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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>6</issue_number>
		<publication_year>2005</publication_year>
	</journal>
	<doi>10.5194/acpd-5-11517-2005</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/5/11517/2005/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/5/11517/2005/acpd-5-11517-2005.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/5/11517/2005/acpd-5-11517-2005.pdf</fulltext_pdf>
	<start_page>11517</start_page>
	<end_page>11555</end_page>
	<publication_date>2005-11-10</publication_date>
	<article_title content_type="html">Conceptual study on nucleation burst evolution in the convective boundary layer – Part III: Physico-chemical characterization</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>O. Hellmuth</name>
			<email>olaf@tropos.de</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Modelling Department, Institute for Tropospheric Research, Permoser Str. 15, 04318 Leipzig, Germany</affiliation>
	</affiliations>
	<abstract content_type="html">In part I of the present paper a revised columnar high-order model
to investigate gas-aerosol interactions in the convective boundary
layer (CBL) was proposed.
In part II the model capability to predict first-, second-, and
third-order moments of meteorological variables in the CBL was
demonstrated using available observational data.
In the present part, the high-order modelling concept is extented to sulfur
and ammonia chemistry as well as to aerosol dynamics.
Based on the previous CBL simulation,
two conceptual scenarios of the evolution of ultrafine condensation nuclei (UCN)
in an anthropogenically influenced CBL are investigated.
The scenarios differ in the treatment of new particle formation, whereas
homogeneous nucleation according to the classical nucleation theory
is considered.
The first scenario considers nucleation
of a binary system consisting of water vapour and sulfuric acid vapour,
the second one on nucleation of a ternary system additionally involving
ammonia.
Here, the two scenarios are discussed in detail, whereas
special attention is payed to the role of turbulence in the formation
of the typical UCN burst behaviour, that can often be observed in
the Prandtl layer.</abstract>
	<references>
	</references>
</article>

