<?xml version="1.0" encoding="utf-8"?><rss version="2.0"><channel><title>ACPD - Latest Articles</title><link>http://www.atmos-chem-phys-discuss.net/</link><description>Atmospheric Chemistry and Physics Discussions Latest Articles</description><language>en</language><item><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><pubDate>Tue, 21 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Tue, 21 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Fri, 17 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Fri, 17 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Fri, 17 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Fri, 17 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Wed, 15 May 2013 00:00:00 +0200</pubDate></item><item><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><pubDate>Wed, 15 May 2013 00:00:00 +0200</pubDate></item><item><title>Chemical evolution of organic aerosol in Los Angeles during the CalNex 2010 study</title><link>http://www.atmos-chem-phys-discuss.net/13/12867/2013/</link><description>&lt;b&gt;Chemical evolution of organic aerosol in Los Angeles during the CalNex 2010 study&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12867-12911, 2013&lt;br /&gt;&lt;br /&gt;Author(s): R. Holzinger, A. H. Goldstein, P. L. Hayes, J. L. Jimenez, and J. Timkovsky&lt;br /&gt;&lt;br /&gt;During the CalNex study (15 May to 16 June 2010) a large suite of
  instruments was operated at the Los Angeles area ground supersite to
  characterize the sources and atmospheric processing of atmospheric
  pollution. The thermal-desorption proton-transfer-reaction
  mass-spectrometer (TD-PTR-MS) was deployed to an urban area for the
  first time and detected 691 organic ions in aerosol samples, the
  mean total concentration of which was estimated as
  3.3 &amp;mu;g m&lt;sup&gt;&amp;minus;3&lt;/sup&gt;. Based on comparison to total organic
  aerosol (OA) measurements, we estimate that approximately 50%
  of the OA mass at this site was directly measured by the TD-PTR-MS.
  Based on correlations with aerosol mass spectrometer (AMS) OA
  components, the ions were grouped to represent hydrocarbon-like OA
  (HOA), local OA (LOA), semi-volatile oxygenated OA (SV-OOA), and low
  volatility oxygenated OA (LV-OOA). Mass spectra and thermograms of
  the ion groups are mostly consistent with the assumed sources and/or
  photochemical origin of the OA components. The mass spectra of ions
  representing the primary components HOA and LOA included the highest
  &lt;i&gt;m/z&lt;/i&gt;, consistent with their higher resistance to thermal
  decomposition, and they were volatilized at lower
  temperatures. Photochemical ageing weakens C-C bond strengths (also
  resulting in chemical fragmentation), and produces species of lower
  volatility (through the addition of functional groups). Accordingly
  the mass spectra of ions representing the oxidized OA components
  (SV-OOA, and LV-OOA) lack the highest masses and they are
  volatilized at higher temperatures. Chemical parameters like mean
  carbon number (&lt;span style=&quot;border-top: 1px solid #000; color: #000;&quot;&gt;&lt;i&gt;n&lt;/i&gt;&lt;sub&gt;C&lt;/span&gt;), mean carbon oxidation state
  (&lt;span style=&quot;border-top: 1px solid #000; color: #000;&quot;&gt;OS&lt;sub&gt;C&lt;/sub&gt;&lt;/span&gt;), and the atomic ratios O/C and H/C of the ion
  groups are consistent with the expected sources and photochemical
  processing of the aerosol components. Our data suggest that chemical
  fragmentation gains importance over functionalization as
  photochemical age of OA increases. Surprisingly, the photochemical
  age of OA decreases during the daytime hours, demonstrating the
  importance of rapid production of new (photochemically young) SV-OOA
