<?xml version="1.0" encoding="utf-8"?><!DOCTYPE rss PUBLIC "-//Netscape Communications//DTD RSS 0.91//EN" "http://my.netscape.com/publish/formats/rss-0.91.dtd"><rss version="0.91"><channel><title>AMTD - Latest Articles</title><link>http://www.atmos-meas-tech-discuss.net/</link> <description>Atmospheric Measurement Techniques Discussions Latest Articles</description><language>en</language><item><title>Temperature profiles with bi-static Doppler-RASS and their accuracy</title><link>http://www.atmos-meas-tech-discuss.net/5/1075/2012/</link><description>&lt;b&gt;Temperature profiles with bi-static Doppler-RASS and their accuracy&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 1075-1100, 2012&lt;br /&gt;&lt;br /&gt;Author(s): B. Hennemuth, G. Peters, and H.-J. Kirtzel&lt;br /&gt;&lt;br /&gt;The technique of atmospheric temperature profiling by Doppler-RASS
is discussed. The set up with bi-static (separated transmit and receiving)
antennas implies a range dependent scattering angle. The retrieval
scheme developed by Kon for such antenna geometry is reviewed and
its limits of validity are discussed. Empirical tuning of the efficient
antenna aperture is proposed to fit the retrieved temperature profiles
to reality. Examples of application of the measuring technique for
atmospheric boundary layer characterization are presented.</description><pubDate>Fri, 03 Feb 2012 00:00:00 +0100</pubDate></item><item><title>SCIAMACHY lunar occultation water vapor measurements: retrieval and validation results</title><link>http://www.atmos-meas-tech-discuss.net/5/1029/2012/</link><description>&lt;b&gt;SCIAMACHY lunar occultation water vapor measurements: retrieval and validation results&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 1029-1073, 2012&lt;br /&gt;&lt;br /&gt;Author(s): F. Azam, K. Bramstedt, A. Rozanov, K. Weigel, H. Bovensmann, G. P. Stiller, and J. P. Burrows&lt;br /&gt;&lt;br /&gt;SCIAMACHY lunar occultation measurements have been used to derive vertical
profiles of stratospheric water vapor for the Southern Hemisphere in the near
infrared (NIR) spectral range of 1350–1420 nm. The focus of this study is
to present the retrieval methodology including the sensitivity studies and
optimizations for the implementation of the radiative transfer model on
SCIAMACHY lunar occultation measurements. The study also includes the
validation of the data product with the collocated measurements from two
satellite occultation instruments and two instruments measuring in limb
geometry. The SCIAMACHY lunar occultation water vapor measurements
comparisons with the ACE-FTS instrument have shown an agreement of 5% on
the average that is well within the reported biases of ACE in the
stratosphere. The comparisons with HALOE have also shown good results where
the agreement between the instruments is within 5%. The validations of the
lunar occultation water vapor measurements with MLS instrument are
exceptionally good varying between 1.5 to around 4%. The validations with
MIPAS are in the range of 10%. A validated dataset of water vapor vertical
distributions from SCIAMACHY lunar occultation measurements is expected to
facilitate the understanding of physical and chemical processes in the
southern mid-latitudes and the dynamical processes related to polar vortex.</description><pubDate>Fri, 03 Feb 2012 00:00:00 +0100</pubDate></item><item><title>A new algorithm for brown and black carbon identification and organic carbon detection in fine atmospheric aerosols by a multi-wavelength Aethalometer</title><link>http://www.atmos-meas-tech-discuss.net/5/1003/2012/</link><description>&lt;b&gt;A new algorithm for brown and black carbon identification and organic carbon detection in fine atmospheric aerosols by a multi-wavelength Aethalometer&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 1003-1027, 2012&lt;br /&gt;&lt;br /&gt;Author(s): F. Esposito, M. R. Calvello, E. Gueguen, and G. Pavese&lt;br /&gt;&lt;br /&gt;A novel approach for the analysis of aerosol absorption coefficient
measurements is presented. A 7-wavelenghts aethalometer has been employed to
identify brown carbon (BrC) and black carbon (BC) and to detect organic
carbon (OC) in fine atmospheric aerosols (PM&lt;sub&gt;2.5&lt;/sub&gt;). The Magee Aethalometer
estimates the BC content in atmospheric particulate by measuring the light
attenuation in the aerosols accumulated on a quartz filter, at the standard
wavelength &amp;lambda; = 0.88 μm. The known Magee algorithm is based on the hypothesis of a mass
absorption coefficient inversely proportional to the wavelength. The new
algorithm has been developed and applied to the whole spectral range; it
verifies the spectral absorption behavior and, thus, it distinguishes
between black and brown carbon. Moreover, it allows also to correct the
absorption estimation at the UV wavelength commonly used to qualitatively
detect the presence of mixed hydrocarbons. The algorithm has been applied to
data collected in Agri Valley, located in Southern Italy, where torched
crude oil undergoes a pre-treatment process.
