<?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>H.-R. Wenk</dc:contributor>
  <dc:contributor>W.B. Durham</dc:contributor>
  <dc:contributor>L.A. Stern</dc:contributor>
  <dc:contributor>S. H. Kirby</dc:contributor>
  <dc:creator>K. Bennett</dc:creator>
  <dc:date>1997</dc:date>
  <dc:description>&lt;p&gt;The preferred crystallographic orientation developed during the ice I &amp;larr; II transformation and during the plastic flow of ice II was measured in polycrystalline deuterium oxide (D&lt;sub&gt;2&lt;/sub&gt;O) specimens using low-temperature neutron diffraction. Samples partially transformed from ice I to II under a non-hydrostatic stress developed a preferred crystallographic orientation in the ice II. Samples of pure ice II transformed from ice I under a hydrostatic stress and then when compressed axially, developed a strong preferred orientation of compression axes parallel to (10&lt;span class="overline"&gt;1&lt;/span&gt;0). A match to the observed preferred orientation using the viscoplastic self-consistent theory was obtained only when (10&lt;span class="overline"&gt;1&lt;/span&gt;0) [0001] was taken as the predominant slip system in ice II.&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1080/01418619708209983</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Taylor &amp; Francis</dc:publisher>
  <dc:title>Preferred crystallographic orientation in the ice I ← II transformation and the flow of ice II</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>