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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ANGEO</journal-id>
<journal-title-group>
<journal-title>Annales Geophysicae</journal-title>
<abbrev-journal-title abbrev-type="publisher">ANGEO</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Ann. Geophys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1432-0576</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/angeo-27-989-2009</article-id>
<title-group>
<article-title>A novel code for numerical 3-D MHD studies of CME expansion</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kleimann</surname>
<given-names>J.</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>Kopp</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fichtner</surname>
<given-names>H.</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>Grauer</surname>
<given-names>R.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Nordlys Observatoriet, Universitetet i Tromsø, 9037 Tromsø, Norway</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Institut für Experimentelle und Angewandte Physik, Christian-Albrechts-Universität zu Kiel, 24118 Kiel, Germany</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Institut für Theoretische Physik IV, Ruhr-Universität Bochum, 44780 Bochum, Germany</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Institut für Theoretische Physik I, Ruhr-Universität Bochum, 44780 Bochum, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>02</day>
<month>03</month>
<year>2009</year>
</pub-date>
<volume>27</volume>
<issue>3</issue>
<fpage>989</fpage>
<lpage>1004</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2009 J. Kleimann et al.</copyright-statement>
<copyright-year>2009</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://angeo.copernicus.org/articles/27/989/2009/angeo-27-989-2009.html">This article is available from https://angeo.copernicus.org/articles/27/989/2009/angeo-27-989-2009.html</self-uri>
<self-uri xlink:href="https://angeo.copernicus.org/articles/27/989/2009/angeo-27-989-2009.pdf">The full text article is available as a PDF file from https://angeo.copernicus.org/articles/27/989/2009/angeo-27-989-2009.pdf</self-uri>
<abstract>
<p>A recent third-order, essentially non-oscillatory central scheme to
  advance the equations of single-fluid magnetohydrodynamics (MHD) in
  time has been implemented into a new numerical code. This code
  operates on a 3-D Cartesian, non-staggered grid, and is able to
  handle shock-like gradients without producing spurious
  oscillations.

&lt;br&gt;&lt;br&gt;

  To demonstrate the suitability of our code for the simulation of
  coronal mass ejections (CMEs) and similar heliospheric transients,
  we present selected results from test cases and perform studies of
  the solar wind expansion during phases of minimum solar activity. We
  can demonstrate convergence of the system into a stable Parker-like
  steady state for both hydrodynamic and MHD winds. The model is
  subsequently applied to expansion studies of CME-like plasma
  bubbles, and their evolution is monitored until a stationary state
  similar to the initial one is achieved.
  In spite of the model&apos;s (current) simplicity, we can confirm the
  CME&apos;s nearly self-similar evolution close to the Sun, thus
  highlighting the importance of detailed modelling especially at
  small heliospheric radii.

&lt;br&gt;&lt;br&gt;

  Additionally, alternative methods to implement boundary
  conditions at the coronal base, as well as strategies to ensure a
  solenoidal magnetic field, are discussed and evaluated.</p>
</abstract>
<counts><page-count count="16"/></counts>
</article-meta>
</front>
<body/>
<back>
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