&lt;br&gt;&lt;br&gt;
The Magee Aethalometer has been set to measure Aerosol absorption
coefficients &amp;tau;&lt;sub&gt;aer&lt;/sub&gt; (&amp;lambda;, &lt;i&gt;t&lt;/i&gt;) every 5 min. Wavelength dependence of &amp;tau;&lt;sub&gt;aer&lt;/sub&gt; (&amp;lambda;, &lt;i&gt;t&lt;/i&gt;) has
been analyzed by a best-fit technique and, excluding UV-wavelengths, both
the absorption Angstrom coefficient &amp;alpha; and the BC (or BrC) concentration have
been determined. Finally, daily histograms of &amp;alpha; provide information on
optical properties of carbonaceous aerosol, while the extrapolation at
UV-wavelengths gives information on the presence of semivolatile organic
carbon (OC) particles.</description><pubDate>Wed, 01 Feb 2012 00:00:00 +0100</pubDate></item><item><title>Improved retrieval of SO&lt;sub&gt;2&lt;/sub&gt; from Ozone Monitoring Instrument: residual analysis and data noise correction</title><link>http://www.atmos-meas-tech-discuss.net/5/979/2012/</link><description>&lt;b&gt;Improved retrieval of SO&lt;sub&gt;2&lt;/sub&gt; from Ozone Monitoring Instrument: residual analysis and data noise correction&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 979-1001, 2012&lt;br /&gt;&lt;br /&gt;Author(s): H. Yan, L. Chen, J. Tao, L. Su, and D. Han&lt;br /&gt;&lt;br /&gt;In this study, based on Ozone Monitoring Instrument (OMI) observation
      data and considering the shortage of current Band Residual Difference
      algorithm (BRD) algorithm in data noise correction since late 2008, we
      make a detailed analysis of OMI SO&lt;sub&gt;2&lt;/sub&gt; main noise sources and
      determine the best residual adjustment area by analyzing the different
      residual correction effects. After such modification, the OMI SO&lt;sub&gt;2&lt;/sub&gt;
      PBL results noise which use BRD retrieval algorithm is largely
      reduced, the precision of the SO&lt;sub&gt;2&lt;/sub&gt; results is improved, and the
      optimization of the BRD algorithm for data noise is realized. We
      select China as our study area and compare the results between the
      optimized results and the OMI SO&lt;sub&gt;2&lt;/sub&gt; PBL products. Results show that
      they are consistent with each other in January 2008; however, our
      modified algorithm results have higher precision and more reliable
      SO&lt;sub&gt;2&lt;/sub&gt; spatial distribution in January 2009. Finally, other current
      retrieval error sources are discussed, and further research is needed
      on these areas.</description><pubDate>Fri, 27 Jan 2012 00:00:00 +0100</pubDate></item><item><title>A gas chromatographic instrument for measurement of hydrogen cyanide in the lower atmosphere</title><link>http://www.atmos-meas-tech-discuss.net/5/947/2012/</link><description>&lt;b&gt;A gas chromatographic instrument for measurement of hydrogen cyanide in the lower atmosphere&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 947-978, 2012&lt;br /&gt;&lt;br /&gt;Author(s): J. L. Ambrose, Y. Zhou, K. Haase, H. R. Mayne, R. Talbot, and B. C. Sive&lt;br /&gt;&lt;br /&gt;A gas-chromatographic (GC) instrument was developed for measuring hydrogen
cyanide (HCN) in the lower atmosphere. The main features of the instrument
are (1) a cryogen-free cooler for sample dehumidification and enrichment,
(2) a porous polymer PLOT column for analyte separation, (3) a flame
thermionic detector (FTD) for sensitive and selective detection and (4) a
dynamic dilution system for calibration. We deployed the instrument for a
~4 month period from January&amp;ndash;June 2010 at the AIRMAP atmospheric
monitoring station Thompson Farm 2 (THF2) in rural Durham, NH. A subset of
measurements made during 3&amp;ndash;31 March is presented here with a detailed
description of the instrument features and performance characteristics. The
temporal resolution of the measurements was ~20 min, with a 75 s
sample capture time. The 1&amp;sigma; measurement precision was &lt;10% and
the instrument response linearity was excellent on a calibration scale of
0.10&amp;ndash;0.75 ppbv (&amp;plusmn;5%). The estimated method detection limit (MDL)
and accuracy were 0.021 ppbv and 15%, respectively. From 3&amp;ndash;31 March
2010, ambient HCN mixing ratios ranged from 0.15&amp;ndash;1.0 ppbv (&amp;plusmn;15%), with a mean value of 0.36 &amp;plusmn; 0.16 ppbv (1&amp;sigma;). The
approximate mean background HCN mixing ratio of 0.20 &amp;plusmn; 0.04 ppbv appeared
to agree well with tropospheric column measurements reported previously. The
GC-FTD HCN measurements were strongly correlated with acetonitrile
(CH&lt;sub&gt;3&lt;/sub&gt;CN) measured concurrently with a proton transfer-reaction mass
spectrometer (PTR-MS), as anticipated given our understanding that the
nitriles share a common primary biomass burning source to the global
atmosphere. The nitriles were overall only weakly correlated with CO, which
is reasonable considering the greater diversity of sources for CO. However,
strong correlations with CO were observed on several nights under stable
atmospheric conditions and suggest regional combustion-based sources for the
nitriles. These results demonstrate that the GC-FTD instrument is capable of
making long term, in-situ measurements of HCN in the lower atmosphere. To
date, similar measurements have not been performed, yet they are critically
needed to (1) better evaluate the regional scale distribution of HCN in the
atmosphere and (2) discern the influence of biomass burning on surface air
composition in remote regions.</description><pubDate>Fri, 27 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Multi-sensor Aerosol Products Sampling System (MAPSS)</title><link>http://www.atmos-meas-tech-discuss.net/5/909/2012/</link><description>&lt;b&gt;Multi-sensor Aerosol Products Sampling System (MAPSS)&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 909-945, 2012&lt;br /&gt;&lt;br /&gt;Author(s): M. Petrenko, C. Ichoku, and G. Leptoukh&lt;br /&gt;&lt;br /&gt;Global and local properties of atmospheric aerosols have been extensively
observed and measured using both spaceborne and ground-based instruments,
especially during the last decade. Unique properties retrieved by the
different instruments contribute to an unprecedented availability of the
most complete set of complimentary aerosol measurements ever acquired.