  during daytime. The PTR detects higher organic N concentrations than
  the AMS, the reasons for which are not well understood and cannot be
  explained by known artifacts related to PTR or the AMS. The median
  atomic N/C ratio (6.4%) of the ion group representing LV-OOA is
  a factor 2 higher than N/C of any other ion group. This suggests
  a multiphase chemical source involving ammonium ions is contributing
  to LV-OOA.</description><pubDate>Wed, 15 May 2013 00:00:00 +0200</pubDate></item><item><title>Comparison of ensemble Kalman filter and variational approaches for  CO&lt;sub&gt;2&lt;/sub&gt; data assimilation</title><link>http://www.atmos-chem-phys-discuss.net/13/12825/2013/</link><description>&lt;b&gt;Comparison of ensemble Kalman filter and variational approaches for  CO&lt;sub&gt;2&lt;/sub&gt; data assimilation&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12825-12865, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Chatterjee and A. M. Michalak&lt;br /&gt;&lt;br /&gt;Data assimilation (DA) approaches, such as the variational and the
  ensemble Kalman filter, provide a computationally efficient
  framework for solving the CO&lt;sub&gt;2&lt;/sub&gt; source-sink estimation
  problem. Unlike DA applications for weather prediction and
  constituent assimilation, however, the advantages and disadvantages
  of alternative DA approaches for CO&lt;sub&gt;2&lt;/sub&gt; flux estimation have
  not been extensively explored. In this study, we compare and assess
  estimates from two advanced DA methods (an ensemble square root
  filter and a variational technique) using a simple 1-dimensional
  advection-diffusion inverse problem that has been designed to
  capture the nuances of a real CO&lt;sub&gt;2&lt;/sub&gt; flux estimation
  problem. Experiments are specifically designed to identify the
  impact of the observational density, heterogeneity, and uncertainty,
  as well as operational constraints (i.e., ensemble size, number of
  descent iterations) in order to isolate the degradation in the DA
  estimates relative to the estimates from a batch inverse modeling
  scheme. No dynamical model is explicitly specified for the DA
  methods to keep the problem setup analogous to a real CO&lt;sub&gt;2&lt;/sub&gt;
  flux estimation problem.  Results demonstrate that the performance
  of the DA approaches depends on a complex interplay between the
  measurement network and the operational constraints imposed to make
  the DA algorithms practically feasible. The overall
  advantages/disadvantages of the two examined DA approaches are
  complementary and highlight that, specifically for CO&lt;sub&gt;2&lt;/sub&gt;
  applications, selection of one method over the other should be
  dictated by the carbon science questions being asked, and the
  inversion conditions under which the approaches are being applied.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Direct estimation of the rate constant of the reaction  ClO  +  HO&lt;sub&gt;2&lt;/sub&gt;  → HOCl  +  O&lt;sub&gt;2&lt;/sub&gt; from SMILES atmospheric observations</title><link>http://www.atmos-chem-phys-discuss.net/13/12797/2013/</link><description>&lt;b&gt;Direct estimation of the rate constant of the reaction  ClO  +  HO&lt;sub&gt;2&lt;/sub&gt;  → HOCl  +  O&lt;sub&gt;2&lt;/sub&gt; from SMILES atmospheric observations&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12797-12823, 2013&lt;br /&gt;&lt;br /&gt;Author(s): K. Kuribayashi, H. Sagawa, R. Lehmann, T. O. Sato, and Y. Kasai&lt;br /&gt;&lt;br /&gt;Diurnal variations of  ClO, HO&lt;sub&gt;2&lt;/sub&gt;, and HOCl  were
simultaneously observed by the Superconducting Submillimeter-Wave
Limb-Emission Sounder (SMILES) between 12 October 2009 and 21 April 2010.
