uncertainties in the CM-SAF cloud physical property algorithm with simulated SEVIRI observations&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4311-4340, 2012&lt;br /&gt;&lt;br /&gt;Author(s): B. J. Jonkheid, R. A. Roebeling, and E. van Meijgaard&lt;br /&gt;&lt;br /&gt;The uncertainties in the cloud physical properties derived from satellite
observations make it difficult to interpret model evaluation studies. In this
paper, the uncertainties in the cloud water path (CWP) retrievals derived
with the cloud physical properties retrieval algorithm (CPP) of the climate
monitoring satellite application facility (CM-SAF) are investigated. To this
end, a numerical simulator of MSG-SEVIRI observations was developed that
calculates the reflectances at 0.64 and 1.63 μm for a wide range of
cloud parameters, satellite viewing geometries and surface albedos. These
reflectances are used as input to CPP, and the retrieved values of CWP are
compared to the original input of the simulator.
&lt;br&gt;&lt;br&gt;
It is shown that the CWP retrievals are very sensitive to the assumptions
made in the CPP code. The CWP retrieval errors are generally small for
unbroken single-phase clouds with COT &gt;10, with retrieval errors of
~3% for liquid water clouds to ~10% for ice clouds. When both
liquid water and ice clouds are present in a pixel, the CWP retrieval errors
increase dramatically; depending on the cloud, this can lead to uncertainties
of 40–80%. CWP retrievals also become more uncertain when the cloud does
not cover the entire pixel, leading to errors of ~50% for cloud
fractions of 0.75 and even larger errors for smaller cloud fractions. Thus,
the satellite retrieval of cloud physical properties of broken clouds and
multi-phase clouds is complicated by inherent difficulties, and the proper
interpretation of such retrievals requires extra care.</description><dc:date>2012-02-07T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4279/2012/"><title>An observation-based approach to identify local natural dust events from routine aerosol ground  monitoring</title><link>http://www.atmos-chem-phys-discuss.net/12/4279/2012/</link><description>&lt;b&gt;An observation-based approach to identify local natural dust events from routine aerosol ground  monitoring&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4279-4310, 2012&lt;br /&gt;&lt;br /&gt;Author(s): D. Q. Tong, M. Dan, T. Wang, and P. Lee&lt;br /&gt;&lt;br /&gt;Dust is a major component of atmospheric aerosols in many parts of the world. Although there exist
  many routine aerosol monitoring networks, it is often difficult to obtain dust records from these
  networks, because these monitors are either deployed far away from dust active regions (most
  likely collocated with dense population) or contaminated by anthropogenic sources and other
  natural sources, such as wildfires and vegetation detritus. Here we propose a new approach to
  identify local dust events relying solely on aerosol mass and composition from general-purpose
  aerosol measurements.  Through analyzing the chemical and physical characteristics of aerosol
  observations during satellite-detected dust episodes, we select five indicators to be used to
  identify local dust records: (1) high PM&lt;sub&gt;10&lt;/sub&gt; concentrations; (2) low
  PM&lt;sub&gt;2.5&lt;/sub&gt;/PM&lt;sub&gt;10&lt;/sub&gt; ratio; (3) higher concentrations and percentage of crustal
  elements; (4) lower percentage of anthropogenic pollutants; and (5) low enrichment factors of
  anthropogenic elements. After establishing these identification criteria, we conduct hierarchical
  cluster analysis for all validated aerosol measurement data over 68 IMPROVE sites in the Western
  United States. A total of 182 local dust events were identified over 30 of the 68 locations from
  2000 to 2007. These locations are either close to the four US Deserts, namely the Great Basin
  Desert, the Mojave Desert, the Sonoran Desert, and the Chihuahuan Desert, or in the high wind
  power region (Colorado). During the eight-year study period, the total number of dust events
  displays an interesting four-year activity cycle (one in 2000–2003 and the other in
  2004–2007). The years of 2003, 2002 and 2007 are the three most active dust periods, with 46, 31
  and 24 recorded dust events, respectively, while the years of 2000, 2004 and 2005 are the calmest
  periods, all with single digit dust records. Among these deserts, the Chihuahua Desert (59 cases)
  and the Sonoran Desert (62 cases) are by far the most active source regions. In general, the
  Chihuahua Desert dominates dust activities in the first half of the eight-year period while the
  Sonoran Desert in the second half. The monthly frequency of dust events shows a peak from March to
  July and a second peak in autumn from September to November.  The large quantity of dust events
  occurring in summertime also suggests the prevailing impact of windblown dust across the
  year. This seasonal variation is consistent with previous model simulations over the United
  States.</description><dc:date>2012-02-07T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4243/2012/"><title>Determinants and predictability of global wildfire emissions</title><link>http://www.atmos-chem-phys-discuss.net/12/4243/2012/</link><description>&lt;b&gt;Determinants and predictability of global wildfire emissions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4243-4278, 2012&lt;br /&gt;&lt;br /&gt;Author(s): W. Knorr, V. Lehsten, and A. Arneth&lt;br /&gt;&lt;br /&gt;Biomass burning is one of the largest sources of atmospheric trace gases
and aerosols globally. These emissions have a major impact on the radiative
balance of the atmosphere and on air quality, and are thus of significant
scientific and societal interest. Several datasets have been developed that
quantify those emissions on a global grid and offered to the atmospheric
modelling community. However, no study has yet attempted to systematically
quantify the dependence of the inferred pyrogenic emissions on underlying
assumptions and input data. Such a sensitivity study is needed for
understanding how well we can currently model those emissions and what the
factors are that contribute to uncertainties in those emissions estimates.
