<?xml version="1.0" encoding="utf-8" standalone="no"?>
<!DOCTYPE article SYSTEM "http://www.atmos-chem-phys-discuss.net/inc/acpd/copernicus.dtd">
<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>3</issue_number>
		<publication_year>2006</publication_year>
	</journal>
	<doi>10.5194/acpd-6-5095-2006</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/6/5095/2006/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/6/5095/2006/acpd-6-5095-2006.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/6/5095/2006/acpd-6-5095-2006.pdf</fulltext_pdf>
	<start_page>5095</start_page>
	<end_page>5136</end_page>
	<publication_date>2006-06-22</publication_date>
	<article_title content_type="html">Radiative forcing by aerosols as derived from the AeroCom present-day and pre-industrial simulations</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>M. Schulz</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>C. Textor</name>
		</author>
		<author numeration="3" affiliations="2">
			<name>S. Kinne</name>
		</author>
		<author numeration="4" affiliations="1">
			<name>Y. Balkanski</name>
		</author>
		<author numeration="5" affiliations="3">
			<name>S. Bauer</name>
		</author>
		<author numeration="6" affiliations="4">
			<name>T. Berntsen</name>
		</author>
		<author numeration="7" affiliations="4">
			<name>T. Berglen</name>
		</author>
		<author numeration="8" affiliations="5,11">
			<name>O. Boucher</name>
		</author>
		<author numeration="9" affiliations="6">
			<name>F. Dentener</name>
		</author>
		<author numeration="10" affiliations="1">
			<name>S. Guibert</name>
		</author>
		<author numeration="11" affiliations="4">
			<name>I. S. A. Isaksen</name>
		</author>
		<author numeration="12" affiliations="4">
			<name>T. Iversen</name>
		</author>
		<author numeration="13" affiliations="3">
			<name>D. Koch</name>
		</author>
		<author numeration="14" affiliations="4">
			<name>A. Kirkevåg</name>
		</author>
		<author numeration="15" affiliations="7">
			<name>X. Liu</name>
		</author>
		<author numeration="16" affiliations="8">
			<name>V. Montanaro</name>
		</author>
		<author numeration="17" affiliations="4">
			<name>G. Myhre</name>
		</author>
		<author numeration="18" affiliations="7">
			<name>J. E. Penner</name>
		</author>
		<author numeration="19" affiliations="8">
			<name>G. Pitari</name>
		</author>
		<author numeration="20" affiliations="9">
			<name>S. Reddy</name>
		</author>
		<author numeration="21" affiliations="4">
			<name>Ø. Seland</name>
		</author>
		<author numeration="22" affiliations="2">
			<name>P. Stier</name>
		</author>
		<author numeration="23" affiliations="10">
			<name>T. Takemura</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Laboratoire des Sciences du Climat et de l’Environnement, CEA-CNRS, Gif-sur-Yvette, France</affiliation>
		<affiliation numeration="2" content_type="html">Max-Planck-Institut f&amp;uuml;r Meteorologie, Centre for Marine and Atmospheric Sciences (ZMAW), Hamburg, Germany</affiliation>
		<affiliation numeration="3" content_type="html">Columbia University, GISS, New York, USA</affiliation>
		<affiliation numeration="4" content_type="html">University of Oslo, Department of Geosciences, Oslo, Norway</affiliation>
		<affiliation numeration="5" content_type="html">Hadley Centre, Met Office, Exeter, UK</affiliation>
		<affiliation numeration="6" content_type="html">EC, Joint Research Centre, Institute for Environment and Sustainability, Climate Change Unit, Italy</affiliation>
		<affiliation numeration="7" content_type="html">Department of Atmospheric, Oceanic and Space Sciences, University of Michigan, Ann Arbor, MI, USA</affiliation>
		<affiliation numeration="8" content_type="html">Dipartimento di Fisica, Universit&amp;agrave; degli Studi L’Aquila, Coppito, Italy</affiliation>
		<affiliation numeration="9" content_type="html">NOAA, Geophysical Fluid Dynamics Laboratory, Princeton, New Jersey, USA</affiliation>
		<affiliation numeration="10" content_type="html">Research Institute for Apllied mechanics, Kyushu University, Fukuoka, Japan</affiliation>
		<affiliation numeration="11" content_type="html">Laboratoire d’Optique Atmospherique, Universit&amp;eacute; des Sciences et Technologies de Lille, CNRS, Villeneuve d’Ascq, France</affiliation>
	</affiliations>
	<abstract content_type="html">Nine different global models with detailed aerosol modules have
independently produced instantaneous direct radiative forcing due to
anthropogenic aerosols. The anthropogenic impact is derived from the
difference of two model simulations with identically prescribed aerosol
emissions, one for present-day and one for pre-industrial conditions. The
difference in the energy budget at the top of the atmosphere (ToA) yields a
new harmonized estimate for the aerosol direct radiative forcing (RF) under
all-sky conditions. On a global annual basis RF is &amp;ndash;0.2 Wm&lt;sup&gt;-2&lt;/sup&gt;, with a
standard deviation of &amp;plusmn;0.2 Wm&lt;sup&gt;-2&lt;/sup&gt;. Anthropogenic nitrate and dust are
not included in this estimate. No model shows a significant positive all-sky
RF. The corresponding clear-sky RF is &amp;ndash;0.6 Wm&lt;sup&gt;-2&lt;/sup&gt;. The cloud-sky RF was
derived based on all-sky and clear-sky RF and modelled cloud cover. It was
significantly different from zero and ranged between &amp;ndash;0.16 and +0.34 Wm&lt;sup&gt;-2&lt;/sup&gt;.
A sensitivity analysis shows that the total aerosol RF is
influenced by considerable diversity in simulated residence times, mass
extinction coefficients and most importantly forcing efficiencies (forcing
per unit optical depth). Forcing efficiency differences among models explain
most of the variability, mainly because all-sky forcing estimates require
proper representation of cloud fields and the correct relative altitude
placement between absorbing aerosol and clouds. The analysis of the sulphate
RF shows that differences in sulphate residence times are compensated by
opposite mass extinction coefficients. This is explained by more sulphate
particle humidity growth and thus higher extinction in models with
short-lived sulphate present at lower altitude and vice versa. Solar
absorption within the atmospheric column is estimated at +0.85 Wm&lt;sup&gt;-2&lt;/sup&gt;.
The local annual average maxima of atmospheric forcing exceed +5 Wm&lt;sup&gt;-2&lt;/sup&gt; confirming the regional character of aerosol impacts on climate. The annual
average surface forcing is &amp;ndash;1.03 Wm&lt;sup&gt;-2&lt;/sup&gt;.</abstract>
	<references>
	</references>
</article>

