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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>3</volume_number>
		<issue_number>5</issue_number>
		<publication_year>2003</publication_year>
	</journal>
	<doi>10.5194/acpd-3-5399-2003</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/3/5399/2003/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/3/5399/2003/acpd-3-5399-2003.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/3/5399/2003/acpd-3-5399-2003.pdf</fulltext_pdf>
	<start_page>5399</start_page>
	<end_page>5467</end_page>
	<publication_date>2003-10-29</publication_date>
	<article_title content_type="html">Effects of the physical state of tropospheric ammonium-sulfate-nitrate particles on global aerosol direct radiative forcing</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>S. T. Martin</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>H.-M. Hung</name>
		</author>
		<author numeration="3" affiliations="1,2">
			<name>R. J. Park</name>
		</author>
		<author numeration="4" affiliations="1,2">
			<name>D. J. Jacob</name>
		</author>
		<author numeration="5" affiliations="3">
			<name>R. J. D. Spurr</name>
		</author>
		<author numeration="6" affiliations="3">
			<name>K. V. Chance</name>
		</author>
		<author numeration="7" affiliations="4,5">
			<name>V. Chin</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Division of Engineering and Applied Sciences, Harvard University, USA</affiliation>
		<affiliation numeration="2" content_type="html">Department of Earth and Planetary Sciences, Harvard University, USA</affiliation>
		<affiliation numeration="3" content_type="html">Harvard-Smithsonian Center for Astrophysics, USA</affiliation>
		<affiliation numeration="4" content_type="html">School of Earth and Atmospheric Sciences, Georgia Institute of Technology, USA</affiliation>
		<affiliation numeration="5" content_type="html">Laboratory for Atmospheres, NASA Goddard Space Flight Center, USA</affiliation>
	</affiliations>
	<abstract content_type="html">The effect of aqueous versus crystalline sulfate-nitrate-ammonium tropospheric particles
      on global aerosol direct radiative forcing is assessed. A global three-dimensional chemical
      transport model predicts sulfate, nitrate, and ammonium aerosol mass. An aerosol
      thermodynamics model is called twice, once for the upper side (US) and once for lower side (LS)
      of the hysteresis loop of particle phase. On the LS, the sulfate mass budget is
      40% solid ammonium sulfate, 12% letovicite, 11% ammonium bisulfate, and 37% aqueous. The LS nitrate
      mass budget is 26% solid ammonium nitrate, 7% aqueous, and 67% gas-phase nitric acid release
      due to increased volatility upon crystallization. The LS ammonium budget is
      45% solid ammonium sulfate, 10% letovicite, 6% ammonium bisulfate, 4% ammonium nitrate,
      7% ammonia release due to increased volatility, and 28% aqueous. LS aerosol water mass partitions
      as 22% effloresced to the gas-phase and 78% remaining as aerosol mass. The predicted US/LS
      global fields of aerosol mass are employed in a Mie scattering model to generate global US/LS
      aerosol optical properties, including scattering efficiency, single scattering albedo, and
      asymmetry parameter. Global annual average LS optical depth and mass scattering efficiency
      are, respectively, 0.023 and 10.7 m&lt;sup&gt;2&lt;/sup&gt;&amp;nbsp; (g SO&lt;sub&gt;4&lt;/sub&gt;&lt;sup&gt;2&amp;minus;&lt;/sup&gt;)&lt;sup&gt;&amp;minus;1&lt;/sup&gt;, which compare to US values of 0.030 and
      13.9 m&lt;sup&gt;2&lt;/sup&gt; (g SO&lt;sub&gt;4&lt;/sub&gt;&lt;sup&gt;2&amp;minus;&lt;/sup&gt;)&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. Radiative transport is computed, first for a base case having no aerosol and then for the
      two global fields corresponding to the US and LS of the hysteresis loop. Regional, global,
      seasonal, and annual averages of top-of-the-atmosphere aerosol radiative forcing on the LS and
      US (F&lt;sub&gt;L&lt;/sub&gt; and F&lt;sub&gt;U&lt;/sub&gt;, respectively, in W m&lt;sup&gt;2&amp;minus;&lt;/sup&gt;) are calculated. Including both anthropogenic and natural
      emissions, we obtain global annual averages of F&lt;sub&gt;L&lt;/sub&gt; = &amp;minus;0.750, F&lt;sub&gt;U&lt;/sub&gt; =
      &amp;minus;0.930, and &amp;Delta;F&lt;sub&gt;U,L&lt;/sub&gt; = 24% for full sky calculations without clouds and
      F&lt;sub&gt;L&lt;/sub&gt; = &amp;minus;0.485, F&lt;sub&gt;U&lt;/sub&gt; = &amp;minus;0.605, and &amp;Delta;F&lt;sub&gt;U,L&lt;/sub&gt; =
      25% when clouds are included. Regionally, &amp;Delta;F&lt;sub&gt;U,L&lt;/sub&gt; =
      48% over the USA, 55% over Europe, and 34% over East Asia. Seasonally, &amp;Delta;F&lt;sub&gt;U,L&lt;/sub&gt; varies from
      18% in DJF to 75% in SON over the USA. The global annual average contribution from anthropogenic aerosol is
      F&lt;sub&gt;L&lt;/sub&gt; = &amp;minus;0.314 and F&lt;sub&gt;U&lt;/sub&gt; = &amp;minus;0.404, which yield normalized direct radiative forcings
      (G) of G&lt;sub&gt;L&lt;/sub&gt; = &amp;minus;205 W (g SO&lt;sub&gt;4&lt;/sub&gt;&lt;sup&gt;2&amp;minus;&lt;/sup&gt;)&lt;sup&gt;&amp;minus;1&lt;/sup&gt; and
      G&lt;sub&gt;U&lt;/sub&gt; = &amp;minus;264 W (g SO&lt;sub&gt;4&lt;/sub&gt;&lt;sup&gt;2&amp;minus;&lt;/sup&gt;)&lt;sup&gt;&amp;minus;1&lt;/sup&gt;.</abstract>
	<references>
	</references>
</article>