These were the first global observations of the diurnal variation of
HOCl in the upper atmosphere. A major reaction to produce HOCl
is ClO + HO&lt;sub&gt;2&lt;/sub&gt;   →  HOCl + O&lt;sub&gt;2&lt;/sub&gt; (R1) in extra
polar region. A model study suggested that in the mesosphere during night
this is the only reaction influencing the amount of HOCl and
ClO. The evaluation of the pure reaction period, where only reaction
(R1) occurred in Cl&lt;sub&gt;y&lt;/sub&gt; chemical system, was performed by the
consistency between two reaction rates, HOCl production and ClO
loss, from SMILES observation data. It turned out that the SMILES data at
the pressure level of 0.28 hPa (about 58 km) during night (between local
time 18:30 and 04:00) in the autumn mid-latitude region (20–40&amp;deg; 
February–April 2010) were suitable for the estimation of &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;. The rate
constant was obtained to be &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;(245 K) =  7.73 &amp;pm; 0.26 (1&amp;sigma;)
[&amp;times; 10&lt;sup&gt;–12&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt;/molecule s] from SMILES atmospheric
observations. This result was consistent with that from both the laboratory
experiment and the ab initio calculations for similar low-pressure
conditions. The 1&amp;sigma; precision of &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt; obtained was 2–10 times
better than those of previous laboratory measurements.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Method development estimating ambient mercury concentration from monitored mercury wet deposition</title><link>http://www.atmos-chem-phys-discuss.net/13/12771/2013/</link><description>&lt;b&gt;Method development estimating ambient mercury concentration from monitored mercury wet deposition&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12771-12796, 2013&lt;br /&gt;&lt;br /&gt;Author(s): S. M. Chen, X. Qiu, L. Zhang, F. Yang, and P. Blanchard&lt;br /&gt;&lt;br /&gt;Speciated atmospheric mercury
data have recently been monitored at multiple locations in North
America; but the spatial coverage is far less than
the long-established mercury wet deposition
network. The present study describes a first attempt
linking ambient concentration with wet deposition using Beta distribution
fitting of a ratio estimate. The
mean, median,
mode, standard deviation, and
skewness of the fitted Beta distribution parameters were generated using
data collected in 2009 at 11 monitoring stations.
Comparing the normalized histogram and the fitted density
function, the empirical and fitted Beta distribution of
the ratio shows a close fit. The estimated ambient
mercury concentration was further partitioned into reactive gaseous mercury
and particulate bound mercury using linear regression model developed by
Amos et al. (2012). The method
presented here can be used to roughly estimate mercury ambient concentration
at locations and/or times where such measurement is not available but where
wet deposition is monitored.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Particle partitioning potential of organic compounds is highest in the Eastern US and driven by anthropogenic water</title><link>http://www.atmos-chem-phys-discuss.net/13/12743/2013/</link><description>&lt;b&gt;Particle partitioning potential of organic compounds is highest in the Eastern US and driven by anthropogenic water&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12743-12770, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. G. Carlton and B. J. Turpin&lt;br /&gt;&lt;br /&gt;Gas phase water-soluble organic matter (WSOM&lt;sub&gt;g&lt;/sub&gt;) is
  ubiquitous in the troposphere. In the summertime, the potential for
  these gases to partition to particle phase liquid water
  (H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt;) where they can form secondary organic aerosol
  (SOA&lt;sub&gt;AQ&lt;/sub&gt;) is high in the Eastern US and low elsewhere,
  with the exception of an area near Los Angeles, CA. This spatial
  pattern is driven by mass concentrations of H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt;, not
  WSOM&lt;sub&gt;g&lt;/sub&gt;. H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt; mass concentrations are
  predicted to be high in the Eastern US, largely due to sulfate. The
  ability of sulfate to increase H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt; is
  well-established and routinely included in atmospheric models,
  however WSOM&lt;sub&gt;g&lt;/sub&gt; partitioning to this water and subsequent
  SOA formation is not. The high mass concentrations of
  H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt; in the southeast (SE) US but not the Amazon, may
  help explain why biogenic SOA mass concentrations are high in the SE
  US, but low in the Amazon. Furthermore, during the summertime in the
  Eastern US, the potential for organic gases to partition into liquid
  water is greater than their potential to partition into organic
  matter (OM) because concentrations of WSOM&lt;sub&gt;g&lt;/sub&gt; and
  H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt; are higher than semi-volatile gases
  and OM.  Thus, unless condensed phase yields are substantially
  different (&gt; ~ order of magnitude), we expect that SOA formed