&lt;br&gt;&lt;br&gt;
Here, we combine various satellite-derived burned area products, a
terrestrial ecosystem model to simulate fuel loads and the effect of fire on
ecosystem dynamics, a model of fuel combustion, and various emission models
that relate combusted biomass to the emission of various trace gases and
aerosols. We vary one key parameter of a simple fuel combustion model, the
emission model, and the burned area product and assess its impact on the
computed emissions fields and their uncertainties. We find that choice of
burned area data set has by far the largest impact on interannual
variability of simulated emissions. For total global emissions, burned area
and combustion completeness have the largest impact on emissions for most
species.
&lt;br&gt;&lt;br&gt;
We conclude that reliable information on burned area is key for accurately
modelling spatial and interannual variations of wildfire emissions, but
uncertainties about the combustion process have a similar impact on the
magnitude of global emission estimates. The results are important for
chemical transport modelling studies, and for simulations of biomass burning
impacts on the atmosphere under future climate change scenarios.</description><dc:date>2012-02-06T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4221/2012/"><title>Anthropogenic changes in the surface all-sky UV-B radiation through 1850&amp;ndash;2005 simulated by an Earth system model</title><link>http://www.atmos-chem-phys-discuss.net/12/4221/2012/</link><description>&lt;b&gt;Anthropogenic changes in the surface all-sky UV-B radiation through 1850&amp;ndash;2005 simulated by an Earth system model&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4221-4242, 2012&lt;br /&gt;&lt;br /&gt;Author(s): S. Watanabe, T. Takemura, K. Sudo, T. Yokohata, and H. Kawase&lt;br /&gt;&lt;br /&gt;The historical anthropogenic change in the surface all-sky UV-B (solar
      ultraviolet: 280–315 nm) radiation through 1850–2005 is evaluated
      using an Earth system model. Responses of UV-B dose to anthropogenic
      changes in ozone and aerosols are separately evaluated using a series
      of historical simulations including/excluding these changes. Increases
      in these air pollutants cause reductions in UV-B transmittance, which
      occur gradually/rapidly before/after 1950 in and downwind of
      industrial and deforestation regions. Furthermore, changes in ozone
      transport in the lower stratosphere, which is induced by increasing
      greenhouse gas concentrations, increase ozone concentration in the
      extratropical upper troposphere and lower stratosphere. These
      transient changes work to decrease the amount of UV-B reaching the
      Earth's surface, counteracting the well-known effect increasing UV-B
      due to stratospheric ozone depletion, which developed rapidly after
      ca. 1980. As a consequence, the surface all-sky UV-B radiation change
      between 1850 and 2000 is negative in the tropics and NH extratropics
      and positive in the SH extratropics. Comparing the contributions of
      ozone and aerosol changes to the UV-B change, the transient change in
      ozone absorption of UV-B mainly determines the total change in the
      surface all-sky UV-B radiation at most locations. On the other hand,
      the aerosol direct and indirect effects on UV-B play an equally
      important role to that of ozone in the NH mid-latitudes and
      tropics. A typical example is East Asia
      (25&amp;deg; N–60&amp;deg; N and 120&amp;deg; E–150&amp;deg; E),
      where the effect of aerosols (ca. 70%) dominates the total UV-B
      change.</description><dc:date>2012-02-06T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4185/2012/"><title>Climatological perspectives of air transport from atmospheric boundary  layer to tropopause layer over Asian monsoon regions during boreal summer  inferred from Lagrangian approach</title><link>http://www.atmos-chem-phys-discuss.net/12/4185/2012/</link><description>&lt;b&gt;Climatological perspectives of air transport from atmospheric boundary  layer to tropopause layer over Asian monsoon regions during boreal summer  inferred from Lagrangian approach&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4185-4219, 2012&lt;br /&gt;&lt;br /&gt;Author(s): B. Chen, X. D. Xu, S. Yang, and T. L. Zhao&lt;br /&gt;&lt;br /&gt;The Asian Summer Monsoon (ASM) region has been recognized as a key
      region that plays a vital role in troposphere-to-stratosphere
      transport (TST), which can significantly impact the budget of global
      atmospheric constituents and climate change. However, the details of
      transport from the boundary layer (BL) to tropopause layer (TL) over
      this region, particularly from a climatological perspective, remains
      an issue of uncertainty. In this study, we present the
      climatological properties of BL-to-TL transport over the ASM region
      during boreal summer season (June-July-August) from 2001 to
      2009. A comprehensive tracking analysis is conducted based on a large
      ensemble of TST-trajectories departing from the atmospheric BL and
      arriving at TL. Driven by the winds fields from the NCEP/NCAR (National Centers for Environmental Prediction/National Center for Atmospheric Research) Global
      Forecast System, all TST-trajectories are selected from the high
      resolution datasets generated by the Lagrangian particle transport
      model FLEXPART using a domain-filling technique. Three key atmospheric
      boundary layer sources for BL-to-TL transport are identified with
      their contributions: (i) 38% from the region between tropical Western
      Pacific region and South China Seas (WP), (ii) 21% from Bay of Bengal
      and South Asian subcontinent (BOB), and (iii) 12% from the Tibetan
      Plateau, which includes the South Slope of the Himalayas (TIB). Controlled
      by the different patterns of atmospheric circulation, the air masses
      originating from these three source regions are transported along the
      different tracks into the TL. The spatial distributions of these three
      source regions remain similarly from year to year. The timescales of
      transport from BL to TL by the large-scale ascents range from 1 to 7
      weeks, contributing up to 60–70% of the overall TST; whereas the
      transport governed by the deep convection overshooting becomes faster,
      with timescales of 1–2 days and contributions of
      20–30%. These results provide clear policy implications for the
      control of very short lived substances, especially for the source
