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<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:creator>John A. Moody</dc:creator>
  <dc:date>2010</dc:date>
  <dc:description>&lt;p&gt;Soil moisture, rainfall, runoff, and sediment transport data were collected from four 1-m&lt;sup&gt;2&lt;/sup&gt; hillslope plots after the 2000 Hi Meadow Fire in Colorado. Data were collected daily during three summers, two of which were affected by drought. Maximum 30-minute rainfall intensities, &lt;i&gt;I&lt;sub&gt;30&lt;/sub&gt;&lt;/i&gt;, were less than 20 mm h&lt;sup&gt;-1&lt;/sup&gt; and the average runoff volumes per plot were less than 4.7 L per storm. The data were separated into three sediment transport processes based on rainfall intensity and runoff magnitude: (1) dry ravel, (2) rainsplash, and (3) rainflow and then into eight different particle size classes (&lt;i&gt;D&lt;sub&gt;i&lt;/sub&gt;&lt;/i&gt;). For each class, dry ravel transport had a non-linear dependence on initial soil moisture, &lt;span&gt;θ&lt;/span&gt;&lt;i&gt;&lt;sub&gt;i&lt;/sub&gt;&lt;/i&gt;, with a maximum at intermediate values of &lt;span&gt;θ&lt;/span&gt;&lt;sub&gt;&lt;i&gt;i&lt;/i&gt;&lt;/sub&gt; (5-9 % cm&lt;sup&gt;3&lt;/sup&gt; cm&lt;sup&gt;-3&lt;/sup&gt;). Dry ravel transport rates were small for low &lt;span&gt;θ&lt;/span&gt;&lt;i&gt;&lt;sub&gt;i&lt;/sub&gt;&lt;/i&gt; , which may be caused by a cementation process, and also small for high &lt;span&gt;θ&lt;/span&gt;&lt;sub&gt;&lt;i&gt;i&lt;/i&gt;&lt;/sub&gt; , which may be caused by increased surface tension. Rainsplash transport was confined to the &lt;i&gt;I&lt;sub&gt;30&lt;/sub&gt;&lt;/i&gt; domain from 1-7 mm h&lt;sup&gt;-1&lt;/sup&gt; was proportional to &lt;i&gt;D&lt;sub&gt;i&lt;/sub&gt;&lt;/i&gt;(&lt;i&gt;I&lt;/i&gt;&lt;sup&gt;max&lt;/sup&gt;&lt;sub&gt;30&lt;/sub&gt;)&lt;sup&gt;0.63&lt;/sup&gt;. Rainflow transport (&lt;i&gt;I&lt;sub&gt;30&lt;/sub&gt;&lt;/i&gt; &amp;gt; 7 mm h&lt;sup&gt;-1&lt;/sup&gt;) in shallow flows (&lt;i&gt;h&lt;/i&gt; &amp;lt; 2 mm) was most likely dominated by particles rolling. It had a non-linear dependence on &lt;i&gt;D&lt;sub&gt;i&lt;/sub&gt;&lt;/i&gt; with maximum transport of sediment in the 2-4 mm size class. Transport also depended on stream power, but critical stream power was essentially zero, which may indicate that the rainsplash preceding runoff detached soil for transport by overland flow. &lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:language>en</dc:language>
  <dc:title>Plot-scale sediment transport processes on a burned hillslope as a function of particle size</dc:title>
  <dc:type>text</dc:type>
</oai_dc:dc>