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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ACP</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7324</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/acp-11-4739-2011</article-id>
<title-group>
<article-title>Measurements of the timescales for the mass transfer of water in glassy aerosol at low relative humidity and ambient temperature</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tong</surname>
<given-names>H.-J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Reid</surname>
<given-names>J. 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>Bones</surname>
<given-names>D. L.</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>Luo</surname>
<given-names>B. P.</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>Krieger</surname>
<given-names>U. K.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>School of Chemistry, University of Bristol, Bristol, BS8 1TS, UK</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Institute for Chemical Physics, Beijing Institute of Technology, Beijing 100081, China</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Institute for Atmospheric and Climate Science, ETH Zürich, Zürich, Switzerland</addr-line>
</aff>
<pub-date pub-type="epub">
<day>20</day>
<month>05</month>
<year>2011</year>
</pub-date>
<volume>11</volume>
<issue>10</issue>
<fpage>4739</fpage>
<lpage>4754</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>The influence of glassy states and highly viscous solution phases on the
timescale of aerosol particle equilibration with water vapour is examined.
In particular, the kinetics of mass transfer of water between the condensed
and gas phases has been studied for sucrose solution droplets under
conditions above and below the glass transition relative humidity (RH).
Above the glass transition, sucrose droplets are shown to equilibrate on a
timescale comparable to the change in RH. Below the glass transition, the
timescale for mass transfer is shown to be extremely slow, with particles
remaining in a state of disequilibrium even after timescales of more than
10 000 s. A phenomenological approach for quantifying the time response of
particle size is used to illustrate the influence of the glassy aerosol
state on the kinetics of mass transfer of water: the time is estimated for
the droplet to reach the halfway point from an initial state towards a
disequilibrium state at which the rate of size change decreases below 1 nm
every 10 000 s. This half-time increases above 1000 s once the particle can
be assumed to have formed a glass. The measurements are shown to be
consistent with kinetic simulations of the slow diffusion of water within
the particle bulk. When increasing the RH from below to above the glass
transition, a particle can return to equilibrium with the gas phase on a
timescale of 10&apos;s to 100&apos;s of seconds, once again forming a solution
droplet. This is considerably shorter than the timescale for the size change
of the particle when glassy and suggests that the dissolution of the glassy
core can proceed rapidly, at least at room temperature. Similar behaviour in
the slowing of the mass transfer rate below the glass transition RH is
observed for binary aqueous raffinose solution droplets. Mixed component
droplets of sucrose/sodium chloride/water also show slow equilibration at
low RH, illustrating the importance of understanding the role of the bulk
solution viscosity on the rate of mass transfer with the gas phase, even
under conditions that may not lead to the formation of a glass.</p>
</abstract>
<counts><page-count count="16"/></counts>
</article-meta>
</front>
<body/>
<back>
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