  through aqueous phase pathways (SOA&lt;sub&gt;AQ&lt;/sub&gt;) will dominate
  in the Eastern US. These findings also suggest that
  H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;ptcl&lt;/sub&gt; is largely anthropogenic and provide a previously
  unrecognized mechanism by which anthropogenic pollutants impact the
  amount of SOA mass formed from biogenic organic emissions. The
  previously reported estimate of the controllable fraction of
  biogenic SOA in the Eastern US (50%) is likely too low.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>The impact of horizontal heterogeneities, cloud fraction, and cloud dynamics on warm cloud effective radii and liquid water path from CERES-like Aqua MODIS retrievals</title><link>http://www.atmos-chem-phys-discuss.net/13/12725/2013/</link><description>&lt;b&gt;The impact of horizontal heterogeneities, cloud fraction, and cloud dynamics on warm cloud effective radii and liquid water path from CERES-like Aqua MODIS retrievals&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12725-12742, 2013&lt;br /&gt;&lt;br /&gt;Author(s): D. Painemal, P. Minnis, and S. Sun-Mack&lt;br /&gt;&lt;br /&gt;The impact of horizontal heterogeneities, liquid water path (LWP
  from AMSR-E), and cloud fraction (CF) on MODIS cloud effective
  radius (&lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt;), retrieved from the 2.1 &amp;mu;m
  (&lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt;) and 3.8 &amp;mu;m (&lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt;)
  channels, is investigated for warm clouds over the southeast
  Pacific. Values of &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e&lt;/sub&gt; retrieved using the CERES
  Edition 4 algorithms are averaged at the CERES footprint resolution
  (~ 20 km), while heterogeneities
  (&lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;sigma;&lt;/sub&gt;) are calculated as the ratio between the
  standard deviation and mean 0.64 &amp;mu;m reflectance. The
  value of &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt; strongly depends on CF, with magnitudes
  up to 5 &amp;mu;m larger than those for overcast scenes,
  whereas &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt; remains insensitive to CF. For cloudy
  scenes, both &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt; and &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt; increase
  with &lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;sigma;&lt;/sub&gt; for any given AMSR-E LWP, but
  &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt; changes more than for
  &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt;. Additionally,
  &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt; &amp;ndash; &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt; differences are positive
  (&lt; 1 &amp;mu;m) for homogeneous scenes
  (&lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;sigma;&lt;/sub&gt; &lt; 0.2) and LWP &gt; 50 g m&lt;sup&gt;&amp;minus;2&lt;/sup&gt;, and
  negative (up to −4 &amp;mu;m) for larger
  &lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;sigma;&lt;/sub&gt;. Thus, &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e3.8&lt;/sub&gt; &amp;ndash; &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;e2.1&lt;/sub&gt;
  differences are more likely to reflect biases associated with cloud
  heterogeneities rather than information about the cloud vertical
  structure. The consequences for MODIS LWP are also discussed.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Online coupled regional meteorology-chemistry models in Europe: current status and prospects</title><link>http://www.atmos-chem-phys-discuss.net/13/12541/2013/</link><description>&lt;b&gt;Online coupled regional meteorology-chemistry models in Europe: current status and prospects&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12541-12724, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Baklanov, K. H. Schluenzen, P. Suppan, J. Baldasano, D. Brunner, S. Aksoyoglu, G. Carmichael, J. Douros, J. Flemming, R. Forkel, S. Galmarini, M. Gauss, G. Grell, M. Hirtl, S. Joffre, O. Jorba, E. Kaas, M. Kaasik, G. Kallos, X. Kong, U. Korsholm, A. Kurganskiy, J. Kushta, U. Lohmann, A. Mahura, A. Manders-Groot, A. Maurizi, N. Moussiopoulos, S. T. Rao, N. Savage, C. Seigneur, R. Sokhi, E. Solazzo, S. Solomos, B. Sørensen, G. Tsegas, E. Vignati, B. Vogel, and Y. Zhang&lt;br /&gt;&lt;br /&gt;The simulation of the coupled evolution of atmospheric dynamics,
  pollutant transport, chemical reactions and atmospheric composition
  is one of the most challenging tasks in environmental modelling,
  climate change studies, and weather forecasting for the next decades
  as they all involve strongly integrated processes. Weather strongly
  influences air quality (AQ) and atmospheric transport of hazardous
  materials, while atmospheric composition can influence both weather
  and climate by directly modifying the atmospheric radiation budget
  or indirectly affecting cloud formation. Until recently, however,
  due to the scientific complexities and lack of computational power,
  atmospheric chemistry and weather forecasting have developed as
  separate disciplines, leading to the development of separate
  modelling systems that are only loosely coupled.