      regions over the Indian subcontinent with increasing populations and
      developing industries.</description><dc:date>2012-02-06T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4165/2012/"><title>Atmospheric histories and growth trends of C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;, C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;, C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;</title><link>http://www.atmos-chem-phys-discuss.net/12/4165/2012/</link><description>&lt;b&gt;Atmospheric histories and growth trends of C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;, C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;, C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4165-4184, 2012&lt;br /&gt;&lt;br /&gt;Author(s): D. J. Ivy, T. Arnold, C. M. Harth, L. P. Steele, J. Mühle, M. Rigby, P. K. Salameh, M. Leist, P. B. Krummel, P. J. Fraser, R. F. Weiss, and R. G. Prinn&lt;br /&gt;&lt;br /&gt;The first atmospheric observations and trends are presented
      for the high molecular weight perfluorocarbons (PFCs):
      decafluorobutane (C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;), dodecafluoropentane
      (C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;), tetradecafluorohexane (C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;),
      hexadecafluoroheptane (C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt;) and
      octadecafluorooctane (C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;). Their atmospheric
      histories are based on measurements of 38 Northern Hemisphere
      and 46 Southern Hemisphere archived air samples collected
      between 1973 to 2011 using the Advanced Global Atmospheric
      Gases Experiment (AGAGE) &quot;Medusa&quot; preconcentration gas
      chromatography-mass spectrometry systems. A new calibration
      scale was prepared for each PFC, with estimated accuracies of
      6.8% for C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, 7.8% for
      C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;, 4.0% for C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;, 6.6%
      for C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and 7.9% for C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;. Based
      on our observations the 2011 globally averaged dry air mole
      fractions of these heavy PFCs are: 0.18 parts-per-trillion
      (ppt, i.e., parts per 10&lt;sup&gt;12&lt;/sup&gt;) for C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, 0.12
      ppt for C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;, 0.28 ppt for C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;, 0.12
      ppt for C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and 0.09 ppt for
      C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;. These atmospheric mole fractions combine to
      contribute to a global average radiative forcing of
      0.35 mW m&lt;sup&gt;−2&lt;/sup&gt;, which is 3.6% of the total PFC
      radiative forcing. The globally averaged mean atmospheric
      growth rates of these PFCs during 1973–2011 are 4.58 parts
      per quadrillion (ppq, i.e., parts per 10&lt;sup&gt;15&lt;/sup&gt;) per year (yr)
      for C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, 3.29 ppq yr&lt;sup&gt;−1&lt;/sup&gt; for
      C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;, 7.50 ppq yr&lt;sup&gt;−1&lt;/sup&gt; for C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;,
      3.19 ppq yr&lt;sup&gt;−1&lt;/sup&gt; for C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and
      2.51 ppq yr&lt;sup&gt;−1&lt;/sup&gt; for C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;. The growth rates of
      the heavy perfluorocarbons were largest in the early 1990s for
      C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt; and C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt; and in the mid-to-late
      1990s for C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;, C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; and
      C&lt;sub&gt;8&lt;/sub&gt;F&lt;sub&gt;18&lt;/sub&gt;. The more recent slow down in the growth
      rates of the high molecular weight PFCs suggests that
      emissions are declining as compared to the 1980s and
      1990s. Nevertheless continued monitoring of these potent,
      extremely long-lived greenhouse gases is necessary to verify
      that global PFC emissions continue to decline.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4101/2012/"><title>Central Arctic atmospheric summer conditions during the Arctic Summer Cloud  Ocean Study (ASCOS): contrasting to previous expeditions</title><link>http://www.atmos-chem-phys-discuss.net/12/4101/2012/</link><description>&lt;b&gt;Central Arctic atmospheric summer conditions during the Arctic Summer Cloud  Ocean Study (ASCOS): contrasting to previous expeditions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4101-4164, 2012&lt;br /&gt;&lt;br /&gt;Author(s): M. Tjernström, C. E. Birch, I. M. Brooks, M. D. Shupe, P. O. G. Persson, J. Sedlar, T. Mauritsen, C. Leck, J. Paatero, M. Szczodrak, and C. R. Wheeler&lt;br /&gt;&lt;br /&gt;Understanding the rapidly changing climate in the Arctic is limited by
      a lack of understanding of underlying strong feedback mechanisms that
      are specific to the Arctic. Progress in this field can only be
      obtained by process-level observations; this is the motivation for
      intensive ice-breaker-based campaigns such as that described in this
      paper: the Arctic Summer Cloud-Ocean Study (ASCOS). However, detailed field observations also have to be put in the context of the larger-scale
      meteorology, and short field campaigns have to be analysed within the
      context of the underlying climate state and temporal anomalies from
      this.
&lt;br&gt;&lt;/br&gt;
      To aid in the analysis of other parameters or processes observed
      during this campaign, this paper provides an overview of the
      synoptic-scale meteorology and its climatic anomaly during the ASCOS
      field deployment. It also provides a statistical analysis of key
      features during the campaign, such as some key meteorological
      variables, the vertical structure of the lower troposphere and clouds,
      and energy fluxes at the surface. In order to assess the
      representativity of the ASCOS results, we also compare these features
      to similar observations obtained during three earlier summer
      experiments in the Arctic Ocean, the AOE-96, SHEBA and AOE-2001
      expeditions.
