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	<title>ISTerre - Institut des Sciences de la Terre</title>
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<item xml:lang="en">
		<title>ERC project THEIA</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6081.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6081.html</guid>
		<dc:date>2022-02-14T07:38:21Z</dc:date>
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		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, J&#233;r&#233;mie VIDAL, Max SOLAZZO</dc:creator>



		<description>&lt;p&gt;Experiments&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/" rel="directory"&gt;ERC project THEIA&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;CENTER&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;Project&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/members.html&#034;&gt;About Us&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/publications.html&#034;&gt;Publications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/communications.html&#034;&gt;Communications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/numerics.html&#034;&gt;Numerics&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/experiments.html&#034;&gt;&lt;u&gt;Experiments&lt;/u&gt;&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/gallery.html&#034;&gt;Gallery&lt;/a&gt;&lt;/strong&gt; | &lt;/CENTER&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;Why building experiments?&lt;/h3&gt;
&lt;p&gt;In the frame of the ERC project THEIA, we aim at combining theory, numerics and experiments. They are indeed complementary to investigate the coupling between a solid boundary and a fluid flow, such as the one at the seafloor or at the Core-Mantle Boundary (CMB) :&lt;/p&gt;
&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Theory&lt;/strong&gt; gives physical insights and can directly probe the relevant regime of weak diffusivities and large magnetic fields. But it remains limited to laminar or weak turbulence, and dynamo studies remain a challenge.&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Numerics&lt;/strong&gt; can handle spherical-like geometries, with all the physical ingredients, giving the flow in the whole volume. But it is limited to laminar or weak turbulence, and diffusive effects are over-estimated. Moreover, it remains challenging to include topographic effects in simulations.&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Experiments&lt;/strong&gt; can easily probe the turbulent regime, a key ingredient which remains intractable with theory or numerics. It can also tackle any kind of topography. But the weakly diffusive magnetic effects or the spherical-like geometry remain out-of-reach.&lt;/li&gt;&lt;/ul&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;Two experiments&lt;/h3&gt;
&lt;p&gt;To investigate turbulent boundary couplings in presence of rotation, density variations and topography, we are developing an experimental setup at two different scales: a small, but versatile and easy to modify, setup called mini-THEIA, and a large-scale experiment, less flexible but capable of probing other regimes (e.g. waves interactions):&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;div class='spip_document_11731 spip_document spip_documents spip_document_image spip_documents_left spip_document_left'&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/jpg/th2en0311-003.jpg' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/jpeg&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L125xH180/th2en0311-003-65bab-e2b36.jpg?1789506402' width='125' height='180' alt='' /&gt;&lt;/a&gt;
&lt;/figure&gt;
&lt;/div&gt; &lt;p&gt;&lt;strong&gt;&lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/th2en0211-01_2_.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Mini-THEIA&lt;/a&gt;&lt;/strong&gt; will be able to tackle various experiments in rotating flows. It will allow a &lt;strong&gt;continuous filling and draining&lt;/strong&gt; of the experimental tank, while in rotation (notably to avoid the mixing due to the fluid spin-up). Typical planned experiments are&lt;/p&gt;
&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Linear spin-up&lt;/strong&gt; (or spin-down) of a stratified fluid in presence of topography, in the continuity of &lt;a href=&#034;https://aip.scitation.org/doi/full/10.1063/1.5051111&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Burmann &amp; Noir (2018)&lt;/a&gt;.&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Coupling of floating bodies&lt;/strong&gt; (in order to get rid off unwanted solid friction)&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Filling box experiments&lt;/strong&gt;, with plume injections and draining while in rotation (collaboration with &lt;a href=&#034;https://www.isterre.fr/annuaire/member-web-pages/renaud-deguen/&#034;&gt;Prof. Renaud Deguen&lt;/a&gt;)&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Slichter modes&lt;/strong&gt; measurements, with a rotating flow&lt;/li&gt;&lt;li&gt; &lt;strong&gt;Libration Driven square instabilities&lt;/strong&gt; (LDSI) will be excited and compared with theory (collaboration with &lt;a href=&#034;https://sites.google.com/view/jvidalhome&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;J&#233;r&#233;mie Vidal&lt;/a&gt;)&lt;/li&gt;&lt;/ul&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;BR&gt;&lt;BR&gt;&lt;/p&gt;
&lt;div class='spip_document_11707 spip_document spip_documents spip_document_image spip_documents_left spip_document_left'&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/png/theia.png' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/png&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L415xH200/theia-e6d60-ce975.png?1789506402' width='415' height='200' alt='' /&gt;&lt;/a&gt;
&lt;/figure&gt;
&lt;/div&gt; &lt;p&gt;&lt;strong&gt;&lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/projet_theia_0521-001b_1_.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;The large-scale experiment THEIA&lt;/a&gt;&lt;/strong&gt; requires severe modifications of the experimental room to host the &lt;strong&gt;rotating 18T experiment&lt;/strong&gt; of salty water. This long-term goal experiment will allow to study the &lt;strong&gt;boundary wave drag&lt;/strong&gt; when rotation, topography and &lt;strong&gt;turbulence&lt;/strong&gt; are simultaneously present. It is still under development, and mini-THEIA will help to design it.&lt;/p&gt;&lt;/div&gt;
		
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	</item>
<item xml:lang="en">
		<title>ERC project THEIA</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6080.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6080.html</guid>
		<dc:date>2022-02-10T09:07:26Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, J&#233;r&#233;mie VIDAL, Max SOLAZZO</dc:creator>



