<?xml version='1.0' encoding='utf-8'?>
<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>W.J. Winters</dc:contributor>
  <dc:contributor>D.H. Mason</dc:contributor>
  <dc:creator>W.F. Waite</dc:creator>
  <dc:date>2004</dc:date>
  <dc:description>Bulk properties of gas hydrate-bearing sediment strongly depend on whether hydrate forms primarily in the pore fluid, becomes a load-bearing member of the sediment matrix, or cements sediment grains. Our compressional wave speed measurements through partially water-saturated, methane hydrate-bearing Ottawa sands suggest hydrate surrounds and cements sediment grains. The three Ottawa sand packs tested in the Gas Hydrate And Sediment Test Laboratory Instrument (GHASTLI) contain 38(1)% porosity, initially with distilled water saturating 58, 31, and 16% of that pore space, respectively. From the volume of methane gas produced during hydrate dissociation, we calculated the hydrate concentration in the pore space to be 70, 37, and 20% respectively. Based on these hydrate concentrations and our measured compressional wave speeds, we used a rock physics model to differentiate between potential pore-space hydrate distributions. Model results suggest methane hydrate cements unconsolidated sediment when forming in systems containing an abundant gas phase.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.2138/am-2004-8-906</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Mineralogical Society of  America</dc:publisher>
  <dc:title>Methane hydrate formation in partially water-saturated Ottawa sand</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>