&lt;br&gt;&lt;/br&gt;
  The continuous increase in computer power has now reached a stage
  that enables us to perform online coupling of regional
  meteorological models with atmospheric chemical transport
  models. The focus on integrated systems is timely, since recent
  research has shown that meteorology and chemistry feedbacks are
  important in the context of many research areas and applications,
  including numerical weather prediction (NWP), AQ forecasting as well
  as climate and Earth system modelling. However, the relative
  importance of online integration and its priorities, requirements
  and levels of detail necessary for representing different processes
  and feedbacks can greatly vary for these related communities: (i)
  NWP, (ii) AQ forecasting and assessments, (iii) climate and earth
  system modelling. Additional applications are likely to benefit from
  online modelling, e.g.: simulation of volcanic ash or forest fire
  plumes, pollen warnings, dust storms, oil/gas fires, geo-engineering
  tests involving changes in the radiation balance.
&lt;br&gt;&lt;/br&gt;
  The COST Action ES1004 – European framework for online integrated
  air quality and meteorology modelling (EuMetChem) – aims at paving
  the way towards a new generation of online integrated atmospheric
  chemical transport and meteorology modelling with two-way
  interactions between different atmospheric processes including
  dynamics, chemistry, clouds, radiation, boundary layer and
  emissions. As its first task, we summarise the current status of
  European modelling practices and experience with online coupled
  modelling of meteorology with atmospheric chemistry including
  feedback mechanisms and attempt reviewing the various issues
  connected to the different modules of such online coupled models but
  also providing recommendations for coping with them for the benefit
  of the modelling community at large.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Evaluating global emission inventories of biogenic bromocarbons</title><link>http://www.atmos-chem-phys-discuss.net/13/12485/2013/</link><description>&lt;b&gt;Evaluating global emission inventories of biogenic bromocarbons&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12485-12539, 2013&lt;br /&gt;&lt;br /&gt;Author(s): R. Hossaini, H. Mantle, M. P. Chipperfield, S. A. Montzka, P. Hamer, F. Ziska, B. Quack, K. Krüger, S. Tegtmeier, E. Atlas, S. Sala, A. Engel, H. Bönisch, T. Keber, D. Oram, G. Mills, C. Ordóñez, A. Saiz-Lopez, N. Warwick, Q. Liang, W. Feng, F. Moore, B. R. Miller, V. Marécal, N. A. D. Richards, M. Dorf, and K. Pfeilsticker&lt;br /&gt;&lt;br /&gt;Emissions of halogenated very short-lived substances (VSLS) are
  poorly constrained. However, their inclusion in global models is
  required to simulate a realistic inorganic bromine (Br&lt;sub&gt;y&lt;/sub&gt;)
  loading in both the troposphere, where bromine chemistry perturbs
  global oxidizing capacity, and in the stratosphere, where it is
  a major sink for ozone (O&lt;sub&gt;3&lt;/sub&gt;).  We have performed simulations
  using a 3-D chemical transport model (CTM) including three
  &lt;i&gt;top-down&lt;/i&gt; and a single &lt;i&gt;bottom-up&lt;/i&gt; derived emission
  inventory of the major brominated VSLS bromoform (CHBr&lt;sub&gt;3&lt;/sub&gt;) and
  dibromomethane (CH&lt;sub&gt;2&lt;/sub&gt;Br&lt;sub&gt;2&lt;/sub&gt;). We perform the first concerted
  evaluation of these inventories, comparing both the magnitude and
  spatial distribution of emissions. For a quantitative evaluation of
  each inventory, model output is compared with independent long-term
  observations at National Oceanic and Atmospheric Administration
  (NOAA) ground-based stations and with aircraft observations made
  during the NSF HIAPER Pole-to-Pole Observations (HIPPO) project. For
  CHBr&lt;sub&gt;3&lt;/sub&gt;, the mean absolute deviation between model and surface
  observation ranges from 0.22 (38%) to 0.78 (115%) parts