		<description>&lt;p&gt;Numerics&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/" rel="directory"&gt;ERC project THEIA&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;CENTER&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;Project&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/members.html&#034;&gt;About Us&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/publications.html&#034;&gt;Publications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/communications.html&#034;&gt;Communications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/numerics.html&#034;&gt;&lt;u&gt;Numerics&lt;/u&gt;&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/experiments.html&#034;&gt;Experiments&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/gallery.html&#034;&gt;Gallery&lt;/a&gt;&lt;/strong&gt; | &lt;/CENTER&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;div class='spip_document_11703 spip_document spip_documents spip_document_image spip_documents_left spip_document_left'&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/png/tocco.png' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/png&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L303xH170/tocco-6211a-e2187.png?1789506402' width='303' height='170' alt='' /&gt;&lt;/a&gt;
&lt;/figure&gt;
&lt;/div&gt;
&lt;p&gt;In the frame of the &lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;ERC project THEIA&lt;/a&gt;, we develop from scratch new codes (e.g. &lt;a href=&#034;https://gitlab.com/monvilre/tocco&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;ToCCo&lt;/a&gt;), or we modify existing efficient codes (e.g. &lt;a href=&#034;https://nschaeff.bitbucket.io/xshells/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;XSHELLS&lt;/a&gt;) to investigate small and large scale topographic effects. We detail below some of the codes currently developed and used in the project:&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;1.&lt;/strong&gt; &lt;strong&gt;&lt;a href=&#034;https://gitlab.com/monvilre/tocco&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;ToCCo&lt;/a&gt;&lt;/strong&gt; (Topographic Coupling at Core-Mantle interface), developed by &lt;a href=&#034;https://monvilre.gitlab.io/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;R. Monville&lt;/a&gt;, combines &lt;a href=&#034;https://www.sympy.org/en/index.html&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;symbolic&lt;/a&gt; and &lt;a href=&#034;http://mpmath.org/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;arbitrary-precision numerical&lt;/a&gt; calculations in a local Cartesian box in order to calculate the Boussinesq magneto-hydrodynamic laminar flow along one or two (possibly conducting) solid domains, forced by rotation, topographic, buoyancy and magnetic effects (providing the total boundary stress from pressure, viscous and electromagnetic forces).&lt;br class='autobr' /&gt;
&lt;strong&gt;Associated ERC project publications&lt;/strong&gt;: Monville, C&#233;bron, Jault (2022, in prep.)&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;2.&lt;/strong&gt; &lt;strong&gt;&lt;a href=&#034;https://bitbucket.org/vidalje/shine/src&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;SHINE&lt;/a&gt;&lt;/strong&gt; (Solver for Hydromagnetic INviscid modes in Ellipsoids), developed by &lt;a href=&#034;https://sites.google.com/view/jvidalhome/numerics?authuser=0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;J. Vidal&lt;/a&gt; computes the diffusionless hydromagnetic eigenmodes of either Boussinesq or fully compressible fluids enclosed in co-rotating triaxial ellipsoids. The code handles polynomial perturbations of unprecedented spatial complexity.&lt;br class='autobr' /&gt;
&lt;strong&gt;Associated ERC project publications&lt;/strong&gt;: &lt;a href=&#034;https://royalsocietypublishing.org/doi/10.1098/rspa.2020.0131&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Vidal &amp; C&#233;bron (2020, PRSA)&lt;/a&gt;, &lt;a href=&#034;https://asa.scitation.org/doi/10.1121/10.0005909&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Vidal &amp; C&#233;bron (2021, JASA)&lt;/a&gt;, &lt;a href=&#034;https://royalsocietypublishing.org/doi/10.1098/rspa.2021.0252&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Vidal &amp; C&#233;bron (2021, PRSA)&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;3.&lt;/strong&gt; &lt;strong&gt;&lt;a href=&#034;https://bitbucket.org/vidalje/swan/src&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;SWAN&lt;/a&gt;&lt;/strong&gt; (Short-Wavelength stability ANalysis), developed by &lt;a href=&#034;https://sites.google.com/view/jvidalhome/numerics?authuser=0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;J. Vidal&lt;/a&gt;, probes the linear hydromagnetic stability of generic Boussinesq basic states, by considering short-wavelength perturbations (&lt;a href=&#034;https://doi.org/10.1063/1.858153&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Lifschitz &amp; Hameiri, 1991&lt;/a&gt;). This code gives sufficient conditions for local diffusionless instability.&lt;br class='autobr' /&gt;
&lt;strong&gt;Associated ERC project publications&lt;/strong&gt;: Vidal &amp; C&#233;bron (2022, in prep.)&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;4.&lt;/strong&gt; &lt;strong&gt;&lt;a href=&#034;https://sites.google.com/view/jvidalhome/tools?authuser=0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;SIREN&lt;/a&gt;&lt;/strong&gt; (Stability with IneRtial eigENmodes), developed by &lt;a href=&#034;https://sites.google.com/view/jvidalhome/numerics?authuser=0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;J. Vidal&lt;/a&gt;, probes the linear stability of arbitrary basic flows of uniform vorticity, forced by orbital forcings and enclosed within rigid ellipsoids. The code handles polynomial perturbations of unprecedented spatial complexity in the ellipsoid. &lt;br class='autobr' /&gt;
&lt;strong&gt;Associated ERC project publications&lt;/strong&gt;: Vidal &amp; C&#233;bron (2022, in prep.)&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;5.&lt;/strong&gt; &lt;strong&gt;&lt;a href=&#034;https://nschaeff.bitbucket.io/xshells/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;XSHELLS&lt;/a&gt;&lt;/strong&gt;, developed by &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/nathanael-schaeffer/&#034;&gt;N. Schaeffer&lt;/a&gt;, performs spectral direct numerical simulations (DNS) in spherical geometries using sphericl harmonics.&lt;br class='autobr' /&gt;
&lt;strong&gt;Associated ERC project publications&lt;/strong&gt;: &lt;a href=&#034;https://doi.org/10.1017/jfm.2021.220&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;C&#233;bron et al. (2021)&lt;/a&gt;&lt;/p&gt;&lt;/div&gt;
		
