<?xml version="1.0"?>
<!DOCTYPE article
PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.4 20190208//EN"
       "JATS-journalpublishing1.dtd">
<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" article-type="research-article" dtd-version="1.4" xml:lang="en">
 <front>
  <journal-meta>
   <journal-id journal-id-type="publisher-id">Russian Journal of Earth Sciences</journal-id>
   <journal-title-group>
    <journal-title xml:lang="en">Russian Journal of Earth Sciences</journal-title>
    <trans-title-group xml:lang="ru">
     <trans-title>Russian Journal of Earth Sciences</trans-title>
    </trans-title-group>
   </journal-title-group>
   <issn publication-format="online">1681-1208</issn>
  </journal-meta>
  <article-meta>
   <article-id pub-id-type="publisher-id">47100</article-id>
   <article-categories>
    <subj-group subj-group-type="toc-heading" xml:lang="ru">
     <subject>ОРИГИНАЛЬНЫЕ СТАТЬИ</subject>
    </subj-group>
    <subj-group subj-group-type="toc-heading" xml:lang="en">
     <subject>ORIGINAL ARTICLES</subject>
    </subj-group>
    <subj-group>
     <subject>ОРИГИНАЛЬНЫЕ СТАТЬИ</subject>
    </subj-group>
   </article-categories>
   <title-group>
    <article-title xml:lang="en">Gravitational differentiation of liquid cores of planets and natural satellites</article-title>
    <trans-title-group xml:lang="ru">
     <trans-title>Gravitational differentiation of liquid cores of planets and natural satellites</trans-title>
    </trans-title-group>
   </title-group>
   <contrib-group content-type="authors">
    <contrib contrib-type="author">
     <name-alternatives>
      <name xml:lang="ru">
       <surname>Starchenko</surname>
       <given-names>S V</given-names>
      </name>
      <name xml:lang="en">
       <surname>Starchenko</surname>
       <given-names>S V</given-names>
      </name>
     </name-alternatives>
     <xref ref-type="aff" rid="aff-1"/>
    </contrib>
   </contrib-group>
   <aff-alternatives id="aff-1">
    <aff>
     <institution xml:lang="ru">Institute of Terrestrial Magnetism, Ionosphere, and Radiowave Propagation, Russian Academy of Sciences, Troitsk, Russia</institution>
     <country>ru</country>
    </aff>
    <aff>
     <institution xml:lang="en">Institute of Terrestrial Magnetism, Ionosphere, and Radiowave Propagation, Russian Academy of Sciences, Troitsk, Russia</institution>
     <country>ru</country>
    </aff>
   </aff-alternatives>
   <volume>5</volume>
   <issue>6</issue>
   <fpage>431</fpage>
   <lpage>438</lpage>
   <history>
    <date date-type="received" iso-8601-date="2021-11-10T23:23:04+03:00">
     <day>10</day>
     <month>11</month>
     <year>2021</year>
    </date>
   </history>
   <self-uri xlink:href="https://rjes.ru/en/nauka/article/47100/view">https://rjes.ru/en/nauka/article/47100/view</self-uri>
   <abstract xml:lang="ru">
    <p>Initial equations are obtained, similarity criteria are estimated and a project of simulation experiment is proposed for the gravitational differentiation of liquid cores of planets and natural satellites. It is assumed that, first, the liquid core in an adiabatic state without thermal convection and, second, the inner solid core grows during the crystallization of a heavy component from the liquid core in such a way that the buoyancy force acting on a lighter component is directed strictly along the radius. It is also assumed that the radial distribution of density in the liquid core does not change during the time interval considered. These three natural assumptions enable an analytical description of basic hydrostatic effects controlling slow growth of the solid core, gravitational stratification of the liquid core, and sources of related compositional convection. The similarity criteria of such convection are mostly the same as for thermal convection. Additional criteria are the concentration contrast ~1/10 in the Earth, the compressibility of the liquid core ~10%, and the thickness of a concentration boundary layer ~10-7 that, controlling the freezing-out of the liquid at the inner sphere, can give rise to asymmetry of the solid core. The excitation threshold of the compositional convection is much higher than a similar threshold for thermal convection, and the compositional convection itself can arise only at an intermediate stage of the gravitational differentiation of the core. Observed magnetic fields are largely due to compositional convection in the Earth's core and, probably, in deep interiors of Mercury. At the contemporary evolutionary stage of Venus' interiors, the intensity of compositional convection is most likely insufficient for the magnetic field excitation and it is undoubtedly too weak in the Mars' interiors.</p>
   </abstract>
   <trans-abstract xml:lang="en">
    <p>Initial equations are obtained, similarity criteria are estimated and a project of simulation experiment is proposed for the gravitational differentiation of liquid cores of planets and natural satellites. It is assumed that, first, the liquid core in an adiabatic state without thermal convection and, second, the inner solid core grows during the crystallization of a heavy component from the liquid core in such a way that the buoyancy force acting on a lighter component is directed strictly along the radius. It is also assumed that the radial distribution of density in the liquid core does not change during the time interval considered. These three natural assumptions enable an analytical description of basic hydrostatic effects controlling slow growth of the solid core, gravitational stratification of the liquid core, and sources of related compositional convection. The similarity criteria of such convection are mostly the same as for thermal convection. Additional criteria are the concentration contrast ~1/10 in the Earth, the compressibility of the liquid core ~10%, and the thickness of a concentration boundary layer ~10-7 that, controlling the freezing-out of the liquid at the inner sphere, can give rise to asymmetry of the solid core. The excitation threshold of the compositional convection is much higher than a similar threshold for thermal convection, and the compositional convection itself can arise only at an intermediate stage of the gravitational differentiation of the core. Observed magnetic fields are largely due to compositional convection in the Earth's core and, probably, in deep interiors of Mercury. At the contemporary evolutionary stage of Venus' interiors, the intensity of compositional convection is most likely insufficient for the magnetic field excitation and it is undoubtedly too weak in the Mars' interiors.</p>