  per trillion (ppt) in the tropics, depending on emission
  inventory. For CH&lt;sub&gt;2&lt;/sub&gt;Br&lt;sub&gt;2&lt;/sub&gt;, the range is 0.17 (24%) to 1.25
  (167%) ppt. We also use aircraft observations made during the
  2011 &quot;&lt;b&gt;S&lt;/b&gt;tratospheric Ozone: &lt;b&gt;H&lt;/b&gt;alogen &lt;b&gt;I&lt;/b&gt;mpacts in a &lt;b&gt;V&lt;/b&gt;arying
    &lt;b&gt;A&lt;/b&gt;tmosphere&quot; (SHIVA) campaign, in the tropical West
  Pacific. Here, the performance of the various inventories also
  varies significantly, but overall the CTM is able to reproduce
  observed CHBr&lt;sub&gt;3&lt;/sub&gt; well in the free troposphere using an
  inventory based on observed sea-to-air fluxes. Finally, we identify
  the range of uncertainty associated with these VSLS emission
  inventories on stratospheric bromine loading due to VSLS
  (Br&lt;sub&gt;y&lt;/sub&gt;&lt;sup&gt;VSLS&lt;/sup&gt;). Our simulations show Br&lt;sub&gt;y&lt;/sub&gt;&lt;sup&gt;VSLS&lt;/sup&gt; ranges
  from ~ 4.0 to 8.0  ppt depending on the inventory. We report
  an optimised estimate at the lower end of this range
  (~ 4 ppt) based on combining the CHBr&lt;sub&gt;3&lt;/sub&gt; and
  CH&lt;sub&gt;2&lt;/sub&gt;Br&lt;sub&gt;2&lt;/sub&gt; inventories which give best agreement with the
  compilation of observations in the tropics.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Eddy covariance fluxes and vertical concentration gradient measurements of NO and NO&lt;sub&gt;2&lt;/sub&gt; over a ponderosa pine ecosystem: observational evidence for within canopy removal of NO&lt;sub&gt;x&lt;/sub&gt;</title><link>http://www.atmos-chem-phys-discuss.net/13/12437/2013/</link><description>&lt;b&gt;Eddy covariance fluxes and vertical concentration gradient measurements of NO and NO&lt;sub&gt;2&lt;/sub&gt; over a ponderosa pine ecosystem: observational evidence for within canopy removal of NO&lt;sub&gt;x&lt;/sub&gt;&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12437-12484, 2013&lt;br /&gt;&lt;br /&gt;Author(s): K.-E. Min, S. E. Pusede, E. C. Browne, B. W. LaFranchi, P. J. Wooldridge, and R. C. Cohen&lt;br /&gt;&lt;br /&gt;Exchange of NO&lt;sub&gt;x&lt;/sub&gt; (NO+NO&lt;sub&gt;2&lt;/sub&gt;) between the atmosphere and
  biosphere is important for air quality, climate change, and
  ecosystem nutrient dynamics. There are few direct ecosystem scale
  measurements of the direction and rate of atmosphere-biosphere
  exchange of NO&lt;sub&gt;x&lt;/sub&gt;. As a result, a complete description of the
  processes affecting NO&lt;sub&gt;x&lt;/sub&gt; following emission from soils and/or
  plants as they transit from within the plant/forest canopy to the
  free atmosphere remains poorly constrained and debated. Here, we
  describe measurements of NO and NO&lt;sub&gt;2&lt;/sub&gt; fluxes and vertical
  concentration gradients made during the Biosphere Effects on
  AeRosols and Photochemistry EXperiment 2009. In general, during
  daytime we observe upward fluxes of NO and NO&lt;sub&gt;2&lt;/sub&gt; with
  counter-gradient fluxes of NO. We find that NO&lt;sub&gt;x&lt;/sub&gt; fluxes from
  the forest canopy are smaller than calculated using observed
  flux-gradient relationships for conserved tracers and also smaller
  than measured soil NO emissions. We interpret these differences as
  evidence for the existence of a &quot;canopy reduction factor&quot;. We
  suggest that at this site it is primarily due to chemistry
  converting NO&lt;sub&gt;x&lt;/sub&gt; to higher nitrogen oxides within the forest
  canopy.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Sulfur dioxide (SO&lt;sub&gt;2&lt;/sub&gt;) as observed by MIPAS/Envisat: temporal development and spatial distribution at 15–45 km altitude</title><link>http://www.atmos-chem-phys-discuss.net/13/12389/2013/</link><description>&lt;b&gt;Sulfur dioxide (SO&lt;sub&gt;2&lt;/sub&gt;) as observed by MIPAS/Envisat: temporal development and spatial distribution at 15–45 km altitude&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12389-12436, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Höpfner, N. Glatthor, U. Grabowski, S. Kellmann, M. Kiefer, A. Linden, J. Orphal, G. Stiller, T. von Clarmann, and B. Funke&lt;br /&gt;&lt;br /&gt;We present a climatology of monthly and 10&amp;deg; zonal mean