&lt;br&gt;&lt;/br&gt;
      We find that these expeditions share many key features of the
      summertime lower troposphere. Taking ASCOS and the previous
      expeditions together, a common picture emerges with a large
      amount of low-level cloud in a well-mixed shallow boundary layer,
      capped by a weak to moderately strong inversion where moisture, and
      sometimes also cloud top, penetrate into the lower parts of the
      inversion. Much of the boundary-layer mixing is due to cloud-top
      cooling and subsequent buoyant overturning of the cloud. The cloud
      layer may, or may not, be connected with surface processes depending
      on the depths of the cloud and surface-based boundary layers and on
      the relative strengths of surface-shear and cloud-buoyancy turbulence
      generation. The latter also implies a connection between the cloud
      layer and the free troposphere through entrainment at cloud top.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4073/2012/"><title>Distributions, long term trends and emissions of four perfluorocarbons  in remote parts of the atmosphere and firn air</title><link>http://www.atmos-chem-phys-discuss.net/12/4073/2012/</link><description>&lt;b&gt;Distributions, long term trends and emissions of four perfluorocarbons  in remote parts of the atmosphere and firn air&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4073-4100, 2012&lt;br /&gt;&lt;br /&gt;Author(s): J. C. Laube, C. Hogan, M. J. Newland, F. S. Mani, P. J. Fraser, C. A. M. Brenninkmeijer, P. Martinerie, D. E. Oram, T. Röckmann, J. Schwander, E. Witrant, G. P. Mills, C. E. Reeves, and W. T. Sturges&lt;br /&gt;&lt;br /&gt;We report the first data set of atmospheric abundances for the
      following four perfluoroalkanes: &lt;i&gt;n&lt;/i&gt;-decafluorobutane
      (&lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;), &lt;i&gt;n&lt;/i&gt;-dodecafluoropentane
      (&lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;), &lt;i&gt;n&lt;/i&gt;-tetradecafluorohexane
      (&lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;) and &lt;i&gt;n&lt;/i&gt;-hexadecafluoroheptane
      (&lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt;). All four compounds could be detected
      and quantified in air samples from remote locations in the Southern
      Hemisphere (at Cape Grim, Tasmania, archived samples dating back to
      1978) and the upper troposphere (a passenger aircraft flying from
      Germany to South Africa). Further observations originate from air
      samples extracted from deep firn in Greenland and allow trends of
      atmospheric abundances in the earlier 20th century to be inferred. All
      four compounds were not present in the atmosphere prior to the
      1960s. &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt; and &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt;
      were also measured in samples collected in the stratosphere confirming
      their very long atmospheric lifetimes. Emissions were inferred from
      these observations and found to be comparable with emissions from the
      EDGAR database for &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;6&lt;/sub&gt;F&lt;sub&gt;14&lt;/sub&gt;. However, emissions
      of &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;4&lt;/sub&gt;F&lt;sub&gt;10&lt;/sub&gt;, &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;5&lt;/sub&gt;F&lt;sub&gt;12&lt;/sub&gt; and
      &lt;i&gt;n&lt;/i&gt;-C&lt;sub&gt;7&lt;/sub&gt;F&lt;sub&gt;16&lt;/sub&gt; were found to differ by up to five
      orders of magnitude. Although the abundances of the four
      perfluorocarbons reported here are currently small (less than
      0.3 ppt, parts per trillion) they have
      strong Global Warming Potentials several thousand times higher than
      carbon dioxide and continue to increase in the atmosphere. The sum of
      their cumulative emissions reached 325 mt (million metric tonnes)
      CO&lt;sub&gt;2&lt;/sub&gt; equivalent at the end of
      2009.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/4031/2012/"><title>Retrieval of aerosol optical depth over land based on a time series technique using MSG/SERIVI data</title><link>http://www.atmos-chem-phys-discuss.net/12/4031/2012/</link><description>&lt;b&gt;Retrieval of aerosol optical depth over land based on a time series technique using MSG/SERIVI data&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 4031-4071, 2012&lt;br /&gt;&lt;br /&gt;Author(s): L. Mei, Y. Xue, G. de Leeuw, T. Holzer-Popp, J. Guang, Y. Li, L. Yang, H. Xu, X. Xu, C. Li, Y. Wang, C. Wu, T. Hou, X. He, J. Liu, J. Dong, and Z. Chen&lt;br /&gt;&lt;br /&gt;A novel approach for the joint retrieval of aerosol optical depth (AOD) and
surface reflectance, using Meteosat Second Generation – Spinning Enhanced
Visible and Infrared Imagers (MSG/SEVIRI) observations in two solar
channels, is presented. The retrieval is based on a time series (TS)
technique, which makes use of the two visible bands at 0.6 μm and
0.8 μm in three orderly scan times (15 min interval between two scans)
to retrieve the AOD over land. Using the radiative transfer equation for
plane-parallel atmospheres two coupled differential equations for the upward
and downward fluxes are derived. The boundary conditions for the upward and
downward fluxes at the top and at the bottom of the atmosphere are used in
these equations to provide an analytic solution for the surface reflectance.