		</content:encoded>


		

	</item>
<item xml:lang="en">
		<title>ERC project THEIA</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6079.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6079.html</guid>
		<dc:date>2022-02-10T09:01:26Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, J&#233;r&#233;mie VIDAL, Max SOLAZZO</dc:creator>



		<description>&lt;p&gt;Communications&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/" rel="directory"&gt;ERC project THEIA&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;CENTER&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;Project&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/members.html&#034;&gt;About Us&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/publications.html&#034;&gt;Publications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/communications.html&#034;&gt;&lt;u&gt;Communications&lt;/u&gt;&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/numerics.html&#034;&gt;Numerics&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/experiments.html&#034;&gt;Experiments&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/gallery.html&#034;&gt;Gallery&lt;/a&gt;&lt;/strong&gt; | &lt;/CENTER&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2025 -&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;27.&lt;/strong&gt; Personnettaz P., Meresse A., C&#233;bron D., Scha&#235;ffer N., &lt;a href=&#034;https://airdrive.eventsair.com/eventsairwesteuprod/production-abbey-public/5cc629198f9c4c22a230a24a87d8fa06&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Laminar to turbulent transition in librating spheres&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;2nd European Fluid Dynamics Conference (EFDC2)&lt;/i&gt;, Dublin (Ireland), 26-29 August 2025.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;26.&lt;/strong&gt; C&#233;bron D. , &lt;a href=&#034;https://www.ipgp.fr/actus-et-agenda/agenda/seminaires/tba/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Unravelling the dynamics of non-spherical planetary cores&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;Th&#232;me Int&#233;rieurs de la Terre et des plan&#232;tes&lt;/i&gt;. Invited seminar at IPG Paris, France, April 03, 2025.&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2024 -&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;25.&lt;/strong&gt; Personnettaz P., Scha&#235;ffer N., C&#233;bron D., Mandea M., &lt;a href=&#034;http://nonlineaire.univ-lille.fr/SNL/media/2024/resumes/personnp/main.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Fluid response to the inner core's translational oscillations&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;Rencontres du Non-Lin&#233;aire&lt;/i&gt;, Paris, March 19-20, 2024.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;24.&lt;/strong&gt; Monville R., C&#233;bron D. &amp; Jault D. , &lt;a href=&#034;https://indico.math.cnrs.fr/event/11117/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic effects in planetary magneto-hydrodynamic &#64258;ows&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;Rencontres du Non-Lin&#233;aire&lt;/i&gt;, Paris, March 19-20, 2024. &lt;a href=&#034;https://sdrive.cnrs.fr/s/T2peBpPriGrN76A&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;23.&lt;/strong&gt; Vidal J. , &lt;a href=&#034;https://indico.math.cnrs.fr/event/11117/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Inertia-gravity waves in geophysical vortices&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;Seminar, Institut de Math&#233;matiques de Bourgogne&lt;/i&gt;, Universit&#233; de Bourgogne (France), February 20, 2024. &lt;a href=&#034;https://sdrive.cnrs.fr/s/GiH7Y7Md3wzZHXG&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;22.&lt;/strong&gt; Vidal J. , &lt;a href=&#034;https://www-fourier.univ-grenoble-alpes.fr/~lacavec/MathsInFluids/Programme2324.html&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Ondes d'inertie-gravit&#233; dans un fluide confin&#233;, applications g&#233;ophysiques&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;Seminar &#034;MathsInFluids&#034; - UMPA&lt;/i&gt;, ENS Lyon (France), February 2, 2024. &lt;a href=&#034;https://sdrive.cnrs.fr/s/ibJ6pbHYPmF8dgX&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;21.&lt;/strong&gt; Personnettaz P., Monville R., Scha&#235;ffer N., C&#233;bron D., Mandea M., &lt;a href=&#034;https://efdc1.de/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Beyond spherical boundaries in deep fluid layers of planets&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;1st European Fluid Dynamics Conference (EFDC1)&lt;/i&gt;, Aachen (Germany), September 16-20, 2024.&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2023 -&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;20.