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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ACPD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACPD</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7375</issn>
<publisher><publisher-name>Copernicus GmbH</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acpd-11-24631-2011</article-id>
<title-group>
<article-title>Physical and optical properties of 2010 Eyjafjallajökull volcanic eruption aerosol: ground-based, LIDAR and airborne measurements in France</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hervo</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Quennehen</surname>
<given-names>B.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kristiansen</surname>
<given-names>N. I.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Boulon</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Stohl</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fréville</surname>
<given-names>P.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Pichon</surname>
<given-names>J. M.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Picard</surname>
<given-names>D.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Labazuy</surname>
<given-names>P.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gouhier</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Colomb</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Schwarzenboeck</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sellegri</surname>
<given-names>K.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Laboratoire de Météorologie Physique, Observatoire de Physique du Globe de Clermont-Ferrand, Université Blaise Pascal, CNRS UMR6016 – 24 avenue des Landais, 63177 Aubière cedex, France</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Laboratoire Magma et Volcan, Observatoire de Physique du Globe de Clermont-Ferrand, Université Blaise Pascal, CNRS, Clermont-Ferrand, France</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Norwegian Institute for Air Research, Kjeller, Norway</addr-line>
</aff>
<pub-date pub-type="epub">
<day>01</day>
<month>09</month>
<year>2011</year>
</pub-date>
<volume>11</volume>
<issue>9</issue>
<fpage>24631</fpage>
<lpage>24670</lpage>
<permissions>
<license xlink:type="simple">
<license-p>This is an open-access article ditributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.</license-p>
</license>
</permissions>
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<abstract>
<p>During the Eyjafjallajökull eruption (14 April to 24 May 2010), the
volcanic aerosol cloud was observed across Europe by several airborne
in-situ and ground-based remote-sensing instruments. On 18 and 19 May,
layers of depolarizing particles (i.e. non-spherical particles) were
detected in the free troposphere above the Puy de Dôme station, (France)
with a Rayleigh-Mie LIDAR emitting at a wavelength of 355 nm, with parallel
and crossed polarization channels. These layers in the free troposphere (FT)
were also well captured by simulations with the Lagrangian particle
dispersion model FLEXPART, which furthermore showed that the ash was
eventually entrained into the planetary boundary layer (PBL). Indeed, the
ash cloud was then detected and characterized with a comprehensive set of
in-situ instruments at the Puy de Dôme station (PdD). In agreement with
the FLEXPART simulation, up to 65 μg m&lt;sup&gt;−3&lt;/sup&gt; of particle mass and
2.2 ppb of SO&lt;sub&gt;2&lt;/sub&gt; were measured at PdD, corresponding to concentrations higher
than the 95 percentile of 2 years of measurements at PdD. Moreover, the
number concentration of particles increased to 24 000 cm&lt;sup&gt;−3&lt;/sup&gt;, mainly in
the submicronic mode, but a supermicronic mode was also detected at 2 μm.
The resulting optical properties of the ash aerosol were characterized
by a low Ångström exponent (1.1), showing the dominance of
supermicronic particles. For the first time to our knowledge, the
combination of in-situ optical and physical characterization of the volcanic
ash allowed the calculation of the mass-to-extinction ratio (η) with
no assumptions on the aerosol density, which was found to be significantly
different from the background boundary layer aerosol (max: 1.42 g m&lt;sup&gt;−2&lt;/sup&gt;
as opposed to 0.27 ± 0.03 g m&lt;sup&gt;−2&lt;/sup&gt;). Using this
ratio, ash mass concentration in the volcanic plume derived from LIDAR
measurements was found to be 700 ± 25 μg m&lt;sup&gt;−3&lt;/sup&gt; when the plume was
located in the FT (3000 m a.s.l. – above sea level).
&lt;br&gt;&lt;/br&gt;
This ratio could also be used to retrieve an aerosol mass concentration of
523 ± 54 μg m&lt;sup&gt;−3&lt;/sup&gt; on 19 April, when LIDAR observations detected
the ash cloud at 3000 m a.s.l. in correspondence with model simulations
(FLEXPART). On 22 April, another ash plume entered the BL, and although it
was more diluted than during the May episode, the French research aircraft
ATR42 that passed over Clermont-Ferrand in the PBL confirmed the presence of
particles with a supermicronic mode, again centred on a diameter of 2 μm.
&lt;br&gt;&lt;/br&gt;
This data set combining airborne, ground-based and remote sensing
observations with dispersion model simulations shows an overall very good
coherence during the volcanic eruption period, which allows a good
confidence in the characteristics of the ash particles that can be derived
from this unique data set.</p>
</abstract>
<counts><page-count count="40"/></counts>
</article-meta>
</front>
<body/>
<back>
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