However, some of these measurements remain underutilized, largely due to the
complexities involved in analyzing them synergistically. To characterize the
inconsistencies and bridge the gap that exists between the sensors, we have
established a Multi-sensor Aerosol Products Sampling System (MAPSS), which
consistently samples and generates the spatial statistics (mean, standard
deviation, direction and rate of spatial variation, and spatial correlation
coefficient) of aerosol products from multiple spaceborne sensors, including
MODIS (on Terra and Aqua), MISR, OMI, POLDER, CALIOP, and SeaWiFS. Samples
of satellite aerosol products are extracted over Aerosol Robotic Network
(AERONET) locations as well as over other locations of interest such as
those with available ground-based aerosol observations. In this way, MAPSS
enables a direct cross-characterization and data integration between Level-2
aerosol observations from multiple sensors. In addition, the available
well-characterized co-located ground-based data provides the basis for the
integrated validation of these products. This paper explains the sampling
methodology and concepts used in MAPSS, and demonstrates specific examples
of using MAPSS for an integrated analysis of multiple aerosol products.</description><pubDate>Thu, 26 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Multiple scattering in a dense aerosol atmosphere</title><link>http://www.atmos-meas-tech-discuss.net/5/881/2012/</link><description>&lt;b&gt;Multiple scattering in a dense aerosol atmosphere&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 881-907, 2012&lt;br /&gt;&lt;br /&gt;Author(s): S. Mukai, T. Yokomae, I. Sano, M. Nakata, and A. Kokhanovsky&lt;br /&gt;&lt;br /&gt;This study was designed to develop an efficient algorithm to retrieve
aerosol characteristics in aerosol events, which are associated with dense
concentrations of aerosols in the atmosphere, such as a dust storm or a
biomass burning plume. The idea of successive scattering of light is
reviewed based on the theory of radiative transfer. Then derivation of the
method of successive order of scattering (MSOS) is interpreted in detail,
and it is shown that MSOS is available for a simulation scheme in the dense
radiation field being used to retrieve aerosol properties in the event with
the high optical thickness. Finally our algorithms are practically applied
for the biomass burning aerosol event over the Amazon using Aqua/MODIS data.</description><pubDate>Tue, 24 Jan 2012 00:00:00 +0100</pubDate></item><item><title>On the accuracy of integrated water vapor observations and the potential for mitigating electromagnetic path delay error in InSAR</title><link>http://www.atmos-meas-tech-discuss.net/5/839/2012/</link><description>&lt;b&gt;On the accuracy of integrated water vapor observations and the potential for mitigating electromagnetic path delay error in InSAR&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 839-880, 2012&lt;br /&gt;&lt;br /&gt;Author(s): D. Cimini, N. Pierdicca, E. Pichelli, R. Ferretti, V. Mattioli, S. Bonafoni, M. Montopoli, and D. Perissin&lt;br /&gt;&lt;br /&gt;A field campaign was carried out in the framework of the Mitigation of
Electromagnetic Transmission errors induced by Atmospheric Water Vapour
Effects (METAWAVE) project sponsored by the European Space Agency (ESA) to
investigate the accuracy of currently available sources of atmospheric
columnar integrated water vapor measurements. The METAWAVE campaign took
place in Rome, Italy, for the 2-week period from 19 September to 4 October
2008. The collected dataset includes observations from ground-based
microwave radiometers and Global Positioning System (GPS) receivers, from
meteorological numerical model analysis and predictions, from balloon-borne
in-situ radiosoundings, as well as from spaceborne infrared radiometers. These
different sources of integrated water vapor (IWV) observations have been
analyzed and compared to quantify the accuracy and investigate the potential
for mitigating IWV-related electromagnetic path delay errors in
Interferometric Synthetic Aperture Radar (InSAR) imaging. The results, which
include a triple collocation analysis accounting for errors inherently
present in every IWV measurements, are valid not only to InSAR but also to
any other application involving water vapor sensing. The present analysis
concludes that the sensitivity of InSAR to water vapor turbulent component
is significantly higher than that of the other instruments analyzed here.
Nonetheless, information on the IWV vertical stratification from satellite
observations, numerical models, and GPS receivers may provide valuable aid
to suppress the long spatial wavelength (&gt;20 km) component of the
atmospheric delay, and thus significantly improve the performances of InSAR
phase unwrapping techniques.</description><pubDate>Tue, 24 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Site selective real-time measurements of atmospheric N&lt;sub&gt;2&lt;/sub&gt;O  isotopomers by laser spectroscopy</title><link>http://www.atmos-meas-tech-discuss.net/5/813/2012/</link><description>&lt;b&gt;Site selective real-time measurements of atmospheric N&lt;sub&gt;2&lt;/sub&gt;O  isotopomers by laser spectroscopy&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 813-838, 2012&lt;br /&gt;&lt;br /&gt;Author(s): J. Mohn, B. Tuzson, A. Manninen, N. Yoshida, S. Toyoda, W. A. Brand, and L. Emmenegger&lt;br /&gt;&lt;br /&gt;We describe the first high precision real-time analysis of the
      N&lt;sub&gt;2&lt;/sub&gt;O site-specific isotopic composition at ambient mixing
      ratios. Our technique is based on mid-infrared quantum cascade laser
      absorption spectroscopy (QCLAS) combined with an automated
      preconcentration unit. The QCLAS allows for simultaneous and specific
      analysis of the three main stable N&lt;sub&gt;2&lt;/sub&gt;O isotopic species,
      &lt;sup&gt;14&lt;/sup&gt;N&lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;16&lt;/sup&gt;O, &lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;14&lt;/sup&gt;N&lt;sup&gt;16&lt;/sup&gt;O,