&lt;/strong&gt; Vidal J. , &lt;a href=&#034;https://asp2023.sciencesconf.org/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Inertia-gravity waves in geophysical vortices&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;&#034;Spectral and Resonance Problems for Imaging, Seismology and Materials Science&#034;&lt;/i&gt;, Universit&#233; de Reims Champagne-Ardenne (France), November 20-24, 2023. &lt;a href=&#034;https://sdrive.cnrs.fr/s/T2peBpPriGrN76A&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;19.&lt;/strong&gt; C&#233;bron D. , &lt;a href=&#034;https://adrienmorison.com/workshop-2023-10/program/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Simulations of non-spherical liquid cores of planets&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;Beyond Boussinesq for Astrophysical and Geophysical fluids: Numerical tools and experiments of the future&lt;/i&gt;. ENS Lyon, France, October 19, 2023.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;18.&lt;/strong&gt; Personnettaz P., C&#233;bron D., Scha&#235;ffer N., Mandea M., &lt;a href=&#034;https://cnes-jc2.fr/jc2-2023/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Dissipation mechanisms of the inner core's translational oscillations&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;Journ&#233;es CNES (JC2) 2023&lt;/i&gt;, Toulouse (France), October 11-13, 2023.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;17.&lt;/strong&gt; Personnettaz P., C&#233;bron D., Scha&#235;ffer N., Mandea M., &lt;a href=&#034;https://gafdem.sciencesconf.org/data/pages/program_gafdem_2023_LAST.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Modeling non-spherical e&#64256;ects with parametrized boundary conditions&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;GAFDEM: Geophysical Astrophysical Fluid Dynamics: Experiments and models&lt;/i&gt;, Nice (France), September 11-15, 2023.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;16.&lt;/strong&gt; Monville R., Vidal J., C&#233;bron D. &amp; Schaeffer N., &lt;a href=&#034;https://gfzpublic.gfz-potsdam.de/pubman/faces/ViewItemOverviewPage.jsp?itemId=item_5016637&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic coupling at the core mantle boundary&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;28th General Assembly of The IUGG&lt;/i&gt;, Berlin (Germany), July 11-20 2023. &lt;a href=&#034;https://monvilre.gitlab.io/pdf/IUGG23-Oral.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;15.&lt;/strong&gt; Monville R., Vidal J., C&#233;bron D. &amp; Schaeffer N., &lt;a href=&#034;https://gfzpublic.gfz-potsdam.de/pubman/faces/ViewItemOverviewPage.jsp?itemId=item_5016641&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Generation of planetary core zonal flows by orbital forcings or fingering convection&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;28th General Assembly of The IUGG&lt;/i&gt;, Berlin (Germany), July 11-20 2023. &lt;a href=&#034;https://drive.google.com/file/d/1M-7Y3JjgUD_vlq577jPtU-HwCtwT05gD/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;14.&lt;/strong&gt; C&#233;bron D., Monville R., Vidal J., Sauret A. &amp; Schaeffer N., &lt;a href=&#034;https://gfzpublic.gfz-potsdam.de/pubman/faces/ViewItemOverviewPage.jsp?itemId=item_5016643&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Generation of planetary core zonal flows by orbital forcings or fingering convection&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;28th General Assembly of The IUGG&lt;/i&gt;, Berlin (Germany), July 11-20 2023. &lt;a href=&#034;https://drive.google.com/file/d/1mfQMwpYgqWpPOJ55C6ng5c3uQW7Tqz15/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;13.&lt;/strong&gt; Vidal J. &amp; C&#233;bron D., &lt;a href=&#034;https://gfzpublic.gfz-potsdam.de/pubman/faces/ViewItemOverviewPage.jsp?itemId=item_5016638&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Precession-driven flows and turbulence in planetary liquid cores&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;28th General Assembly of The IUGG&lt;/i&gt;, Berlin (Germany), July 11-20 2023. &lt;a href=&#034;https://drive.google.com/file/d/18JhC-mRyh7iBLirZvWZJFoAFscvbDB-9/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;12.&lt;/strong&gt; Vidal J. &amp; C&#233;bron D., &lt;a href=&#034;http://nonlineaire.univ-lille1.fr/SNL/media/2023/resumes/vidalje/rnl2023_vidal.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Asymptotic models of rotating flows in stress-free ellipsoids&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;26eme Rencontre du Non Lin&#233;aire&lt;/i&gt;, Paris (France), March 28-30 2023. &lt;a href=&#034;https://drive.google.com/file/d/1SDeNH6KnmepPgdlgtuMPTFCWd5o485D8/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2022 -&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;11.&lt;/strong&gt; Monville R., C&#233;bron D., Schaeffer N., &lt;a href=&#034;https://agu.confex.com/agu/fm22/meetingapp.cgi/Paper/1104245&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic Effects in Magnetized and Stratified Fluid Cores&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;AGU Fall Meeting&lt;/i&gt;, Chicago (USA), December 12-16 2022.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;10.