  profiles of sulfur dioxide (SO&lt;sub&gt;2&lt;/sub&gt;) volume mixing ratios (vmr)
  derived from MIPAS/Envisat measurements in the altitude range
  15–45 km from July 2002 until April 2012. The vertical
  resolution varies from 3.5–4 km in the lower stratosphere
  up to 6–10 km at the upper end of the profiles with
  estimated total errors of 5–20 pptv for single profiles of
  SO&lt;sub&gt;2&lt;/sub&gt;. Comparisons with few available observations of
  SO&lt;sub&gt;2&lt;/sub&gt; up to high altitudes from ATMOS, for a volcanically
  perturbed situations from ACE-FTS and, at the lowest altitudes, with
  stratospheric in-situ observations reveal general consistency of the
  datasets. The observations are the first empirical confirmation of
  features of the stratospheric SO&lt;sub&gt;2&lt;/sub&gt; distribution which have
  only been shown by models up to now: (1) the local maximum of
  SO&lt;sub&gt;2&lt;/sub&gt; at around 25–30 km altitude which is explained
  by the conversion of carbonyl sulfide (COS) as the precursor of the
  Junge layer, and (2) the downwelling of SO&lt;sub&gt;2&lt;/sub&gt; rich air to
  altitudes of 25–30 km at high latitudes during winter and
  its subsequent depletion on availability of sunlight. This has been
  proposed as the reason for the sudden appearance of enhanced
  concentrations of condensation nuclei during Arctic and Antarctic
  spring. Further, the strong increase of SO&lt;sub&gt;2&lt;/sub&gt; to values of
  80–100 pptv in the upper stratosphere through photolysis of
  H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; has been confirmed. Lower stratospheric variability
  of SO&lt;sub&gt;2&lt;/sub&gt; could mainly be explained by volcanic activity and no
  hint for a strong anthropogenic influence has been found. Regression
  analysis revealed a QBO (quasi-biennial oscillation) signal of the
  SO&lt;sub&gt;2&lt;/sub&gt; time series in the tropics at about 30–35 km,
  a SAO (semi-annual oscillation) signal at tropical and subtropical
  latitudes above 32 km and annual periodics predominantly at
  high latitudes. Further, the analysis indicates a correlation with
  the solar cycle in the tropics and southern subtropics above
  30 km. Significant negative linear trends are found in the
  tropical lower stratosphere, probably due to reduced tropical
  volcanic activity and at southern mid-latitudes above
  35 km. A positive trend is visible in the lower and middle
  stratosphere at polar to subtropical southern latitudes.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Trends in stratospheric ozone profiles using functional mixed models</title><link>http://www.atmos-chem-phys-discuss.net/13/12337/2013/</link><description>&lt;b&gt;Trends in stratospheric ozone profiles using functional mixed models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12337-12387, 2013&lt;br /&gt;&lt;br /&gt;Author(s): A. Y. Park, S. Guillas, and I. Petropavlovskikh&lt;br /&gt;&lt;br /&gt;This paper is devoted to the modeling of altitude-dependent patterns
  of ozone variations over time. Umkher ozone profiles (quarter of
  Umkehr layer) from 1978 to 2011 are investigated at two locations:
  Boulder (USA) and Arosa (Switzerland). The study consists of two
  statistical stages. First we approximate ozone profiles employing an
  appropriate basis. To capture primary modes of ozone variations
  without losing essential information, a functional principal
  component analysis is performed as it penalizes roughness of the
  function and smooths excessive variations in the shape of the ozone
  profiles. As a result, data driven basis functions are obtained.