      &lt;sup&gt;14&lt;/sup&gt;N&lt;sup&gt;14&lt;/sup&gt;N&lt;sup&gt;16&lt;/sup&gt;O, and the respective site-specific relative
      isotope ratio differences &amp;delta;&lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;&amp;alpha;&lt;/sup&gt; and &amp;delta;&lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;&amp;beta;&lt;/sup&gt;. Continuous, stand-alone operation is achieved by
      using liquid nitrogen free N&lt;sub&gt;2&lt;/sub&gt;O preconcentration,
      a quasi-room-temperature quantum cascade laser (QCL), quantitative
      sample transfer to the QCLAS, and an optimized calibration
      algorithm. The N&lt;sub&gt;2&lt;/sub&gt;O site-specific isotopic composition (&amp;delta;&lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;&amp;alpha;&lt;/sup&gt; and &amp;delta;&lt;sup&gt;15&lt;/sup&gt;N&lt;sup&gt;&amp;beta;&lt;/sup&gt;) can be analysed
      with a long term precision of 0.2&amp;permil;. The potential of this
      analytical tool is illustrated by continuous N&lt;sub&gt;2&lt;/sub&gt;O isotopomer
      measurements above a grassland plot over three weeks period, which
      allowed identification of microbial source and sink processes.</description><pubDate>Mon, 23 Jan 2012 00:00:00 +0100</pubDate></item><item><title>New dynamic NNORSY ozone profile climatology</title><link>http://www.atmos-meas-tech-discuss.net/5/775/2012/</link><description>&lt;b&gt;New dynamic NNORSY ozone profile climatology&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 775-812, 2012&lt;br /&gt;&lt;br /&gt;Author(s): A. K. Kaifel, M. Felder, C. DeClercq, and J.-C. Lambert&lt;br /&gt;&lt;br /&gt;Climatological ozone profile data are widely used as a-priori information
for total ozone using DOAS type retrievals as well as for ozone profile
retrieval using optimal estimation, for data assimilation or evaluation of
3-D chemistry-transport models and a lot of other applications in
atmospheric sciences and remote sensing. For most applications it is
important that the climatology represents not only long term mean values but
also the links between ozone and dynamic input parameters. These dynamic
input parameters should be easily accessible from auxiliary datasets or
easily measureable, and obviously should have a high correlation with ozone.
For ozone profile these parameters are mainly total ozone column and
temperature profile data. This was the outcome of a user consultation
carried out in the framework of developing a new, dynamic ozone profile
climatology.
&lt;br&gt;&lt;br&gt;
The new ozone profile climatology is based on the Neural Network Ozone
Retrieval System (NNORSY) widely used for ozone profile retrieval from UV
and IR satellite sounder data. NNORSY allows implicit modelling of any
non-linear correspondence between input parameters (predictors) and ozone
profile target vector. This paper presents the approach, setup and
validation of a new family of ozone profile climatologies with static as
well as dynamic input parameters (total ozone and temperature profile). The
neural network training relies on ozone profile measurement data of well
known quality provided by ground based (ozonesondes) and satellite based
(SAGE II, HALOE, and POAM-III) measurements over the years 1995–2007. In
total, four different combinations (modes) for input parameters (date,
geolocation, total ozone column and temperature profile) are available.
&lt;br&gt;&lt;br&gt;
The geophysical validation spans from pole to pole using independent
ozonesonde, lidar and satellite data (ACE-FTS, AURA-MLS) for individual and
time series comparisons as well as for analysing the vertical and meridian
structure of different modes of the NNORSY ozone profile climatology. The
NNORSY ozone profile climatology is available to the community as a
comprehensive software library.</description><pubDate>Wed, 18 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Evaluation of turbulent dissipation rate retrievals from Doppler cloud radar</title><link>http://www.atmos-meas-tech-discuss.net/5/747/2012/</link><description>&lt;b&gt;Evaluation of turbulent dissipation rate retrievals from Doppler cloud radar&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 747-774, 2012&lt;br /&gt;&lt;br /&gt;Author(s): M. D. Shupe, I. M. Brooks, and G. Canut&lt;br /&gt;&lt;br /&gt;Turbulent dissipation rate retrievals from cloud radar Doppler velocity measurements are evaluated
  using independent, in situ observations in Arctic stratocumulus clouds. In situ validation data
  sets of dissipation rate are derived using sonic anemometer measurements from a tethered balloon
  and high frequency pressure variation observations from a research aircraft, both flown in
  proximity to stationary, ground-based radars. Modest biases are found among the data sets in
  particularly low- or high-turbulence regimes, but in general the radar-retrieved values correspond
  well with the in situ measurements. Root mean square differences are typically a factor of 4–6
  relative to any given magnitude of dissipation rate. These differences are no larger than those
  found when comparing dissipation rates computed from tethered-balloon and 15-m tower sonic
  measurements made at spatial distances of a few hundred meters. Moreover, radar retrievals are
  able to capture the vertical dissipation rate structure observed by the in situ sensors, while
  offering substantially more information on the time variability of turbulence profiles. Together
  these evaluations indicate that radar-based retrievals can, at a minimum, be used to determine the
  vertical structure of turbulence in Arctic stratocumulus clouds.</description><pubDate>Wed, 18 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Desert dust satellite retrieval intercomparison</title><link>http://www.atmos-meas-tech-discuss.net/5/691/2012/</link><description>&lt;b&gt;Desert dust satellite retrieval intercomparison&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 691-746, 2012&lt;br /&gt;&lt;br /&gt;Author(s): E. Carboni, G. E. Thomas, A. M. Sayer, R. Siddans, C. A. Poulsen, R. G. Grainger, C. Ahn, D. Antoine, S. Bevan, R. Braak, H. Brindley, S. DeSouza-Machado, J. L. Deuzé, D. Diner, F. Ducos, W. Grey, C. Hsu, O. V. Kalashnikova, R. Kahn, P. R. J. North, C. Salustro, A. Smith, D. Tanré, O. Torres, and B. Veihelmann&lt;br /&gt;&lt;br /&gt;This work provides a comparison of satellite retrievals of Saharan desert
