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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics Discussions</journal_title>
		<journal_url>www.atmos-chem-phys-discuss.net</journal_url>
		<issn>1680-7367</issn>
		<eissn>1680-7375</eissn>
		<volume_number>5</volume_number>
		<issue_number>5</issue_number>
		<publication_year>2005</publication_year>
	</journal>
	<doi>10.5194/acpd-5-10155-2005</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/5/10155/2005/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/5/10155/2005/acpd-5-10155-2005.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/5/10155/2005/acpd-5-10155-2005.pdf</fulltext_pdf>
	<start_page>10155</start_page>
	<end_page>10195</end_page>
	<publication_date>2005-10-19</publication_date>
	<article_title content_type="html">Robust relations between CCN and the vertical evolution of cloud drop size distribution in deep convective clouds</article_title>
	<authors>
		<author numeration="1" affiliations="1,2">
			<name>E. Freud</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>D. Rosenfeld</name>
		</author>
		<author numeration="3" affiliations="3">
			<name>M. O. Andreae</name>
		</author>
		<author numeration="4" affiliations="4">
			<name>A. A. Costa</name>
		</author>
		<author numeration="5" affiliations="5">
			<name>P. Artaxo</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Institute of Earth Sciences, The Hebrew University of Jerusalem, Jerusalem, Israel</affiliation>
		<affiliation numeration="2" content_type="html">Department of Applied Environmental Sciences, Stockholm University, Stockholm, Sweden</affiliation>
		<affiliation numeration="3" content_type="html">Biogeochemistry Department, Max Planck Institute for Chemistry, Mainz, Germany</affiliation>
		<affiliation numeration="4" content_type="html">Department of Geology and Geophysics, Yale University, CT, USA</affiliation>
		<affiliation numeration="5" content_type="html">Institute of Physics, Sao Paulo University, Brazil</affiliation>
	</affiliations>
	<abstract content_type="html">In-situ measurements in convective clouds (up to the freezing level) over the Amazon
basin show that smoke from deforestation fires prevents clouds from precipitating until they
acquire a vertical development of at least 4 km, compared to only 1&amp;ndash;2 km in clean clouds. The
average cloud depth required for the onset of warm rain increased by ~350 m for each
additional 100 cloud condensation nuclei per cm&lt;sup&gt;3&lt;/sup&gt; at a super-saturation of 0.5% (&lt;I&gt;CCN&lt;/I&gt;&lt;sub&gt;0.5%&lt;/sub&gt;). In
polluted clouds, the diameter of modal liquid water content grows much slower with cloud
depth (at least by a factor of ~2), due to the large number of droplets that compete for
available water and to the suppressed coalescence processes. Contrary to what other studies
have suggested, we did not observe this effect to reach saturation at 3000 or more
accumulation mode particles per cm&lt;sup&gt;3&lt;/sup&gt;. The &lt;I&gt;CCN&lt;/I&gt;&lt;sub&gt;0.5%&lt;/sub&gt; concentration was found to be a very good
predictor for the cloud depth required for the onset of warm precipitation and other
microphysical factors, leaving only a secondary role for the updraft velocities in determining
the cloud drop size distributions.

&lt;br&gt;&lt;br&gt;
The effective radius of the cloud droplets (&lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt;) was found to be a quite robust parameter for
a given environment and cloud depth, showing only a small effect of partial droplet
evaporation from the cloud&apos;s mixing with its drier environment. This supports one of the basic
assumptions of satellite analysis of cloud microphysical processes: the ability to look at
different cloud top heights in the same region and regard their &lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt; as if they had been measured
inside one well developed cloud. The dependence of &lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt; on the adiabatic fraction decreased
higher in the clouds, especially for cleaner conditions, and disappeared at &lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt;&amp;#x2265;~10 &amp;micro;m. We
propose that droplet coalescence, which is at its peak when warm rain is formed in the cloud
at &lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt;~10 &amp;micro;m, continues to be significant during the cloud&apos;s mixing with the entrained air,
canceling out the decrease in &lt;i&gt;r&lt;sub&gt;e&lt;/sub&gt;&lt;/i&gt; due to evaporation.</abstract>
	<references>
	</references>
</article>

