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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:contributor>Barbara I. Anderson</dc:contributor>
  <dc:contributor>John Rasmus</dc:contributor>
  <dc:contributor>Keli Sun</dc:contributor>
  <dc:contributor>Qiming Li</dc:contributor>
  <dc:contributor>Timothy S. Collett</dc:contributor>
  <dc:contributor>David S. Goldberg</dc:contributor>
  <dc:creator>Anne E. Cook</dc:creator>
  <dc:date>2012</dc:date>
  <dc:description>We present new results and interpretations of the electricalanisotropy and reservoir architecture in gashydrate-bearingsands using logging data collected during the Gulf of MexicoGasHydrate Joint Industry Project Leg II. We focus specifically on sandreservoirs in Hole Alaminos Canyon 21 A (AC21-A), Hole Green Canyon 955 H (GC955-H) and Hole Walker Ridge 313 H (WR313-H). Using a new logging-while-drilling directional resistivity tool and a one-dimensional inversion developed by Schlumberger, we resolve the resistivity of the current flowing parallel to the bedding, &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&amp;#124;&lt;/sub&gt; and the resistivity of the current flowing perpendicular to the bedding, &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&lt;u&gt;&amp;#124;&lt;/u&gt;&lt;/sub&gt;. We find the sandreservoir in Hole AC21-A to be relatively isotropic, with &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&amp;#124;&lt;/sub&gt; and &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&lt;u&gt;&amp;#124;&lt;/u&gt;&lt;/sub&gt; values close to 2 &amp;Omega; m. In contrast, the gashydrate-bearingsandreservoirs in Holes GC955-H and WR313-H are highly anisotropic. In these reservoirs, &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&amp;#124;&lt;/sub&gt; is between 2 and 30 &amp;Omega; m, and &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;&lt;u&gt;&amp;#124;&lt;/u&gt;&lt;/sub&gt; is generally an order of magnitude higher. Using Schlumberger's WebMI models, we were able to replicate multiple resistivity measurements and determine the formation resistivity the gashydrate-bearingsandreservoir in Hole WR313-H. The results showed that gashydrate saturations within a single reservoir unit are highly variable. For example, the sand units in Hole WR313-H contain thin layers (on the order of 10-100 cm) with varying gashydrate saturations between 15 and 95%. Our combined modeling results clearly indicate that the gashydrate-bearingsandreservoirs in Holes GC955-H and WR313-H are highly anisotropic due to varying saturations of gashydrate forming in thin layers within larger sand units.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1016/j.marpetgeo.2011.09.003</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Elsevier</dc:publisher>
  <dc:title>Electrical anisotropy of gas hydrate-bearing sand reservoirs in the Gulf of Mexico</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>