dust aerosol optical depth (AOD) during a strong dust event through March
2006. In this event, a large dust plume was transported over desert,
vegetated, and ocean surfaces. The aim is to identify and understand the
differences between current algorithms, and hence improve future retrieval
algorithms. The satellite instruments considered are AATSR, AIRS, MERIS,
MISR, MODIS, OMI, POLDER, and SEVIRI. An interesting aspect is that the
different algorithms make use of different instrument characteristics to
obtain retrievals over bright surfaces. These include multi-angle approaches
(MISR, AATSR), polarisation measurements (POLDER), single-view approaches
using solar wavelengths (OMI, MODIS), and the thermal infrared spectral
region (SEVIRI, AIRS). Differences between instruments, together with the
comparison of different retrieval algorithms applied to measurements from the
same instrument, provide a unique insight into the performance and
characteristics of the various techniques employed. As well as the
intercomparison between different satellite products, the AODs have also been
compared to co-located AERONET data. Despite the fact that the agreement
between satellite and AERONET AODs is reasonably good for all of the
datasets, there are significant differences between them when compared to
each other, especially over land. These differences are partially due to
differences in the algorithms, such as assumptions about aerosol model and
surface properties. However, in this comparison of spatially and temporally
averaged data, at least as significant as these differences are sampling
issues related to the actual footprint of each instrument on the
heterogeneous aerosol field, cloud identification and the quality control
flags of each dataset.</description><pubDate>Tue, 17 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Sensitivity of the Single Particle Soot Photometer to different black carbon types</title><link>http://www.atmos-meas-tech-discuss.net/5/663/2012/</link><description>&lt;b&gt;Sensitivity of the Single Particle Soot Photometer to different black carbon types&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 663-690, 2012&lt;br /&gt;&lt;br /&gt;Author(s): M. Laborde, P. Mertes, P. Zieger, J. Dommen, U. Baltensperger, and M. Gysel&lt;br /&gt;&lt;br /&gt;Black carbon (BC) is nowadays mainly of anthropogenic origin. It is the
dominant light absorbing component of atmospheric aerosols, playing an
important role in the earth's radiative balance and therefore
relevant to climate change studies. In addition, BC is known to be harmful to
humans making it relevant to policy makers. Nevertheless, the measurement of
BC remains biased by the instrument-based definition of BC. The Single
Particle Soot Photometer (SP2), allows the measurement of the refractory BC
(rBC) mass of individual particle using laser-induced incandescence. However
the SP2 needs an empirical calibration to retrieve the rBC mass from the
incandescence signal and the sensitivity of the SP2 differs between different
BC types. Ideally, for atmospheric studies, the SP2 should be calibrated
using ambient particles containing a known mass of ambient rBC. However, such
&quot;ambient BC&quot; calibration particles cannot easily be obtained and thus
commercially available BC particles are commonly used for SP2 calibration
instead. In this study we tested the sensitivity of the SP2 to different BC
types in order to characterize the potential error introduced by using
non-ambient BC for calibration. The sensitivity of the SP2 was determined for
rBC from thermodenuded diesel exhaust, wood burning exhaust and ambient
particles as well as for commercially available products:
Aquadag&lt;sup&gt;® &lt;/sup&gt; and fullerene soot.
&lt;br&gt;&lt;br&gt;
Thermodenuded, fresh diesel exhaust has been found to be ideal for SP2
calibration for two reasons. First, the small amount of non-BC matter upon
emission reduces the risk of bias due to incomplete removal of non-BC matter
and second, it is considered to represent atmospheric rBC as diesel exhaust
is the main source of BC in most locations. The SP2 was found to be up to
16% less sensitive to rBC from thermodenuded ambient particles (&amp;le;15 fg) than rBC from diesel exhaust, however, at least part of this
difference can be explained by incomplete removal of non-refractory
components in the thermodenuder. The SP2 sensitivity to rBC from wood burning
exhaust agrees with the one of rBC from diesel exhaust within an error of
less than 14% (&amp;le;40 fg).
&lt;br&gt;&lt;br&gt;
If, due to experimental restrictions, diesel exhaust cannot be used,
untreated fullerene soot was found to give a SP2 calibration curve similar to
diesel exhaust and ambient rBC (within ±10% for a rBC mass &amp;le;15 fg) and is therefore recommended although two different batches
differed by ~14% between themselves. In addition, the SP2 was found to
be up to 40% more sensitive to Aquadag&lt;sup&gt;® &lt;/sup&gt;  than to
diesel exhaust rBC. Therefore Aquadag&lt;sup&gt;® &lt;/sup&gt;  cannot be
recommended for atmospheric application. These findings for fullerene soot
and Aquadag&lt;sup&gt;® &lt;/sup&gt;confirm results from previous
literature.</description><pubDate>Tue, 17 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Retrieving aerosol in a cloudy environment: aerosol availability as a function of spatial and temporal resolution</title><link>http://www.atmos-meas-tech-discuss.net/5/627/2012/</link><description>&lt;b&gt;Retrieving aerosol in a cloudy environment: aerosol availability as a function of spatial and temporal resolution&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 627-662, 2012&lt;br /&gt;&lt;br /&gt;Author(s): L. A. Remer, S. Mattoo, R. C. Levy, A. Heidinger, R. B. Pierce, and M. Chin&lt;br /&gt;&lt;br /&gt;The challenge of using satellite observations to retrieve aerosol