To derive these fluxes, the aerosol single scattering albedo (SSA)  and asymmetry
factor are required to provide a solution. These are provided from a set of
six pre-defined aerosol types with the SSA and
asymmetry factor (&lt;i&gt;g&lt;/i&gt;). We assume one aerosol type for a grid of 1° × 1°
and the surface reflectance changes little between two consequent scans. A
&lt;i&gt;k&lt;/i&gt; approximation was used in the inversion to find the best solution of
atmospheric properties and surface reflectance. The algorithm makes use of
numerical minimisation routines to obtain the optimal solution of
atmospheric properties and surface reflectance by selection of the most
suitable aerosol type from pre-defined sets. Also, it is assumed that the
surface reflectance is little influenced by aerosol scattering at 1.6 μm
and therefore the ratio of surface reflectances in the solar band for two
consequent scans can be well-approximated by the ratio of the reflectances
at 1.6 μm. A further assumption is that the surface reflectance varies
only slightly over a period of 30 min.
&lt;br&gt;&lt;br&gt;
A detailed analysis of the retrieval results show that it is suitable for
AOD retrieval over land. Six Aerosol Robotic Network (AERONET) sites with different surface types
were used for detailed analysis and 42 other AERONET sites were used for
validation. From 445 collocations representing stable and homogeneous
aerosol type, we found that &gt;75% of MSG-retrieved AOD values compared
to AERONET observed values with an error envelope of &amp;plusmn;0.05 &amp;plusmn; 0.15&amp;tau; and a high correlation
(&lt;i&gt;R&lt;/i&gt; &gt; 0.86). The AOD datasets derived using the TS method with SEVIRI data
was also compared with collocated AOD products derived from the NASA TERRA
and AQUA MODIS data using the dark dense vegetation (DDV) method and the
Deep Blue algorithms. Using the TS method, AOD could be retrieved for more
pixels than with the NASA Deep Blue algorithm. The AOD values derived
compare favourably.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3983/2012/"><title>MAX-DOAS measurements of NO&lt;sub&gt;2&lt;/sub&gt;, HCHO and CHOCHO at a rural site in Southern China</title><link>http://www.atmos-chem-phys-discuss.net/12/3983/2012/</link><description>&lt;b&gt;MAX-DOAS measurements of NO&lt;sub&gt;2&lt;/sub&gt;, HCHO and CHOCHO at a rural site in Southern China&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3983-4029, 2012&lt;br /&gt;&lt;br /&gt;Author(s): X. Li, T. Brauers, A. Hofzumahaus, K. Lu, Y. P. Li, M. Shao, T. Wagner, and A. Wahner&lt;br /&gt;&lt;br /&gt;We performed MAX-DOAS measurements during the PRIDE-PRD2006 campaign
      in the Pearl River Delta region (PRD), China, for 4 weeks in July 2006
      at a site located 60 km north of Guangzhou. The vertical
      distributions of NO&lt;sub&gt;2&lt;/sub&gt;, HCHO, and CHOCHO were
      independently retrieved by an automated iteration method. The MAX-DOAS
      measured NO&lt;sub&gt;2&lt;/sub&gt; mixing ratios showed reasonable agreement with
      the simultaneous, ground based in-situ data. While the tropospheric
      NO&lt;sub&gt;2&lt;/sub&gt; vertical column densities (VCDs) observed by OMI on board
      EOS-Aura satellite agreed with those by MAX-DOAS, the 3-D chemical
      transport model CMAQ overestimated the NO&lt;sub&gt;2&lt;/sub&gt; VCDs as well as the
      surface concentrations by about 40%. From this observation,
      a reduction of NO&lt;sub&gt;X&lt;/sub&gt; emission strength in CMAQ seems to be
      necessary in order to well reproduce the NO&lt;sub&gt;2&lt;/sub&gt; observations. The
      average mixing ratios of HCHO and CHOCHO were 12 ppb
      and 1.6 ppb, respectively, substantially higher than in other rural
      or semirural environments. The high ratio of 0.135 between
      CHOCHO and HCHO corresponds to the high VOCs reactivity
      and high HO&lt;sub&gt;X&lt;/sub&gt; turnover rate consistent with other observations
      during the campaign.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3941/2012/"><title>Tropospheric methanol observations from space: retrieval evaluation  and constraints on the seasonality of biogenic emissions</title><link>http://www.atmos-chem-phys-discuss.net/12/3941/2012/</link><description>&lt;b&gt;Tropospheric methanol observations from space: retrieval evaluation  and constraints on the seasonality of biogenic emissions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3941-3982, 2012&lt;br /&gt;&lt;br /&gt;Author(s): K. C. Wells, D. B. Millet, L. Hu, K. E. Cady-Pereira, Y. Xiao, M. W. Shephard, C. L. Clerbaux, L. Clarisse, P.-F. Coheur, E. C. Apel, J. de Gouw, C. Warneke, H. B. Singh, A. H. Goldstein, and B. C. Sive&lt;br /&gt;&lt;br /&gt;Methanol retrievals from nadir-viewing space-based sensors offer
      powerful new information for quantifying methanol emissions on
      a global scale. Here we apply an ensemble of aircraft observations
      over North America to evaluate new methanol measurements from the
      Tropospheric Emission Spectrometer (TES) on the Aura satellite, and
      combine the TES data with observations from the Infrared Atmospheric
      Sounding Interferometer (IASI) on the MetOp-A satellite to investigate
      the seasonality of methanol emissions from northern midlatitude
      ecosystems. Using the GEOS-Chem chemical transport model as an
      intercomparison platform, we find that the TES retrieval performs well
      when the degrees of freedom for signal (DOFS) are above 0.5, in which
      case the model : TES regressions are generally consistent with the
      model : aircraft comparisons. Including retrievals with DOFS below
      0.5 degrades the comparisons, as these are excessively influenced by
      the a priori. The comparisons suggest DOFS &gt; 0.5 as a minimum
      threshold for interpreting retrievals of trace gases with a weak