&lt;/strong&gt; Monville R., Vidal J., C&#233;bron D., Schaeffer N., &lt;a href=&#034;https://agu.confex.com/agu/fm22/meetingapp.cgi/Paper/1103042&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Rotating Double-Diffusive Convection: Flows and Dynamos in Stably Stratified Deep Layers of Planets&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;AGU Fall Meeting&lt;/i&gt;, Chicago (USA), December 12-16 2022. &lt;a href=&#034;https://drive.google.com/file/d/1M-7Y3JjgUD_vlq577jPtU-HwCtwT05gD/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;9.&lt;/strong&gt; Monville R., C&#233;bron D., Jault D., &lt;a href=&#034;https://monvilre.gitlab.io/publications.html&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic effects in magnetized and stratified fluid cores&lt;/a&gt;, &lt;br class='autobr' /&gt;
&lt;i&gt;17th Symposium of SEDI&lt;/i&gt;, ETH Zurich (Switzerland), July 11- July 15 2022.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;8.&lt;/strong&gt; C&#233;bron D., Monville R., Vidal J., Sauret A., Schaeffer N., &lt;a href=&#034;https://drive.google.com/file/d/1mfQMwpYgqWpPOJ55C6ng5c3uQW7Tqz15/view?usp=sharing&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Generation of planetary core zonal flows by mechanical forcings &amp; fingering convection&lt;/a&gt;&lt;br class='autobr' /&gt;
&lt;i&gt;17th Symposium of SEDI&lt;/i&gt;, ETH Zurich (Switzerland), July 11- July 15 2022.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;7.&lt;/strong&gt; Vidal J., C&#233;bron D., &lt;a href=&#034;https://drive.google.com/file/d/1bYOu5_S34Qeof9kf1Xjd8C1Y6B-b2LrV/view?usp=sharing&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Asymptotic models of rotating flows in ellipsoidal planets&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;17th Symposium of SEDI&lt;/i&gt;, ETH Zurich (Switzerland), July 11- July 15 2022.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;6.&lt;/strong&gt; Monville R., C&#233;bron D., Jault D., &lt;a href=&#034;https://monvilre.gitlab.io/pdf/Poster_PNP_compressed.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic effects in magnetized and stratified fluid cores&lt;/a&gt;&lt;br class='autobr' /&gt;
17th Colloque quadriennal de bilan et prospective du PNP, ENS Lyon (France), June 29- July 1 2022&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;5.&lt;/strong&gt; C&#233;bron D., Monville R., Vidal J., Sauret A., Schaeffer N., &lt;a href=&#034;https://drive.google.com/file/d/1mfQMwpYgqWpPOJ55C6ng5c3uQW7Tqz15/view?usp=sharing&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Generation of planetary core zonal flows by mechanical forcings &amp; fingering convection&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;Colloque quadriennal de bilan et prospective du PNP&lt;/i&gt;, ENS Lyon (France), June 29- July 1 2022.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;4.&lt;/strong&gt; Vidal J. &amp; C&#233;bron D., &lt;a href=&#034;https://drive.google.com/file/d/1bYOu5_S34Qeof9kf1Xjd8C1Y6B-b2LrV/view?usp=sharing&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Asymptotic models of rotating flows in ellipsoidal planets&lt;/a&gt; &lt;br class='autobr' /&gt;
&lt;i&gt;Colloque quadriennal de bilan et prospective du PNP&lt;/i&gt;, ENS Lyon (France), June 29- July 1 2022.&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2021 -&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;3.&lt;/strong&gt; Monville R., C&#233;bron D., Jault D., &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/presentation_grezu.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Topographic effects in a stratified layer at the top of the Earth's core&lt;/a&gt;&lt;br class='autobr' /&gt;
Workshop &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/grezumeetingprogram_1_.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Grenoble-Zurich-Marseille-ROB&lt;/a&gt;, ETH Zurich (Switzerland), November 16 2021.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;2.&lt;/strong&gt; Vidal J. &amp; C&#233;bron D., &lt;a href=&#034;https://drive.google.com/file/d/1PJ7lZlDDfr5B21Bd4NZz5rw6sw49LFON/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Kinematic dynamos in triaxial ellipsoids&lt;/a&gt;&lt;br class='autobr' /&gt;
Workshop &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/grezumeetingprogram_1_.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Grenoble-Zurich-Marseille-ROB&lt;/a&gt;, ETH Zurich (Switzerland), November 16 2021.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;1.&lt;/strong&gt; Monville R., C&#233;bron D., Jault D., &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/presentation_iaga_final.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Topographic effects at the core-mantle boundary&lt;/a&gt;&lt;br class='autobr' /&gt;
International conference &lt;a href=&#034;https://storage.unitedwebnetwork.com/files/805/d7e471c039e6826a2b452716c6a85c7a.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;IAGA-IASPEI 2021&lt;/a&gt;, Hyderabad (India), 21-27 August 2021.&lt;/p&gt;&lt;/div&gt;
		