      properties in a cloudy environment is to prevent contamination of the
      aerosol signal from clouds, while maintaining sufficient aerosol
      product yield to satisfy specific applications. We investigate aerosol
      retrieval availability at different instrument pixel resolutions,
      using the standard MODIS aerosol cloud mask applied to MODIS data and
      a new GOES-R cloud mask applied to GOES data for a domain covering
      North America and surrounding oceans. Aerosol availability is not the
      same as the cloud free fraction and takes into account the technqiues
      used in the MODIS algorithm to avoid clouds, reduce noise and maintain
      sufficient numbers of aerosol retrievals. The inherent spatial
      resolution of each instrument, 0.5 × 0.5 km for MODIS and
      1 × 1 km for GOES, is systematically degraded to
      1 × 1 km, 2 × 2 km, 4 × 4 km and
      8 × 8 km resolutions and then analyzed as to how that
      degradation would affect the availability of an aerosol retrieval,
      assuming an aerosol product resolution at 8 × 8 km. The
      results show that as pixel size increases, availability decreases
      until at 8 × 8 km 70% to 85% of the retrievals
      available at 0.5 km have been lost. The diurnal pattern of aerosol
      retrieval availability examined for one day in the summer suggests
      that coarse resolution sensors (i.e. 4 × 4 km or
      8 × 8 km) may be able to retrieve aerosol early in the
      morning that would otherwise be missed at the time of current polar
      orbiting satellites, but not the diurnal aerosol properties due to
      cloud cover developed during the day. In contrast finer resolution
      sensors (i.e. 1 × 1 km or 2 × 2 km) have much
      better opportunity to retrieve aerosols in the partly cloudy scenes
      and better chance of returning the diurnal aerosol properties. Large
      differences in the results of the two cloud masks designed for MODIS
      aerosol and GOES cloud products strongly reinforce that cloud masks
      must be developed with specific purposes in mind and that a generic
      cloud mask applied to an independent aerosol retrieval will likely
      fail.</description><pubDate>Fri, 13 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Multi-wavelength Raman lidar, sunphotometric and aircraft measurements in combination with inversion models for the estimation of the aerosol optical and physico-chemical properties over Athens, Greece</title><link>http://www.atmos-meas-tech-discuss.net/5/589/2012/</link><description>&lt;b&gt;Multi-wavelength Raman lidar, sunphotometric and aircraft measurements in combination with inversion models for the estimation of the aerosol optical and physico-chemical properties over Athens, Greece&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 589-625, 2012&lt;br /&gt;&lt;br /&gt;Author(s): R. E. Mamouri, A. Papayannis, V. Amiridis, D. Müller, P. Kokkalis, S. Rapsomanikis, E. T. Karageorgos, G. Tsaknakis, A. Nenes, S. Kazadzis, and E. Remoundaki&lt;br /&gt;&lt;br /&gt;A novel procedure has been developed to retrieve, simultaneously, the
optical, microphysical and chemical properties of tropospheric aerosols with
a multi-wavelength Raman lidar system in the troposphere over an urban site
(Athens, Greece: 37.9° N, 23.6° E, 200 m a.s.l.) using data obtained
during the European Space Agency (ESA) THERMOPOLIS project which took place
between 15–31 July 2009 over the Greater Athens Area (GAA). We selected to
apply our procedure for a case study of intense aerosol layers occurred on
20–21 July 2009. The National Technical University of Athens (NTUA) EOLE
6-wavelength Raman lidar system has been used to provide the vertical
profiles of the optical properties of aerosols (extinction and backscatter
coefficients, lidar ratio) and the water vapor mixing ratio. An inversion
algorithm was used to derive the mean aerosol microphysical properties (mean
effective radius – &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt;), single-scattering albedo (ω) and mean complex
refractive index (&lt;i&gt;m&lt;/i&gt;) at selected heights in the 2–3 km height region. We found
that &lt;i&gt;r&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt; was 0.3–0.4 μm, ω at 532 nm ranged from 0.63 to 0.88 and
&lt;i&gt;m&lt;/i&gt; ranged from 1.45 + 0.015&lt;i&gt;i&lt;/i&gt; to 1.56 + 0.05&lt;i&gt;i&lt;/i&gt;, in good accordance with in situ aircraft
measurements. The final data set of the aerosol microphysical properties
along with the water vapor and temperature profiles were incorporated into
the ISORROPIA model to infer an in situ aerosol composition consistent with the
retrieved &lt;i&gt;m&lt;/i&gt; and ω values. The retrieved aerosol chemical composition in the
2–3 km height region gave a variable range of sulfate (0–60%) and organic
carbon (OC) content (0–50%), although the OC content increased (up to
50%) and the sulfate content dropped (up to 30%) around 3 km height;
in connection with the retrieved low ω value (0.63), indicates the presence
of absorbing biomass burning smoke mixed with urban haze. Finally, the
retrieved aerosol microphysical properties were compared with
column-integrated sunphotometer data.</description><pubDate>Fri, 13 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Validation of ACE and OSIRIS ozone and NO&lt;sub&gt;2&lt;/sub&gt; measurements using ground-based instruments at 80° N</title><link>http://www.atmos-meas-tech-discuss.net/5/517/2012/</link><description>&lt;b&gt;Validation of ACE and OSIRIS ozone and NO&lt;sub&gt;2&lt;/sub&gt; measurements using ground-based instruments at 80° N&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 517-588, 2012&lt;br /&gt;&lt;br /&gt;Author(s): C. Adams, K. Strong, R. L. Batchelor, P. F. Bernath, S. Brohede, C. Boone, D. Degenstein, W. H. Daffer, J. R. Drummond, P. F. Fogal, E. Farahani, C. Fayt, A. Fraser, F. Goutail, F. Hendrick, F. Kolonjari, R. Lindenmaier, G. Manney, C. T. McElroy, C. A. McLinden, J. Mendonca, J.-H. Park, B. Pavlovic, A. Pazmino, C. Roth, V. Savastiouk, K. A. Walker, D. Weaver, and X. Zhao&lt;br /&gt;&lt;br /&gt;The Optical Spectrograph and Infra-Red Imager System (OSIRIS) and the