      tropospheric signal. We analyze one full year of satellite
      observations and find that GEOS-Chem, driven with MEGANv2.1 biogenic
      emissions, underestimates observed methanol concentrations throughout
      the midlatitudes in springtime, with the timing of the seasonal peak
      in model emissions 1–2 months too late. We attribute this
      discrepancy to an underestimate of emissions from new leaves in MEGAN,
      and apply the satellite data to better quantify the seasonal change in
      methanol emissions for midlatitude ecosystems. The derived parameters
      (relative emission factors of 11.0, 1.0, 0.05 and 8.6 for new,
      growing, mature, and old leaves, respectively, plus a leaf area index
      activity factor of 0.75 for expanding canopies with leaf area
      index &lt; 2.0) provide a more realistic simulation of seasonal
      methanol concentrations in midlatitudes on the basis of IASI, TES, and
      ground-based measurements.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3875/2012/"><title>Projections of mid-century summer air-quality for North America: effects of changes in climate and precursor emissions</title><link>http://www.atmos-chem-phys-discuss.net/12/3875/2012/</link><description>&lt;b&gt;Projections of mid-century summer air-quality for North America: effects of changes in climate and precursor emissions&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3875-3940, 2012&lt;br /&gt;&lt;br /&gt;Author(s): J. Kelly, P. A. Makar, and D. A. Plummer&lt;br /&gt;&lt;br /&gt;Ten year simulations of North American current and future air-quality were
carried out using a regional air-quality model driven by a regional climate
model, in turn driven by a general circulation model. Three separate summer
scenarios were performed: a scenario representing the years 1997 to 2006,
and two SRES A2 climate scenarios for the years 2041 to 2050. The first
future climate scenario makes use of 2002 anthropogenic precursor emissions,
and the second applied emissions scaling factors derived from the IPCC
Representative Concentration Pathway 6 (RCP 6) scenario to estimate
emissions for 2050 from existing 2020 projections. Ten-year averages of
ozone and PM&lt;sub&gt;2.5&lt;/sub&gt; at North American monitoring network stations were used
to evaluate the model's current chemical climatology. The model was found to
have a similar performance for ozone as when driven by an operational
weather forecast model. The PM&lt;sub&gt;2.5&lt;/sub&gt; predictions had larger negative
biases, likely resulting from the absence of rainwater evaporation, and from
sub-regional negative biases in the surface temperature fields, in the
version of the climate model used here.
&lt;br&gt;&lt;br&gt;
The differences between the two future climate simulations and the current
climate simulation were used to predict the changes to air-quality that
might be expected in a future warmer climate, if anthropogenic precursor
emissions remain constant at their current levels, versus if the RCP 6
emissions controls were adopted. Metrics of concentration, human health, and
ecosystem damage were compared for the simulations. The scenario with future
climate and current anthropogenic emissions resulted in worse air-quality
than for current conditions – that is, the effect of climate-change alone,
all other factors being similar, would be a worsening of air-quality. These
effects are spatially inhomogeneous, with the magnitude and sign of the
changes varying with region. The scenario with future climate and RCP 6
emissions for 2050 resulted in an improved air-quality, with decreases in
key pollutant concentrations, in acute human mortality associated with
air-pollution, and in sulphur and ozone deposition to the ecosystem. The
positive outcomes of the RCP 6 emissions reductions were found to be of
greater magnitude than the negative outcomes of climate change alone. The
RCP 6 scenario however resulted in an increase in the deposition of
nitrogen, as a result of increased ammonia emissions expected in that
scenario, compared to current ammonia emissions levels.
&lt;br&gt;&lt;br&gt;
The results of the study raise the possibility that simultaneous reductions
of greenhouse gases and air pollution precursors may further reduce air
pollution levels, with the added benefits of an immediate reduction in the
impacts of air pollution on human and ecosystem health. Further scenarios to
investigate this possibility are therefore recommended.</description><dc:date>2012-02-03T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3781/2012/"><title>The EMEP MSC-W chemical transport model &amp;ndash; Part 1: Model description</title><link>http://www.atmos-chem-phys-discuss.net/12/3781/2012/</link><description>&lt;b&gt;The EMEP MSC-W chemical transport model &amp;ndash; Part 1: Model description&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3781-3874, 2012&lt;br /&gt;&lt;br /&gt;Author(s): D. Simpson, A. Benedictow, H. Berge, R. Bergström, L. D. Emberson, H. Fagerli, G. D. Hayman, M. Gauss, J. E. Jonson, M. E. Jenkin, A. Nyíri, C. Richter, V. S. Semeena, S. Tsyro, J.-P. Tuovinen, Á. Valdebenito, and P. Wind&lt;br /&gt;&lt;br /&gt;The Meteorological Synthesizing Centre-West (MSC-W) of
the European Monitoring and Evaluation Programme (EMEP)  has been performing
model calculations in support of the Convention on Long Range Transboundary Air Pollution (CLRTAP)
for more than 30 yr.
The EMEP MSC-W chemical transport model is still one of the key tools within
European air pollution policy assessments.
&lt;br&gt;&lt;br&gt;
Traditionally, the EMEP  model has covered all of Europe with
a resolution of about 50 × 50 km&lt;sup&gt;2&lt;/sup&gt;,
and extending vertically from ground
level to the tropopause (100 hPa). The model has undergone substantial
development in recent years, and is now applied on scales
ranging from local (ca. 5 km grid size) to global (with 1 degree
resolution).