   </trans-abstract>
   <kwd-group xml:lang="ru">
    <kwd>gravitational differentiation</kwd>
    <kwd>liquid cores</kwd>
    <kwd>simulation experiment</kwd>
    <kwd>gravitational stratification.</kwd>
   </kwd-group>
   <kwd-group xml:lang="en">
    <kwd>gravitational differentiation</kwd>
    <kwd>liquid cores</kwd>
    <kwd>simulation experiment</kwd>
    <kwd>gravitational stratification.</kwd>
   </kwd-group>
  </article-meta>
 </front>
 <body>
  <p></p>
 </body>
 <back>
  <ref-list>
   <ref id="B1">
    <label>1.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Braginsky, Geophys. Astrophys. Fluid Dynamics, v. 79, 1995., doi: 10.1080/03091929508228992</mixed-citation>
     <mixed-citation xml:lang="en">Braginsky, Geophys. Astrophys. Fluid Dynamics, v. 79, 1995., doi: 10.1080/03091929508228992</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B2">
    <label>2.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Busse, J. Fluid Mech., v. 44, 1970., doi: 10.1017/S0022112070001921</mixed-citation>
     <mixed-citation xml:lang="en">Busse, J. Fluid Mech., v. 44, 1970., doi: 10.1017/S0022112070001921</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B3">
    <label>3.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Dziewonski, Phys. Earth Planet. Inter., v. 25, 1981., doi: 10.1016/0031-92018190046-7</mixed-citation>
     <mixed-citation xml:lang="en">Dziewonski, Phys. Earth Planet. Inter., v. 25, 1981., doi: 10.1016/0031-92018190046-7</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B4">
    <label>4.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Glatzmaier, Contemporary Physics, v. 38, no. 4, 1997., doi: 10.1080/001075197182351</mixed-citation>
     <mixed-citation xml:lang="en">Glatzmaier, Contemporary Physics, v. 38, no. 4, 1997., doi: 10.1080/001075197182351</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B5">
    <label>5.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Jones, J. Fluid Mech., v. 405, 2000., doi: 10.1017/S0022112099007235</mixed-citation>
     <mixed-citation xml:lang="en">Jones, J. Fluid Mech., v. 405, 2000., doi: 10.1017/S0022112099007235</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B6">
    <label>6.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Kuskov, Astron. Vestnik, v. 32, no. 1, 1998.</mixed-citation>
     <mixed-citation xml:lang="en">Kuskov, Astron. Vestnik, v. 32, no. 1, 1998.</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B7">
    <label>7.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Lister, Phys. Earth Planet. Inter., v. 91, 1995., doi: 10.1016/0031-92019503042-U</mixed-citation>
     <mixed-citation xml:lang="en">Lister, Phys. Earth Planet. Inter., v. 91, 1995., doi: 10.1016/0031-92019503042-U</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B8">
    <label>8.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Loper, Geophys. J. R. Astron. Soc., v. 54, 1978.</mixed-citation>
     <mixed-citation xml:lang="en">Loper, Geophys. J. R. Astron. Soc., v. 54, 1978.</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B9">
    <label>9.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Starchenko, Phys. Earth Planet. Inter., v. 117, no. 1-4, 2000., doi: 10.1016/S0031-92019900099-0</mixed-citation>
     <mixed-citation xml:lang="en">Starchenko, Phys. Earth Planet. Inter., v. 117, no. 1-4, 2000., doi: 10.1016/S0031-92019900099-0</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B10">
    <label>10.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Starchenko, NATO Science Series II: Mathematics, Physics and Chemistry, v. 26, 2001.</mixed-citation>
     <mixed-citation xml:lang="en">Starchenko, NATO Science Series II: Mathematics, Physics and Chemistry, v. 26, 2001.</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B11">
    <label>11.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Starchenko, Icarus, v. 157, 2002., doi: 10.1006/icar.2002.6842</mixed-citation>
     <mixed-citation xml:lang="en">Starchenko, Icarus, v. 157, 2002., doi: 10.1006/icar.2002.6842</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B12">
    <label>12.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Stevenson, Icarus, v. 54, 1983., doi: 10.1016/0019-10358390241-5</mixed-citation>
     <mixed-citation xml:lang="en">Stevenson, Icarus, v. 54, 1983., doi: 10.1016/0019-10358390241-5</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B13">
    <label>13.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Sumita, Science, v. 286, 1999., doi: 10.1126/science.286.5444.1547</mixed-citation>
     <mixed-citation xml:lang="en">Sumita, Science, v. 286, 1999., doi: 10.1126/science.286.5444.1547</mixed-citation>
    </citation-alternatives>
   </ref>
   <ref id="B14">
    <label>14.</label>
    <citation-alternatives>
     <mixed-citation xml:lang="ru">Wijs, Nature, v. 392, 1998., doi: 10.1038/33905</mixed-citation>
     <mixed-citation xml:lang="en">Wijs, Nature, v. 392, 1998., doi: 10.1038/33905</mixed-citation>
    </citation-alternatives>
   </ref>
  </ref-list>
 </back>
</article>
