Presentation Open Access
Schindler, Felix;
Zürner, Till;
Vogt, Tobias;
Eckert, Sven;
Schumacher, Jörg
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<identifier identifierType="DOI">10.14278/rodare.228</identifier>
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<creator>
<creatorName>Schindler, Felix</creatorName>
<givenName>Felix</givenName>
<familyName>Schindler</familyName>
<affiliation>Helmholtz-Zentrum Dresden-Rossendorf</affiliation>
</creator>
<creator>
<creatorName>Zürner, Till</creatorName>
<givenName>Till</givenName>
<familyName>Zürner</familyName>
<affiliation>Technische Universität Ilmenau</affiliation>
</creator>
<creator>
<creatorName>Vogt, Tobias</creatorName>
<givenName>Tobias</givenName>
<familyName>Vogt</familyName>
<nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0002-0022-5758</nameIdentifier>
<affiliation>Helmholtz-Zentrum Dresden-Rossendorf</affiliation>
</creator>
<creator>
<creatorName>Eckert, Sven</creatorName>
<givenName>Sven</givenName>
<familyName>Eckert</familyName>
<nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0003-1639-5417</nameIdentifier>
<affiliation>Helmholtz-Zentrum Dresden-Rossendorf</affiliation>
</creator>
<creator>
<creatorName>Schumacher, Jörg</creatorName>
<givenName>Jörg</givenName>
<familyName>Schumacher</familyName>
<affiliation>Technische Universität Ilmenau</affiliation>
</creator>
</creators>
<titles>
<title>Low Prandtl Number Rayleigh-Bénard Convection in a Vertical Magnetic Field</title>
</titles>
<publisher>Rodare</publisher>
<publicationYear>2019</publicationYear>
<subjects>
<subject>Rayleigh-Bénard-Convection</subject>
<subject>Magnetohydrodynamic</subject>
<subject>low Prandtl Number</subject>
<subject>liquid metal</subject>
<subject>Ultrasound velocimetry</subject>
</subjects>
<dates>
<date dateType="Issued">2019-07-01</date>
</dates>
<language>en</language>
<resourceType resourceTypeGeneral="Text">Presentation</resourceType>
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<relatedIdentifier relatedIdentifierType="DOI" relationType="IsCitedBy">10.1103/physreve.62.r4520</relatedIdentifier>
<relatedIdentifier relatedIdentifierType="DOI" relationType="IsCitedBy">10.1017/jfm.2018.479</relatedIdentifier>
<relatedIdentifier relatedIdentifierType="DOI" relationType="IsCitedBy">10.1073/pnas.1417741112</relatedIdentifier>
<relatedIdentifier relatedIdentifierType="DOI" relationType="IsSupplementedBy">10.1017/jfm.2019.556</relatedIdentifier>
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<version>1.0</version>
<rightsList>
<rights rightsURI="https://creativecommons.org/licenses/by/4.0/legalcode">Creative Commons Attribution 4.0 International</rights>
<rights rightsURI="info:eu-repo/semantics/openAccess">Open Access</rights>
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<descriptions>
<description descriptionType="Abstract"><p>Lecture (Conference)</p>
<p>11th PAMIR International Conference- Fundamental and Applied MHD July 1-5, 2019, Reims, EVEM France</p>
<p>We are investigating turbulent Rayleigh-B&eacute;nard convection in liquid metal under the<br>
influence of a vertical magnetic field. Utilizing a combination of thermocouple (TC) and<br>
ultrasound-Doppler-velocimetry (UDV) measurements gives us the possibility to directly<br>
determine the temperature and velocity field, respectively. Further this gives us the<br>
possibility to observe changes in the large-scale flow structure.<br>
By applying magnetic fields to the liquid metal convection, we quantified changes of heat<br>
and momentum transport in the liquid metal alloy GaInSn. The experimental results of our<br>
setup agree well with theory findings and direct numerical simulations of the dynamics in<br>
our convection cell. The requirement of large computing power at these parameters makes<br>
it hard to simulate long-term dynamics with time scales from minutes to several hours. Thus<br>
to investigate slow developing dynamics like sloshing, rotation, or deformation of the large-<br>
scale flow structure model experiments are indispensable.<br>
We demonstrate the suppression of the convective flow by a vertical magnetic field in a<br>
cylindrical cell of aspect ratio 1. In this setup Rayleigh numbers up to 6&middot;107 are<br>
investigated. The flow structure at low Hartmann numbers is a single roll large scale<br>
circulation (LSC). Increasing the Hartmann number leads to a transition from the single-roll<br>
LSC into a cell structure. An even stronger magnetic field supresses the flow in the center<br>
of the cell completely and expels the flow to the side walls.<br>
Even above the critical Hartmann numbers corresponding to the Chandrasekhar limit for<br>
the onset of magnetoconvection in a fluid layer without lateral boundaries we still observe<br>
remarkable flows near the side walls. The destabilising effect of the non-conducting side<br>
walls was predicted by theory and simulations, and is here for the first time experimentally<br>
confirmed.</p>
<p>&nbsp;</p></description>
<description descriptionType="Other">Support by Deutsche Forschungsgemeinschaft with grants VO 2332/1-1 and SCHU 1410/29-1</description>
<description descriptionType="Other">{"references": ["10.1017/S0022112096004491", "10.1103/physreve.62.r4520", "10.1017/jfm.2018.479", "10.1073/pnas.1417741112", "10.1017/jfm.2019.556", "https://www.hzdr.de/publications/Publ-28698"]}</description>
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