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		<title>ERC project THEIA</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia.html</guid>
		<dc:date>2022-02-09T07:48:38Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, J&#233;r&#233;mie VIDAL, Max SOLAZZO</dc:creator>



		<description>&lt;p&gt;Publications&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/" rel="directory"&gt;ERC project THEIA&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;CENTER&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;Project&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/members.html&#034;&gt;About Us&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/publications.html&#034;&gt;&lt;u&gt;Publications&lt;/u&gt;&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/communications.html&#034;&gt;Communications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/numerics.html&#034;&gt;Numerics&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/experiments.html&#034;&gt;Experiments&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/gallery.html&#034;&gt;Gallery&lt;/a&gt;&lt;/strong&gt; | &lt;/CENTER&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2025 -&lt;/h3&gt;
&lt;p&gt;22. &lt;strong&gt;Semiconvection in rotating spherical shells&lt;/strong&gt;&lt;br class='autobr' /&gt;
P. Pruzina, &lt;u&gt; D. C&#233;bron&lt;/u&gt; , N. Schaeffer, J. Vidal,&lt;br class='autobr' /&gt;
In prep.&lt;/p&gt;
&lt;p&gt;21. &lt;strong&gt;Investigating the Drag Force Due to Inertial Waves Generated by Topography&lt;/strong&gt;&lt;br class='autobr' /&gt;
V. Giraud, J. Noir, R. Monville, J. Vidal, &lt;u&gt; D. C&#233;bron&lt;/u&gt; ,&lt;br class='autobr' /&gt;
In prep.&lt;/p&gt;
&lt;p&gt;20. &lt;strong&gt;Hydromagnetic drag on a rapidly oscillating sphere&lt;/strong&gt;&lt;br class='autobr' /&gt;
&lt;u&gt; D. C&#233;bron&lt;/u&gt; &amp; P. Personnettaz,&lt;br class='autobr' /&gt;
In prep.&lt;/p&gt;
&lt;p&gt;19. &lt;strong&gt;Dissipation of the translational oscillations of the inner core&lt;/strong&gt;&lt;br class='autobr' /&gt;
P. Personnettaz, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, N. Schaeffer, R. Deguen, M. Mandea,&lt;br class='autobr' /&gt;
In prep.&lt;/p&gt;
&lt;p&gt;18. &lt;strong&gt;Did lunar tides sustain the early Earth's geodynamo?&lt;/strong&gt;&lt;br class='autobr' /&gt; J. Vidal &amp; &lt;u&gt; D. C&#233;bron&lt;/u&gt;&lt;br class='autobr' /&gt;
In review. &lt;a href=&#034;https://arxiv.org/pdf/2506.19039&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;17. &lt;strong&gt;Semiconvection unlocks dynamo action in stably-stratified regions of gaseous planets&lt;/strong&gt;&lt;br class='autobr' /&gt;
P. Pruzina, &lt;u&gt; D. C&#233;bron&lt;/u&gt; , N. Schaeffer,&lt;br class='autobr' /&gt;
In review. &lt;a href=&#034;https://arxiv.org/pdf/2506.18521&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;16. &lt;strong&gt;Modal Acoustic Velocimetry in libration-driven flows&lt;/strong&gt;&lt;br class='autobr' /&gt;
H.-C. Nataf, S. Su, P. Roux, P. Cardin, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, Y. Do,&lt;br class='autobr' /&gt;
In review.&lt;/p&gt;
&lt;p&gt;15. &lt;a href=&#034;https://arxiv.org/abs/2402.12992&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;On gravito-inertial surface waves&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
Y. Colin de Verdi&#232;re &amp; J. Vidal&lt;br class='autobr' /&gt;
Contemporary Mathematics (accepted). &lt;a href=&#034;https://arxiv.org/abs/2402.12992&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Preprint&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;14. &lt;a href=&#034;https://arxiv.org/abs/2305.01369&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;The spectrum of the Poincar&#233; operator in an ellipsoid&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
Y. Colin de Verdi&#232;re &amp; J. Vidal&lt;br class='autobr' /&gt;
Journal of Spectral Theory. &lt;a href=&#034;https://arxiv.org/pdf/2305.01369.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Preprint&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;13. &lt;a href=&#034;http://dx.doi.org/10.1029/2024JB029770&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Topographic Drag at the Core-Mantle Interface&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
R. Monville, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, D. Jault,&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of Geophysical Research - Solid Earth&lt;/i&gt;, &lt;strong&gt;130&lt;/strong&gt;, e2024JB029770, 2025. &lt;a href=&#034;https://hal.science/hal-05033958v1/document&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;, &lt;a href=&#034;https://hal.science/hal-05033958v1/file/2024jb029770-sup-0001-supporting%20information%20si-s01.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Supp. Mat.&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2024 -&lt;/h3&gt;
&lt;p&gt;12. &lt;a href=&#034;https://royalsocietypublishing.org/doi/10.1098/rspa.2023.0789&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Inertia-gravity waves in geophysical vortices&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
Vidal J. &amp; Colin de Verdi&#232;re Y., 2024, &lt;br class='autobr' /&gt;
&lt;i&gt;Proceeding of the Royal Society A&lt;/i&gt;, 480 (2285), 20230789. &lt;a href=&#034;https://sdrive.cnrs.fr/s/3qnNbAiLbHCbizA&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;11. &lt;a href=&#034;https://comptes-rendus.academie-sciences.fr/physique/articles/10.5802/crphys.219/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Geophysical flows with topography, a playground for laboratory experiments&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
J. Vidal, J. Noir, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, F. Burmann, R. Monville, V. Giraud, &lt;br class='autobr' /&gt;