The  model is used to simulate photo-oxidants and
both inorganic and organic aerosols.
&lt;br&gt;&lt;br&gt;
In 2008 the EMEP model was released for the first time as public domain
code, along with all required input data for model runs for one year.
Since then, many changes have been made to the model physics, and input data.
The second release of the EMEP MSC-W model
became available in mid
2011, and a new release is targeted for early 2012.  This publication is
intended to document this third release of the EMEP MSC-W model.
The model formulations are given, along with details
of input data-sets which are used, and brief background
on some of the choices made in the formulation are
presented.
The model code itself is available at 
&lt;a href=&quot;http://www.emep.int&quot;target=&quot;_blank&quot;&gt;www.emep.int&lt;/a&gt;, along with
the data required to  run for a full year over Europe.</description><dc:date>2012-02-02T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3731/2012/"><title>Lessons learnt from the first EMEP intensive measurement periods</title><link>http://www.atmos-chem-phys-discuss.net/12/3731/2012/</link><description>&lt;b&gt;Lessons learnt from the first EMEP intensive measurement periods&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3731-3780, 2012&lt;br /&gt;&lt;br /&gt;Author(s): W. Aas, S. Tsyro, E. Bieber, R. Bergström, D. Ceburnis, T. Ellermann, H. Fagerli, M. Frölich, R. Gehrig, U. Makkonen, E. Nemitz, R. Otjes, N. Perez, C. Perrino, A. S. H. Prévôt, J.-P. Putaud, D. Simpson, G. Spindler, M. Vana, and K. E. Yttri&lt;br /&gt;&lt;br /&gt;The first EMEP intensive measurement periods were held in June 2006 and
January 2007. The measurements aimed to characterize the aerosol chemical
compositions, including the gas/aerosol partitioning of inorganic compounds.
The measurement program during these periods included daily or hourly
measurements of the secondary inorganic components, with additional
measurements of elemental- and organic carbon (EC and OC) and mineral dust
in PM&lt;sub&gt;1&lt;/sub&gt;, PM&lt;sub&gt;2.5&lt;/sub&gt; and PM&lt;sub&gt;10&lt;/sub&gt;. These measurements have provided
extended knowledge regarding the composition of particulate matter and the
temporal and spatial variability of PM, as well as an extended database for
the assessment of chemical transport models. This paper summarise the first
experiences of making use of measurements from the first EMEP intensive
measurement periods along with EMEP model results from the updated model
version to characterise aerosol composition. We investigated how the PM
chemical composition varies between the summer and the winter month and
geographically.
&lt;br&gt;&lt;br&gt;
The observation and model data are in general agreement regarding the main
features of PM&lt;sub&gt;10&lt;/sub&gt; and PM&lt;sub&gt;2.5&lt;/sub&gt; composition and the relative
contribution of different components, though the EMEP model tends to
slightly underestimate PM&lt;sub&gt;10&lt;/sub&gt; and PM&lt;sub&gt;2.5&lt;/sub&gt; compared to measurements.
The intensive measurement data has identified areas where improvements are
needed. In particular, the model description of formation of coarse nitrate
on sea salt and dust particles requires further attention. Hourly concurrent
measurements of gaseous and particulate components for the first time
facilitated testing of modelled diurnal variability of the gas/aerosol
partitioning of nitrogen species. In general, the modelled diurnal cycles of
nitrate and ammonium aerosols are in good agreement with the measurements.
As expected, the diurnal variability of ammonia is not very well captured,
but this will probably improve if the EMEP model is coupled to a dynamic,
mechanistic ammonia emission module. The largest underestimations of aerosol
mass are seen in Italy during winter, which to a large extent may be
explained by an underestimation of residential wood burning source. It
should be noted that both primary and secondary OC has been included in the
calculations for the first time, showing promising results. Mineral dust is
important, especially in southern Europe, and the model seems to capture the
dust episodes well. The lack of measurements of mineral dust hampers the
possibility for model evaluation for this highly uncertain PM component.
