<?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">ESDD</journal-id>
<journal-title-group>
<journal-title>Earth System Dynamics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ESDD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam. Discuss.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">2190-4995</issn>
<publisher><publisher-name></publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/esd-2023-21</article-id>
<title-group>
<article-title>Gaia: Complex systems prediction for time to adapt to climate shocks</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hunt</surname>
<given-names>Allen G.</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>Sahimi</surname>
<given-names>Muhammad</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>Faybishenko</surname>
<given-names>Boris</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Egli</surname>
<given-names>Markus</given-names>
<ext-link>https://orcid.org/0000-0002-1528-3440</ext-link>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kabala</surname>
<given-names>Zbigniew J.</given-names>
<ext-link>https://orcid.org/0000-0002-3502-7081</ext-link>
</name>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ghanbarian</surname>
<given-names>Behzad</given-names>
</name>
<xref ref-type="aff" rid="aff6">
<sup>6</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yu</surname>
<given-names>Fang</given-names>
</name>
<xref ref-type="aff" rid="aff7">
<sup>7</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Department of Physics, Wright State University, 3640 Colonel Glenn Highway, Dayton, OH 45435, USA</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Department of Chemical Engineering and Materials Science, University of Southern California, Los Angeles, CA, USA</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Energy Geosciences Division, Lawrence Berkeley National Laboratory, University of California, Berkeley, CA 94720, USA</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Department of Geography, University of Zurich, Winterthurerstrasse 190, 8057 Zurich, Switzerland</addr-line>
</aff>
<aff id="aff5">
<label>5</label>
<addr-line>Department of Civil &amp; Environmental Engineering, Duke University, Durham, NC 27708, USA</addr-line>
</aff>
<aff id="aff6">
<label>6</label>
<addr-line>Porous Media Research Lab, Department of Geology, Kansas State University, Manhattan, KS 66506, USA</addr-line>
</aff>
<aff id="aff7">
<label>7</label>
<addr-line>Department of Forestry, Beihua University, 3999 Binjiangdong Road, Jilin, China, 132013</addr-line>
</aff>
<pub-date pub-type="epub">
<day>27</day>
<month>09</month>
<year>2023</year>
</pub-date>
<volume>2023</volume>
<fpage>1</fpage>
<lpage>13</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2023 Allen G. Hunt et al.</copyright-statement>
<copyright-year>2023</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://esd.copernicus.org/preprints/esd-2023-21/">This article is available from https://esd.copernicus.org/preprints/esd-2023-21/</self-uri>
<self-uri xlink:href="https://esd.copernicus.org/preprints/esd-2023-21/esd-2023-21.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/preprints/esd-2023-21/esd-2023-21.pdf</self-uri>
<abstract>
<p>&lt;p&gt;Earth&amp;rsquo;s climate has undergone significant fluctuations in the geologic past. We focus on the glacial episodes that followed the major waves of invasion of land plants. Twice in Earth&amp;rsquo;s history the impacts of land plant innovations on the atmosphere through increased CO&lt;sub&gt;2&lt;/sub&gt; drawdown have precipitated sufficient cooling to produce ice ages. Each time, however, adaptation of soil ecosystems eventually helped re-establish apparent steady-state conditions, i.e., new equilibrium temperature and atmospheric CO&lt;sub&gt;2&lt;/sub&gt; content, ending each of the glacial episodes. In each case, the time interval between the initial innovation and the emergence from the glacial episode was approximately 60 Myr. The consistency of the time scale of the response invites an explanation in terms of a universal rate of dispersal of genetic information that encapsulates the biogeochemical cycle of cellulose production and decay. In this paper, we postulate that the long time for adaptation is a consequence of the time required for the spread of an entire clade though the soil to continental scale. Although 60 Myr appears to be a long time, it is very short compared to the time required for diffusion to transport even molecules like HCO&lt;sub&gt;3&lt;sup&gt;&amp;minus;&lt;/sup&gt;&lt;/sub&gt; or sugar through the soil over a continental distance of 5,000 km, which is between 10&lt;sup&gt;14&lt;/sup&gt; and 10&lt;sup&gt;16&lt;/sup&gt; years for solutes with such soil diffusion constants in the range 10&lt;sup&gt;&amp;minus;11&lt;/sup&gt; m&lt;sup&gt;2 &lt;/sup&gt;s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. Horizontal solute transport through heterogeneous media by advection might be considered as a dispersal mechanism, but is also known to require enormous time scales (ca. 150 Myr for 500 m). We also seek a relevant mechanism in the known scaling of plant and fungal growth rates as a function of time, which can facilitate as well the movement of bacteria, and predicted these rates theoretically on the basis of the universal optimal 2D paths tortuosity from percolation. Comparison with actual data pairs (7,000) for plant and fungal growth rates were used to verify these predictions over 13 orders of magnitude of time, from about one minute to 100 kyr; extrapolation over less than three additional orders of time yields a continental-scale transport time of 80 Myr. We now interpret this prediction in terms of Margulis&amp;rsquo; understanding of emergent behavior of coupled (soil and plant) ecosystems responding to climate shocks induced by plant innovations.&lt;/p&gt;</p>
</abstract>
<counts><page-count count="13"/></counts>
</article-meta>
</front>
<body/>
<back>
</back>
</article>