<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "https://jats.nlm.nih.gov/nlm-dtd/publishing/3.0/journalpublishing3.dtd">
<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" specific-use="SMUR" dtd-version="3.0" xml:lang="en">
<front>
<journal-meta>
<journal-id journal-id-type="publisher">EGUsphere</journal-id>
<journal-title-group>
<journal-title>EGUsphere</journal-title>
<abbrev-journal-title abbrev-type="publisher">EGUsphere</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">EGUsphere</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub"></issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/egusphere-2024-3496</article-id>
<title-group>
<article-title>On the global geodynamic consequences of different phase boundary morphologies</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Morgan</surname>
<given-names>Gwynfor T.</given-names>
<ext-link>https://orcid.org/0009-0008-5802-6074</ext-link>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Davies</surname>
<given-names>J. Huw</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Myhill</surname>
<given-names>Robert</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Panton</surname>
<given-names>James</given-names>
<ext-link>https://orcid.org/0000-0002-1345-9406</ext-link>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>School of Earth and Environmental Sciences, Cardiff University, Park Place, Cardiff, Wales</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>School of Earth Sciences, University of Bristol, Bristol, England</addr-line>
</aff>
<pub-date pub-type="epub">
<day>25</day>
<month>11</month>
<year>2024</year>
</pub-date>
<volume>2024</volume>
<fpage>1</fpage>
<lpage>25</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2024 Gwynfor T. Morgan et al.</copyright-statement>
<copyright-year>2024</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://egusphere.copernicus.org/preprints/2024/egusphere-2024-3496/">This article is available from https://egusphere.copernicus.org/preprints/2024/egusphere-2024-3496/</self-uri>
<self-uri xlink:href="https://egusphere.copernicus.org/preprints/2024/egusphere-2024-3496/egusphere-2024-3496.pdf">The full text article is available as a PDF file from https://egusphere.copernicus.org/preprints/2024/egusphere-2024-3496/egusphere-2024-3496.pdf</self-uri>
<abstract>
<p>Phase transitions can influence mantle convection patterns, inhibiting or promoting vertical flow. One such transition is the ringwoodite-to-bridgmanite plus periclase transition, which has a negative Clapeyron slope and therefore reduces mantle flow between the upper and lower mantle. Interactions between different transitions and significant Clapeyron slope curvature can potentially result in complexities in mid-mantle geodynamics &amp;ndash; affecting the stagnation of slabs and free upward motion of plumes.&lt;/p&gt;
&lt;p&gt;Here, we consider two examples where non-linear phase boundary morphologies have been invoked to explain mid-mantle dynamics: (1) the intersection of the ringwoodite-to-bridgmanite plus periclase transition with the bridgmanite-to-akimotoite and ringwoodite-to-akimotoite plus periclase transitions, forming a &apos;branching&apos; morphology, and (2) the curvature of the garnet-to-bridgmanite transition. Using simple mantle convection or circulation simulations, we find that the dynamic impact of these example phase transitions are limited by either the uniqueness of thermodynamic state or the low magnitude of the phase buoyancy parameter respectively. Therefore it is unlikely that these phase boundary morphologies will, by themselves, prevent material exchange across the mid-mantle.</p>
</abstract>
<counts><page-count count="25"/></counts>
<funding-group>
<award-group id="gs1">
<funding-source>Natural Environment Research Council</funding-source>
<award-id>NE/T012633/1</award-id>
<award-id>NE/T012595/1</award-id>
</award-group>
</funding-group>
</article-meta>
</front>
<body/>
<back>
</back>
</article>