&lt;br&gt;&lt;br&gt;
There are also lessons learnt regarding improved measurements for future
intensive periods. There is a need for increased comparability between the
measurements at different sites. For the nitrogen compounds it is clear that
more measurements using artefact free methods based on continuous
measurement methods and/or denuders are needed. For EC/OC, a reference
methodology (both in field and laboratory) was lacking during these periods
giving problems with comparability, though presently measurement protocols
have been established and these should be followed by the Parties to the
EMEP Protocol. For measurements with no defined protocols, it might be a
good solution to use centralised laboratories to ensure comparability across
the network. To cope with the introduction of these new measurements new
reporting guidelines have been developed to ensure that all proper
information about the methodologies and data quality is given.</description><dc:date>2012-02-02T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3695/2012/"><title>Regional air-quality forecasting for the Pacific Northwest using MOPITT/TERRA assimilated carbon monoxide MOZART-4 forecasts as a near real-time boundary condition</title><link>http://www.atmos-chem-phys-discuss.net/12/3695/2012/</link><description>&lt;b&gt;Regional air-quality forecasting for the Pacific Northwest using MOPITT/TERRA assimilated carbon monoxide MOZART-4 forecasts as a near real-time boundary condition&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3695-3730, 2012&lt;br /&gt;&lt;br /&gt;Author(s): F. L. Herron-Thorpe, G. H. Mount, L. K. Emmons, B. K. Lamb, S. H. Chung, and J. K. Vaughan&lt;br /&gt;&lt;br /&gt;Results from a regional air quality forecast model, AIRPACT-3, were compared
to AIRS carbon monoxide column densities for the spring of 2010 over the
Pacific Northwest. AIRPACT-3 column densities showed high correlation
(&lt;i&gt;R&lt;/i&gt;&gt;0.9) but were significantly biased (~25 %) with significant
under-predictions for spring months with significant transport from Asia. The
AIRPACT-3 CO bias relative to AIRS was eliminated by incorporating dynamic
boundary conditions derived from NCAR's MOZART forecasts with assimilated
MOPITT carbon monoxide. Changes in ozone-related boundary conditions derived
from MOZART forecasts are also discussed and found to affect background
levels by ±10 ppb but not found to significantly affect peak ozone
surface concentrations.</description><dc:date>2012-02-02T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3655/2012/"><title>Biogenic influence on cloud microphysics over the global ocean</title><link>http://www.atmos-chem-phys-discuss.net/12/3655/2012/</link><description>&lt;b&gt;Biogenic influence on cloud microphysics over the global ocean&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3655-3694, 2012&lt;br /&gt;&lt;br /&gt;Author(s): A. Lana, R. Simó, S. M. Vallina, and J. Dachs&lt;br /&gt;&lt;br /&gt;Aerosols have a large potential to influence climate through their
      effects on the microphysics and optical properties of clouds and,
      hence, on the Earth's radiation budget. Aerosol-cloud interactions
      have been intensively studied in polluted air, but the possibility
      that the marine biosphere plays a role in regulating cloud
      brightness in the pristine oceanic atmosphere remains largely
      unexplored. We used 9 yr of global satellite data and ocean
      climatologies to derive parameterizations of (a) production fluxes of
      sulfur aerosols formed by the oxidation of the biogenic gas
      dimethylsulfide emitted from the sea surface; (b) production fluxes of
      secondary organic aerosols from biogenic organic volatiles;
      (c) emission fluxes of biogenic primary organic aerosols ejected by
      wind action on sea surface; and (d) emission fluxes of sea salt also
      lifted by the wind upon bubble bursting. Series of global weekly
      estimates of these fluxes were correlated to series of cloud droplet
      effective radius data derived from satellite (MODIS). Similar analyses
      were conducted in more detail at 6 locations spread among polluted and
      clean regions of the oceanic atmosphere. The outcome of the
      statistical analysis was that negative correlation was common at mid
      and high latitude for sulfur and organic secondary aerosols,
      indicating both might be important in seeding cloud droplet
      activation. Conversely, primary aerosols (organic and sea salt) showed
      more variable, non-significant or positive correlations, indicating
      that, despite contributing to large shares of the marine aerosol mass,
      they are not major drivers of the variability of cloud
      microphysics. Uncertainties and synergisms are discussed, and
      recommendations of research needs are given.</description><dc:date>2012-02-02T00:00:00+01:00</dc:date></item><item rdf:about="http://www.atmos-chem-phys-discuss.net/12/3619/2012/"><title>Signals of El Niño Modoki in the tropical tropopause layer and stratosphere</title><link>http://www.atmos-chem-phys-discuss.net/12/3619/2012/</link><description>&lt;b&gt;Signals of El Niño Modoki in the tropical tropopause layer and stratosphere&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 12, 3619-3653, 2012&lt;br /&gt;&lt;br /&gt;Author(s): F. Xie, J. Li, W. Tian, and J. Feng&lt;br /&gt;&lt;br /&gt;The effects of El Niño Modoki events on the tropical tropopause layer
(TTL) and on the stratosphere were investigated using European Center for
Medium Range Weather Forecasting (ECMWF) reanalysis data, satellite
observations from the Aura satellite Microwave Limb Sounder (MLS), oceanic
El Niño indices, and general climate model outputs. El Niño Modoki
events tend to depress convective activities in the western and eastern
Pacific but enhance convective activities in the central and northern
Pacific. Consequently, during Modoki events, negative water vapor anomalies
occur in the western and eastern Pacific upper troposphere, whereas there
are positive anomalies in the central and northern Pacific upper
troposphere. The spatial patterns of the outgoing longwave radiation (OLR)
and upper tropospheric water vapor anomalies exhibit a tripolar form. The
empirical orthogonal function (EOF) analysis of the OLR and upper
tropospheric water vapor anomalies reveals that canonical El Niño events
are associated with the leading mode of the EOF, while El Niño Modoki
events correspond to the second mode. El Niño Modoki activities tend to
moisten the lower and middle stratosphere, but dry the upper stratosphere.
It was also found that the canonical El Niño signal can overlay linearly
on the QBO signal in the stratosphere, whereas the interaction between the
El Niño Modoki and QBO signals is non-linear. Because of these
non-linear interactions, El Niño Modoki events have a reverse effect on
high latitudes stratosphere, as compared with the effects of typical Modoki
events, i.e. the northern polar vortex is stronger and colder but the
southern polar vortex is weaker and warmer during El Niño Modoki events.
However, simulations suggest that canonical El Niño and El Niño
Modoki activities actually have the same influence on high latitudes
stratosphere, in the absence of interactions between QBO and ENSO signals.
The present results also reveal that canonical El Niño events have a
greater impact on the high-latitude Northern Hemisphere stratosphere than on
the high-latitude Southern Hemisphere stratosphere. However, El Niño
Modoki events can more profoundly influence the high-latitude Southern
Hemisphere stratosphere than the high-latitude Northern Hemisphere
stratosphere.</description><dc:date>2012-02-02T00:00:00+01:00</dc:date></item></rdf:RDF>