&lt;i&gt;Comptes Rendus. Physique&lt;/i&gt;, pp. 1-52, 2024. &lt;a href=&#034;https://arxiv.org/pdf/2501.03396&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;10. &lt;a href=&#034;https://doi.org/10.1029/2024GL110749&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Compaction-driven convection in the growing inner core&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
K. W. Lim, R. Deguen, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, A. Schulze, M. Mandea,&lt;br class='autobr' /&gt;
&lt;i&gt;Geophysical Research Letters&lt;/i&gt;, &lt;strong&gt;51&lt;/strong&gt;, e2024GL110749, 2024. &lt;a href=&#034;https://hal.science/hal-04877533v1/document&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;, &lt;a href=&#034;https://agupubs.onlinelibrary.wiley.com/action/downloadSupplement?doi=10.1029%2F2024GL110749&amp;file=2024GL110749-sup-0001-Supporting+Information+SI-S01.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Sup. Mat.&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2023 -&lt;/h3&gt;
&lt;p&gt;9. &lt;a href=&#034;https://doi.org/10.1063/5.0149836&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;MHz free electron laser x-ray diffraction and modeling of pulsed laser heated diamond anvil cell&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
N. Jaisle, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, Z. Kon&#244;pkov&#225;, et al.,&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of Applied Physics&lt;/i&gt;, &lt;strong&gt;134&lt;/strong&gt;, 095904, 2023. &lt;a href=&#034;https://drive.google.com/file/d/1cs77uW5rUwlfIdc9yhNBCwQ3g9ydWVBY/view&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;8. &lt;a href=&#034;https://doi.org/10.1017/jfm.2022.976&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Precession-driven flows in stress-free ellipsoids&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
J. Vidal &amp; D. C&#233;bron&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of Fluid Mechanics&lt;/i&gt;, &lt;strong&gt;954&lt;/strong&gt;, A5, 2023. &lt;a href=&#034;https://arxiv.org/pdf/2301.03254.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2022 -&lt;/h3&gt;
&lt;p&gt;7. &lt;a href=&#034;https://doi.org/10.1038/s43017-022-00264-1&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Sustaining Earth's magnetic dynamo&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
M. Landeau, A. Fournier, H.-C. Nataf, &lt;u&gt;D. C&#233;bron&lt;/u&gt;, N. Schaeffer&lt;br class='autobr' /&gt;
&lt;i&gt;Nature Reviews Earth &amp; Environment&lt;/i&gt;, &lt;strong&gt;3&lt;/strong&gt;, 255&#8211;269, 2022. &lt;a href=&#034;https://www.nature.com/articles/s43017-022-00264-1.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;, or &lt;a href=&#034;https://rdcu.be/cIGqQ&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;open link&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;6. &lt;a href=&#034;https://doi.org/10.1007/s10712-021-09668-y&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Core Eigenmodes and their Impact on the Earth's Rotation&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
S. A. Triana, M. Dumberry, D. C&#233;bron, J. Vidal, A. Trinh., F. Gerick, J. Rekier, &lt;br class='autobr' /&gt;
&lt;i&gt;Surveys in Geophysics&lt;/i&gt;, &lt;strong&gt;43&lt;/strong&gt;, 107-148, 2022. &lt;a href=&#034;https://link.springer.com/content/pdf/10.1007/s10712-021-09668-y.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2021 -&lt;/h3&gt;
&lt;p&gt;5. &lt;a href=&#034;https://doi.org/10.1121/10.0005909&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Acoustic modes of rapidly rotating ellipsoids subject to centrifugal gravity&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
J. Vidal &amp; D. C&#233;bron,&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of the Acoustical Society of America&lt;/i&gt;, &lt;strong&gt;150&lt;/strong&gt; (2), 1467-1478, 2021. &lt;a href=&#034;https://arxiv.org/pdf/2108.13688.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;4. &lt;a href=&#034;https://doi.org/10.1017/jfm.2021.356&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;The effects of a Robin boundary condition on thermal convection in a rotating spherical shell&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
T. Clarte, N. Schaeffer, S. Labrosse &amp; J. Vidal,&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of Fluid Mechanics&lt;/i&gt;, &lt;strong&gt;918&lt;/strong&gt;, A36, 2021. &lt;a href=&#034;https://arxiv.org/pdf/2011.03412.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;3. &lt;a href=&#034;https://royalsocietypublishing.org/doi/10.1098/rspa.2021.0252&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Kinematic dynamos in triaxial ellipsoids&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
J. Vidal &amp; D. C&#233;bron,&lt;br class='autobr' /&gt;
&lt;i&gt;Proceedings of the Royal Society A&lt;/i&gt;, &lt;strong&gt;477&lt;/strong&gt; (2252), 20210252, 2021. &lt;a href=&#034;https://arxiv.org/pdf/2109.03232.pdf&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;2. &lt;a href=&#034;https://doi.org/10.1017/jfm.2021.220&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Mean zonal flows induced by weak mechanical forcings in rotating spheroids&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
D. C&#233;bron, J. Vidal, N. Schaeffer, A. Borderies, A. Sauret,&lt;br class='autobr' /&gt;
&lt;i&gt;Journal of Fluid Mechanics&lt;/i&gt;, &lt;strong&gt;916&lt;/strong&gt;, A39, 2021. &lt;a href=&#034;https://hal.archives-ouvertes.fr/hal-03162825/document&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- 2020 -&lt;/h3&gt;
&lt;p&gt;1. &lt;a href=&#034;https://doi.org/10.1098/rspa.2020.0131&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;&lt;strong&gt;Acoustic and inertial modes in planetary-like rotating ellipsoids&lt;/strong&gt;&lt;/a&gt;&lt;br class='autobr' /&gt;
J. Vidal &amp; D. C&#233;bron,&lt;br class='autobr' /&gt;
&lt;i&gt;Proceedings of the Royal Society A&lt;/i&gt;, &lt;strong&gt;476&lt;/strong&gt;, 20200131, 2020. &lt;a href=&#034;https://arxiv.org/abs/2108.13795&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;PDF&lt;/a&gt;&lt;/p&gt;&lt;/div&gt;
		
