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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>9</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2009</publication_year>
	</journal>
	<doi>10.5194/acpd-9-4653-2009</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/9/4653/2009/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/9/4653/2009/acpd-9-4653-2009.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/9/4653/2009/acpd-9-4653-2009.pdf</fulltext_pdf>
	<start_page>4653</start_page>
	<end_page>4689</end_page>
	<publication_date>2009-02-24</publication_date>
	<article_title content_type="html">Measurements of particle masses of inorganic salt particles for calibration of  cloud condensation nuclei counters</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>M. Kuwata</name>
			<email>kuwata@atmos.rcast.u-tokyo.ac.jp</email>
		</author>
		<author numeration="2" affiliations="1">
			<name>Y. Kondo</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Research Center for Advanced Science and Technology, the University of  Tokyo, Tokyo, Japan</affiliation>
	</affiliations>
	<abstract content_type="html">We measured the mobility equivalent critical dry diameter for CCN
      activation (&lt;i&gt;d&lt;sub&gt;c&lt;sub&gt;me&lt;/sub&gt;&lt;/sub&gt;&lt;/i&gt;) and the particle mass of size-selected
      (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; and NaCl particles to calibrate a CCN counter
      (CCNC) precisely. The CCNC was operated downstream of a differential
      mobility analyzer (DMA) for the measurement of &lt;i&gt;d&lt;sub&gt;c&lt;sub&gt;me&lt;/sub&gt;&lt;/sub&gt;&lt;/i&gt;. The
      particle mass was measured using an aerosol particle mass analyzer
      (APM) operated downstream of the DMA. The measurement of particle mass
      was conducted for 50–150-nm particles. Effective densities
      (&amp;rho;&lt;sub&gt;eff&lt;/sub&gt;) of (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; particles were
      1.67–1.75  g cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt;, which correspond to the dynamic shape
      factors (χ) of 1.01–1.04. This shows that (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; 
particles are not completely spherical. In the case of NaCl particles,
      &amp;rho;&lt;sub&gt;eff&lt;/sub&gt; was 1.75–1.99 g cm&lt;sup&gt;&amp;minus;3&lt;/sup&gt; and χ was
      1.05–1.14, demonstrating that their particle shape was
      non-spherical. Using these experimental data, the volume equivalent
      critical dry diameter (&lt;i&gt;d&lt;sub&gt;c&lt;sub&gt;ve&lt;/sub&gt;&lt;/sub&gt;&lt;/i&gt;) was calculated, and it was used as
      an input parameter for calculations of critical supersaturation
      (&lt;i&gt;S&lt;/i&gt;). Several thermodynamics models were used for the calculation of
      water activity. When the Pitzer model was employed for the
      calculations, the critical &lt;i&gt;S&lt;/i&gt; calculated for (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; and
      NaCl agreed to well within the uncertainty of 2% (relative). This
      result demonstrates that the use of the Pitzer model for the
      calibration of CCNCs gives the most probable value of &lt;i&gt;S&lt;/i&gt;.</abstract>
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