<?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>L.A. Stern</dc:contributor>
  <dc:creator>S. H. Kirby</dc:creator>
  <dc:date>1993</dc:date>
  <dc:description>&lt;p&gt;This paper is a review of some of the rich and varied interactions between non-hydrostatic stress and phase transformations or mineral reactions, drawn mainly from results of experiments done on mineral single crystals in our laboratory or our co-authors. The state of stress and inelastic deformation can enter explicitly into the equilibrium phase relations and kinetics of mineral reactions. Alternatively, phase transformations can have prominent effects on theology and on the nature of inelastic deformation. Our examples represent five types of structural phase changes, each of which is distinguished by particular mechanical effects. In increasing structural complexity, these include: (1)&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;displacive phase transformations&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;involving no bond-breaking, which may produce anomalous brittle behavior. A primary example is the&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;a&lt;/i&gt;-&lt;i&gt;β&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;quartz transition which shows anomalously low fracture strength and tertiary creep behavior near the transition temperature; (2)&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;martensitic-like transformations&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;involving transformation strains dominated by shear deformation. Examples include the orthoenstatite → clinoenstatite and&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;span class="math"&gt;&lt;span id="MathJax-Element-1-Frame" class="MathJax_SVG" data-mathml="&lt;math xmlns=&amp;quot;http://www.w3.org/1998/Math/MathML&amp;quot;&gt;&lt;mtext&gt;w&lt;/mtext&gt;&lt;mtext&gt;u&lt;/mtext&gt;&lt;mtext&gt;&amp;amp;#x308;&lt;/mtext&gt;&lt;mtext&gt;rtzite&lt;/mtext&gt;&lt;mtext&gt;&amp;amp;#x2192;&lt;/mtext&gt;&lt;mtext&gt;sphalerite&lt;/mtext&gt;&lt;/math&gt;"&gt;&lt;span class="MJX_Assistive_MathML"&gt;würtzite→sphalerite&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;transformations; (3)&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;coherent exsolution&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;or precipitation of a mineral solute from a supersaturated solid-solution, with anisotropy of precipitation and creep rates produced under nonhydrostatic stress. Examples include exsolution of corundum from MgO ·&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;n&lt;/i&gt;Al&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;spinels and Ca-clinopyroxene from orthopyroxene; (4)&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;order-disorder&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;transformations that are believed to cause anomalous plastic yield strengthening, such as&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;MgO&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;-&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;nAl&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt;&lt;i&gt;O&lt;/i&gt;&lt;sub&gt;3&lt;/sub&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;spinels; and (5)&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;i&gt;near-surface devolatilization&lt;/i&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;of hydrous silicate single-crystals that produces a fundamental brittleness thought to be connected with dehydration at microcracks at temperatures well below nominal macroscopic dehydration temperatures.&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1016/0191-8141(93)90165-7</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Elsevier</dc:publisher>
  <dc:title>Experimental dynamic metamorphism of mineral single crystals</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>