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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>6</volume_number>
		<issue_number>4</issue_number>
		<publication_year>2006</publication_year>
	</journal>
	<doi>10.5194/acpd-6-8241-2006</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/6/8241/2006/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/6/8241/2006/acpd-6-8241-2006.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/6/8241/2006/acpd-6-8241-2006.pdf</fulltext_pdf>
	<start_page>8241</start_page>
	<end_page>8284</end_page>
	<publication_date>2006-08-29</publication_date>
	<article_title content_type="html">Mesoscale modelling of water vapour in the tropical UTLS: two case studies from the HIBISCUS campaign</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>V. Marécal</name>
		</author>
		<author numeration="2" affiliations="2,3">
			<name>G. Durry</name>
		</author>
		<author numeration="3" affiliations="4">
			<name>K. Longo</name>
		</author>
		<author numeration="4" affiliations="4">
			<name>S. Freitas</name>
		</author>
		<author numeration="5" affiliations="2">
			<name>E. D. Rivière</name>
		</author>
		<author numeration="6" affiliations="1">
			<name>M. Pirre</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Laboratoire de Physique et Chimie de l’Environnement, CNRS and Université d’Orléans, 3A Avenue de la Recherche Scientifique, 45071 Orléans cedex 2, France</affiliation>
		<affiliation numeration="2" content_type="html">Groupe de Spectroscopie Moléculaire et Atmosphérique, CNRS and Université de Reims, Moulin de la Housse, B.P. 1039, 51687 Reims Cedex, France</affiliation>
		<affiliation numeration="3" content_type="html">Service d’Aéronomie, CNRS and Institut Pierre Simon Laplace, 91371 Verrières-le-Buisson Cedex, France</affiliation>
		<affiliation numeration="4" content_type="html">Centro de Previs&amp;#2227;o de Tempo e Estudos Climàticos, Rodovia Presidente Dutra, km 40 SPRJ 12630-000, Cachoeira Paulista – SP, Brazil</affiliation>
	</affiliations>
	<abstract content_type="html">In this study, we evaluate the ability of the BRAMS mesoscale model compared
to ECMWF global analysis to simulate the observed vertical variations of
water vapour in the tropical upper troposphere and lower stratosphere
(UTLS). The observations are balloon-borne measurements of water vapour
mixing ratio and temperature from micro-SDLA (Tunable Diode Laser
Spectrometer) instrument. Data from two balloon flights performed during the
2004 HIBISCUS field campaign are used to compare with the mesoscale
simulations and to ECMWF analysis.

&lt;br&gt;&lt;br&gt;
The mesoscale model performs significantly better than ECMWF analysis for
water vapour in the upper troposphere and similarly or slightly worse for
temperature. The improvement provided by the mesoscale model for water
vapour comes mainly from (i) the enhanced vertical resolution in the UTLS
(250 m for BRAMS and ~1 km for ECMWF model) and (ii) the more detailed
microphysical parameterization providing ice supersaturations as in the
observations. The ECMWF vertical resolution (~1 km) is too coarse to
capture the observed fine scale vertical variations of water vapour in the
UTLS. In near saturated or supersaturated layers, the mesoscale model
relative humidity with respect to ice saturation is close to observations
provided that the temperature profile is realistic. For temperature, ECMWF
analysis gives good results partly thanks to data assimilation. The analysis
of the mesoscale model results showed that in undersaturated layers, the
water vapour profile depends mainly on the dynamics. In
saturated/supersaturated layers, microphysical processes play an important
role and have to be taken into account on top of the dynamical processes to
understand the water vapour profiles.

&lt;br&gt;&lt;br&gt;
In the lower stratosphere, the ECMWF model and the BRAMS model give very
similar water vapour profiles that are significantly dryer than micro-SDLA
measurements. This similarity comes from the fact that BRAMS is initialised
using ECMWF analysis and that no mesoscale process acts in the stratosphere
leading to no modification of the BRAMS results with respect to ECMWF
analysis.</abstract>
	<references>
	</references>
</article>