Atmospheric Chemistry Experiment (ACE) have been taking measurements from
space since 2001 and 2003, respectively. This paper presents intercomparisons
between ozone and NO&lt;sub&gt;2&lt;/sub&gt; measured by the ACE and OSIRIS satellite
instruments and by ground-based instruments at the Polar Environment
Atmospheric Research Laboratory (PEARL), which is located at Eureka, Canada
(80° N, 86° W) and is operated by the Canadian Network for
the Detection of Atmospheric Change (CANDAC). The ground-based instruments
included in this study are four zenith-sky differential optical absorption
spectroscopy (DOAS) instruments, one Bruker Fourier transform infrared
spectrometer (FTIR) and four Brewer spectrophotometers. Ozone total columns
measured by the DOAS instruments were retrieved using new Network for the
Detection of Atmospheric Composition Change (NDACC) guidelines and agree to
within 3.2%. The DOAS ozone columns agree with the Brewer
spectrophotometers with mean relative differences that are smaller than
1.5%. This suggests that for these instruments the new NDACC data
guidelines were successful in producing a homogenous and accurate ozone
dataset at 80° N. Satellite 14–52 km ozone and 17–40 km NO&lt;sub&gt;2&lt;/sub&gt;
partial columns within 500 km of PEARL were calculated for ACE-FTS Version
2.2 (v2.2) plus updates, ACE-FTS v3.0, ACE-MAESTRO (Measurements of Aerosol
Extinction in the Stratosphere and Troposphere Retrieved by Occultation) v1.2
and OSIRIS SaskMART v5.0x ozone and Optimal Estimation v3.0 NO&lt;sub&gt;2&lt;/sub&gt; data
products. The new ACE-FTS v3.0 and the validated ACE-FTS v2.2 partial columns
are nearly identical, with mean relative differences of 0.0 ± 0.2%
for ozone and −0.2 ± 0.1% for v2.2 minus v3.3 NO&lt;sub&gt;2&lt;/sub&gt;. Ozone
columns were constructed from 14–52 km satellite and 0–14 km ozonesonde
partial columns and compared with the ground-based total column measurements.
The satellite-plus-sonde measurements agree with the ground-based ozone total
columns with mean relative differences of 0.1–7.3%. For NO&lt;sub&gt;2&lt;/sub&gt;, partial
columns from 17 km upward were scaled to noon using a photochemical model.
Mean relative differences between OSIRIS, ACE-FTS and ground-based
NO&lt;sub&gt;2&lt;/sub&gt; measurements do not exceed 20%. ACE-MAESTRO measures more
NO&lt;sub&gt;2&lt;/sub&gt; than the other instruments, with mean relative differences of
25–52%. Seasonal variation in the differences between partial columns is
observed, suggesting that there are systematic errors in the measurements,
the photochemical model corrections, and/or in the coincidence criteria. For
ozone spring-time measurements, additional coincidence criteria based on
stratospheric temperature and the location of the polar vortex were found to
improve agreement between some of the instruments. For ACE-FTS v2.2 minus
Bruker FTIR, the 2007–2009 spring-time mean relative difference improved
from −5.0 ± 0.4% to −3.1 ± 0.8% with the dynamical
selection criteria. This was the largest improvement, likely because both
instruments measure direct sunlight and therefore have well-characterized
lines-of-sight compared with scattered sunlight measurements. For NO&lt;sub&gt;2&lt;/sub&gt;,
the addition of a ±1° latitude coincidence criterion improved
spring-time intercomparison results, likely due to the sharp latitudinal
gradient of NO&lt;sub&gt;2&lt;/sub&gt; during polar sunrise. The differences between satellite
and ground-based measurements do not show any obvious trends over the
missions, indicating that both the ACE and OSIRIS instruments continue to
perform well.</description><pubDate>Thu, 12 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Relative drifts and stability of satellite and ground-based stratospheric ozone profiles at NDACC lidar stations</title><link>http://www.atmos-meas-tech-discuss.net/5/471/2012/</link><description>&lt;b&gt;Relative drifts and stability of satellite and ground-based stratospheric ozone profiles at NDACC lidar stations&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 471-516, 2012&lt;br /&gt;&lt;br /&gt;Author(s): P. J. Nair, S. Godin-Beekmann, L. Froidevaux, L. E. Flynn, J. M. Zawodny, J. M. Russell III, A. Pazmiño, G. Ancellet, W. Steinbrecht, H. Claude, T. Leblanc, S. McDermid, J. A. E. van Gijsel, B. Johnson, A. Thomas, D. Hubert, J.-C. Lambert, and H. Nakane&lt;br /&gt;&lt;br /&gt;The long-term evolution of stratospheric ozone at different stations
      in the low and mid-latitudes is investigated. The analysis is
      performed by comparing the collocated profiles of ozone lidars, at the
      northern mid-latitudes (Meteorological Observatory
      Hohenpeißenberg, Haute-Provence Observatory, Tsukuba and Table
      Mountain Facility), tropics (Mauna Loa Observatory) and southern
      mid-latitudes (Lauder), with ozonesondes and space-borne sensors
      (SBUV(/2), SAGE II, HALOE, UARS MLS and Aura MLS), extracted around
      the stations. Relative differences are calculated to find biases and
      temporal drifts in the measurements. All measurement techniques show
      their best agreement with respect to the lidar at 20–40 km, where
      the differences are within &amp;plusmn;3% and drifts are less than
      &amp;plusmn;0.3% yr&lt;sup&gt;&amp;minus;1&lt;/sup&gt; at all stations. In addition, the
      stability of the long-term ozone observations (lidar, SBUV(/2), SAGE
      II and HALOE) is evaluated by the cross-comparison of each data
      set. In general, all lidars and SBUV(/2) exhibit near zero drifts and
      the comparison between SAGE II and HALOE shows larger, but
      insignificant drifts. The RMS of the drifts of lidar and SBUV(/2) is
      0.22 and 0.27% yr&lt;sup&gt;&amp;minus;1&lt;/sup&gt;, respectively.  The average drifts of
      the long-term data sets, derived from various comparisons, are less
      than &amp;plusmn;0.3% yr&lt;sup&gt;&amp;minus;1&lt;/sup&gt; in 20–40 km at all stations.