  Secondly we estimate the effects of covariates – month, year
  (trend), quasi biennial oscillation, the Solar cycle, arctic
  oscillation and the El Niño/Southern Oscillation cycle – on the
  principal component scores of ozone profiles over time using
  generalized additive models. The effects are smooth functions of the
  covariates, and are represented by knot-based regression cubic
  splines. Finally we employ generalized additive mixed effects models
  incorporating a more complex error structure that reflects the
  observed seasonality in the data. The analysis provides more
  accurate estimates of influences and trends, together with enhanced
  uncertainty quantification. We are able to capture fine variations
  in the time evolution of the profiles such as the semi-annual
  oscillation. We conclude by showing the trends by altitude over
  Boulder. The strongly declining trends over 2003–2011 for altitudes
  of 32–64 hPa show that stratospheric ozone is not yet fully
  recovering.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item><item><title>Simulation of trace gases and aerosols over the Indian domain: evaluation of the WRF-Chem Model</title><link>http://www.atmos-chem-phys-discuss.net/13/12287/2013/</link><description>&lt;b&gt;Simulation of trace gases and aerosols over the Indian domain: evaluation of the WRF-Chem Model&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Chemistry and Physics Discussions, 13, 12287-12336, 2013&lt;br /&gt;&lt;br /&gt;Author(s): M. Michael, A. Yadav, S. N. Tripathi, V. P. Kanawade, A. Gaur, P. Sadavarte, and C. Venkataraman&lt;br /&gt;&lt;br /&gt;The &quot;online&quot; meteorological and chemical transport Weather
  Research and Forecasting/Chemistry (WRF-Chem) model has been
  implemented over the Indian subcontinent for three consecutive
  summers in 2008, 2009 and 2010 to study the aerosol properties over
  the domain. The initial and boundary conditions are obtained from
  NCAR reanalysis data. The emission rates of sulfur dioxide, black
  carbon, organic carbon and PM&lt;sub&gt;2.5&lt;/sub&gt;, which are developed over
  India at a grid resolution of 0.25&amp;deg; × 0.25&amp;deg;
  have been used in the present study. The remaining emissions are
  obtained from global inventories (RETRO and EDGAR). The model
  simulated the meteorological parameters, trace gases and particulate
  matter. Predicted mixing ratios of trace gases (Ozone, carbon
  monoxide and sulfur dioxide) are compared with ground based
  observations over Kanpur. Simulated aerosol optical depth are
  compared with those observed at nine Aerosol Robotic Network
  stations (AERONET). The simulations show that the aerosol optical
  depth of the less polluted regions is better simulated compared to
  that of the locations where the aerosol loading is very high. The
  vertical profiles of extinction coefficient observed at Kanpur
  Micropulse Lidar Network (MPLNET) station is in agreement with the
  simulated values for altitudes greater than 1.5 km and
  qualitatively simulate the elevated layers of aerosols. The
  simulated mass concentration of black carbon shows very good
  correlation with observations, due to the better local emission
  inventory used. The vertical profiles of black carbon at various
  locations have also been compared with observations from aircraft
  campaign held during pre-monsoon period of 2008 and 2009 resulting
  in good agreement.  This study shows that WRF-Chem model captures
  many important features of the observations and therefore can be
  used for understanding and predicting regional atmospheric
  composition over Indian subcontinent.</description><pubDate>Tue, 14 May 2013 00:00:00 +0200</pubDate></item></channel></rss>