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<article language="en">
	<journal>
		<journal_title>The Cryosphere Discussions</journal_title>
		<journal_url>www.the-cryosphere-discuss.net</journal_url>
		<issn>1994-0432</issn>
		<eissn>1994-0440</eissn>
		<volume_number>6</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2012</publication_year>
	</journal>
	<doi>10.5194/tcd-6-125-2012</doi>
	<article_url>http://www.the-cryosphere-discuss.net/6/125/2012/</article_url>
	<abstract_html>http://www.the-cryosphere-discuss.net/6/125/2012/tcd-6-125-2012.html</abstract_html>
	<fulltext_pdf>http://www.the-cryosphere-discuss.net/6/125/2012/tcd-6-125-2012.pdf</fulltext_pdf>
	<start_page>125</start_page>
	<end_page>158</end_page>
	<publication_date>2012-01-13</publication_date>
	<article_title content_type="html">Initial sea-ice growth in open water: properties of grease ice and nilas</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>A. K. Naumann</name>
			<email>ann-kristin.naumann@zmaw.de</email>
		</author>
		<author numeration="2" affiliations="1">
			<name>D. Notz</name>
		</author>
		<author numeration="3" affiliations="2">
			<name>L. Håvik</name>
		</author>
		<author numeration="4" affiliations="2">
			<name>A. Sirevaag</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Max Planck Institute for Meteorology, Hamburg, Germany</affiliation>
		<affiliation numeration="2" content_type="html">Bjerknes Centre for Climate Research, University of Bergen, Bergen, Norway</affiliation>
	</affiliations>
	<abstract content_type="html">To investigate initial sea-ice growth in open water, we carried out an
      ice-tank study with three different setups: grease ice grew in
      experiments with waves and in experiments with a current and wind,
      while nilas formed in a quiescent experimental setup. In this paper we
      focus on the differences in bulk salinity, solid fraction and
      thickness between these two ice types.
&lt;br&gt;&lt;/br&gt;
      We find that the bulk salinity of the grease-ice layer remains almost
      constant until the ice starts to consolidate. In contrast, the bulk
      salinity of nilas is in the first hours of ice formation well
      described by a linear decrease of 2.1 g kg&lt;sup&gt;−1&lt;/sup&gt; h&lt;sup&gt;−1&lt;/sup&gt;
      independent of air temperature.  Such rapid decrease in bulk salinity
      can be understood qualitatively in the light of a Rayleigh number, the
      maximum of which is reached while the nilas is still less than
      1 cm thick.
&lt;br&gt;&lt;/br&gt;
      Comparing three different methods to measure solid fraction in grease
      ice based on (a) salt conservation, (b) mass conservation and (c)
      energy conservation, we find that the method based on salt
      conservation does not give reliable results if the salinity of the
      interstitial water is approximated as being equal to the salinity of
      the upper water layer. Instead the increase in salinity of the
      interstitial water during grease-ice formation must be taken into
      account. We find that the solid fraction of grease ice is relatively
      constant with values of 0.25, whereas it increases to values as high
      as 0.5 as soon as the grease ice consolidates at its surface. In
      contrast, the solid fraction of nilas increases continuously in the
      first hours of ice formation.
&lt;br&gt;&lt;/br&gt;
      The ice thickness is found to be twice as large in the first 24 h of
      ice formation in the setup with a current and wind compared to the
      other two setups, since the wind keeps parts of the water surface ice
      free. The development of the ice thickness can be reproduced well with
      simple, one dimensional models given only the air temperature or the
      ice surface temperature.</abstract>
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</article>