      A combined time series of the relative differences between SAGE II,
      HALOE and Aura MLS with respect to lidar data at six sites is
      constructed, to obtain long-term data sets lasting up to 27 yr.
      The relative drifts derived from these combined data are very small,
      within &amp;plusmn;0.2% yr&lt;sup&gt;&amp;minus;1&lt;/sup&gt;.</description><pubDate>Thu, 12 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Using sonic anemometer temperature to measure sensible heat flux in strong winds</title><link>http://www.atmos-meas-tech-discuss.net/5/447/2012/</link><description>&lt;b&gt;Using sonic anemometer temperature to measure sensible heat flux in strong winds&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 447-469, 2012&lt;br /&gt;&lt;br /&gt;Author(s): S. P. Burns, T. W. Horst, P. D. Blanken, and R. K. Monson&lt;br /&gt;&lt;br /&gt;The sensible heat flux (&lt;i&gt;H&lt;/i&gt;) is a significant component of the surface
energy balance (SEB). Sonic anemometers simultaneously measure the
turbulent fluctuations of vertical wind (&lt;i&gt;w&lt;/i&gt;') and sonic temperature
(&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;s&lt;/sub&gt;'), and are commonly used to measure &lt;i&gt;H&lt;/i&gt;. Our study examines
30-min heat fluxes measured with a Campbell Scientific model CSAT3
sonic anemometer above a subalpine forest. We compare &lt;i&gt;H&lt;/i&gt; calculated
with &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;s&lt;/sub&gt; to &lt;i&gt;H&lt;/i&gt; calculated with a co-located thermocouple and find
that for horizontal wind speed (&lt;i&gt;U&lt;/i&gt;) less than 8 m s&lt;sup&gt;−1&lt;/sup&gt; the
agreement is &amp;asymp;&amp;plusmn;30 W m&lt;sup&gt;−2&lt;/sup&gt;. However, for &lt;i&gt;U&lt;/i&gt; &amp;gt;&amp;asymp; 8 m s&lt;sup&gt;−1&lt;/sup&gt;,
the CSAT3 &lt;i&gt;H&lt;/i&gt; becomes larger than &lt;i&gt;H&lt;/i&gt;
calculated with the thermocouple, reaching a maximum difference of
≈250 W m&lt;sup&gt;−2&lt;/sup&gt; at &lt;i&gt;U&lt;/i&gt; ≈ 18 m s&lt;sup&gt;−1&lt;/sup&gt;. &lt;i&gt;H&lt;/i&gt; calculated
with the thermocouple results in a SEB that is relatively independent
of &lt;i&gt;U&lt;/i&gt; at high wind speeds. In contrast, the SEB calculated with &lt;i&gt;H&lt;/i&gt;
from the CSAT3 varies considerably with &lt;i&gt;U&lt;/i&gt;, particularly at night.
Cospectral analysis of &lt;span style=&quot;border-top: 1px solid #000;color:#000;&quot;&gt;&lt;i&gt;w&lt;/i&gt;'&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;s&lt;/sub&gt;'&lt;/span&gt; suggest that spurious
correlation is a problem during high winds which leads to a positive
(additive) increase in &lt;i&gt;H&lt;/i&gt; calculated with the CSAT3. At night, when
&lt;i&gt;H&lt;/i&gt; is typically negative, this CSAT3 error results in a measured &lt;i&gt;H&lt;/i&gt;
that falsely approaches zero or even becomes positive. Within a
broader context, the usefulness of side-by-side instrument comparisons
are discussed.</description><pubDate>Thu, 12 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Using Markov switching models to infer dry and rainy periods from telecommunication microwave link signals</title><link>http://www.atmos-meas-tech-discuss.net/5/411/2012/</link><description>&lt;b&gt;Using Markov switching models to infer dry and rainy periods from telecommunication microwave link signals&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 411-445, 2012&lt;br /&gt;&lt;br /&gt;Author(s): Z. Wang, M. Schleiss, J. Jaffrain, A. Berne, and J. Rieckermann&lt;br /&gt;&lt;br /&gt;A Markov switching algorithm is introduced to classify
      attenuation measurements from telecommunication microwave
      links into dry and rainy periods. It is based on a simple
      state-space model and has the advantage of not relying on
      empirically estimated threshold parameters. The algorithm is
      applied to data collected using a new and original
      experimental set-up in the vicinity of Zürich,
      Switzerland. The false dry and false rain detection rates of
      the algorithm are evaluated and compared to 3 other algorithms
      from the literature. The results show that, on average, the
      Markov switching model outperforms the other algorithms. It is
      also shown that the classification performance can be further
      improved if redundant information from multiple channels is
      used.</description><pubDate>Thu, 12 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Atmospheric effect on the ground-based measurements of broadband surface albedo</title><link>http://www.atmos-meas-tech-discuss.net/5/385/2012/</link><description>&lt;b&gt;Atmospheric effect on the ground-based measurements of broadband surface albedo&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Atmospheric Measurement Techniques Discussions, 5, 385-409, 2012&lt;br /&gt;&lt;br /&gt;Author(s): T. Manninen, A. Riihelä, and G. de Leeuw&lt;br /&gt;&lt;br /&gt;Ground-based pyranometer measurements of broadband surface albedo values are
affected by the atmospheric conditions. A new method for estimating the
magnitude of this effect in clear sky conditions is presented. Global and
reflected radiation values and AOD values at two wavelengths are needed to
apply the method. Depending on the atmospheric optical depth and the sun
zenith angle values the effect can be as large as 20%. For the test case
of Cabauw the atmosphere caused typically 5% higher surface albedo values
than the corresponding black-sky surface albedo values.</description><pubDate>Wed, 11 Jan 2012 00:00:00 +0100</pubDate></item></channel></rss>