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<item xml:lang="en">
		<title>ERC project THEIA</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6078.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/erc-project-theia-6078.html</guid>
		<dc:date>2022-02-09T07:47:35Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, J&#233;r&#233;mie VIDAL, Max SOLAZZO</dc:creator>



		<description>&lt;p&gt;About Us&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/on-going-projects/erc-project-theia/" rel="directory"&gt;ERC project THEIA&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;CENTER&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/&#034;&gt;Project&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/members.html&#034;&gt;&lt;u&gt;About Us&lt;/u&gt;&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/publications.html&#034;&gt;Publications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/communications.html&#034;&gt;Communications&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/numerics.html&#034;&gt;Numerics&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/experiments.html&#034;&gt;Experiments&lt;/a&gt;&lt;/strong&gt; | &lt;strong&gt;&lt;a href=&#034;https://www.isterre.fr/english/research-observation/teams-1105/geodynamo/means-and-tools/on-going-projects/erc-project-theia/article/gallery.html&#034;&gt;Gallery&lt;/a&gt;&lt;/strong&gt; | &lt;/CENTER&gt;
&lt;p&gt;&lt;/ br &gt;&lt;br class='autobr' /&gt;
&lt;/ br &gt;&lt;/p&gt;
&lt;h3 class=&#034;spip&#034;&gt;- Current members -&lt;/h3&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;PI&lt;/strong&gt; : &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/david-cebron/&#034;&gt;David C&#233;bron&lt;/a&gt;, CNRS researcher and team leader of the Geodynamo group of ISTerre&lt;/li&gt;&lt;/ul&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Research Fellow (2024-2025) &lt;/strong&gt; : &lt;a href=&#034;https://orcid.org/0000-0003-0458-2856&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Paul Pruzina&lt;/a&gt;, working on semi-convection dynamo in planetary spherical fluid layers in rapid rotation&lt;/li&gt;&lt;/ul&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Research Fellow (2025-2026) &lt;/strong&gt; : &lt;a href=&#034;https://orcid.org/0000-0001-8990-0643&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Paolo Personnettaz&lt;/a&gt;, working on parameterization of topographic effects in spherical planetary cores&lt;/li&gt;&lt;/ul&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Engineer&lt;/strong&gt; : &lt;a href=&#034;https://www.linkedin.com/in/maxsolazzo/?originalSubdomain=fr&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Max Solazzo&lt;/a&gt;, CNRS engineer (ISTerre), who design and build the planned project experiments (turbulence studies)&lt;/li&gt;&lt;/ul&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;ISTerre collaborators&lt;/strong&gt; : the &lt;a href=&#034;https://www.isterre.fr/french/recherche-observation/equipes/geodynamo/&#034;&gt;Geodynamo group&lt;/a&gt;, in particular &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/dominique-jault/&#034;&gt;D. Jault&lt;/a&gt; for theory, &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/nathanael-schaeffer/&#034;&gt;N. Schaeffer&lt;/a&gt; for the &lt;a href=&#034;https://nschaeff.bitbucket.io/xshells/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;XSHELLS&lt;/a&gt; simulations, &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/renaud-deguen/&#034;&gt;R. Deguen&lt;/a&gt; and &lt;a href=&#034;https://www.isterre.fr/annuaire/pages-web-du-personnel/henri-claude-nataf/&#034;&gt;H.-C. Nataf&lt;/a&gt; for the experiments&lt;/li&gt;&lt;/ul&gt;&lt;h3 class=&#034;spip&#034;&gt;- Past members -&lt;/h3&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;PhD (2020-2024) &lt;/strong&gt; : &lt;a href=&#034;https://scholar.google.fr/citations?user=NwCJ_ZMAAAAJ&amp;hl=fr&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;R&#233;my Monville&lt;/a&gt;, working on small scale topographic effects (local models). Phd topic: &lt;a href=&#034;http://www.theses.fr/s246730&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Topographic coupling in planetary cores&lt;/a&gt;&lt;/li&gt;&lt;/ul&gt;&lt;ul class=&#034;spip&#034; role=&#034;list&#034;&gt;&lt;li&gt; &lt;strong&gt;Research Fellow (2020-2025) &lt;/strong&gt; : &lt;a href=&#034;https://sites.google.com/view/jvidalhome&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;J&#233;r&#233;mie Vidal&lt;/a&gt;, working on ellipsoidal planetary cores (global models) to study large scale topographic effects&lt;/li&gt;&lt;/ul&gt;&lt;/div&gt;
		
		</content:encoded>


		

	</item>
<item xml:lang="en">
		<title>The ZoRo experiment</title>
		<link>https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/laboratory-experiments/article/the-zoro-experiment.html</link>
		<guid isPermaLink="true">https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/laboratory-experiments/article/the-zoro-experiment.html</guid>
		<dc:date>2020-07-06T10:17:29Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>en</dc:language>
		<dc:creator>David C&#201;BRON, Henri-Claude NATAF, Max SOLAZZO, Philippe CARDIN, Yann DO</dc:creator>



		<description>&lt;p&gt;The ZoRo experiment was built to investigate the formation of &lt;strong&gt;zo&lt;/strong&gt;nal jets in &lt;strong&gt;ro&lt;/strong&gt;tating fluids, such as the atmospheres of giant planets (Jupiter, Saturn), and planetary liquid cores.&lt;/p&gt;

-
&lt;a href="https://www.isterre.fr/english/research/research-teams/geodynamo/means-and-tools/laboratory-experiments/" rel="directory"&gt;Laboratory experiments&lt;/a&gt;


		</description>


 <content:encoded>&lt;div class='rss_texte'&gt;&lt;p&gt;Funded by the French National Research Agency (&lt;a href=&#034;https://anr.fr&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;ANR&lt;/a&gt;) through the &lt;a href='https://www.isterre.fr/french/recherche/projets-de-recherche/projets-anr/projets-termines/article/tudy-turbulence-et-dynamo-dans-les-noyaux-planetaires.html' class=&#034;spip_in&#034; hreflang=&#034;fr&#034;&gt;TuDy project&lt;/a&gt; (2013-2019), the ZoRo experiment was built to investigate the formation of &lt;strong&gt;zo&lt;/strong&gt;nal jets in &lt;strong&gt;ro&lt;/strong&gt;tating fluids, such as the atmospheres of giant planets (Jupiter, Saturn), and planetary liquid cores. The ZoRo project was further funded by &lt;a href='https://www.isterre.fr/english/research/research-projects/future-investment-program-pia-labex-equipex/completed-projects/article/labex-osug-2020-velocimetrie-par-splitting-de-modes-acoustiques.html' class=&#034;spip_in&#034; hreflang=&#034;fr&#034;&gt;Labex OSUG@2020&lt;/a&gt; (2013-2014) and &lt;a href=&#034;https://pnpinsu.fr/&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Programme National de Plan&#233;tologie&lt;/a&gt; (2022).&lt;/p&gt;
&lt;p&gt;The geodynamo team has developed a unique method to map fluid flow in a rapidly rotating gas-filled spheroid: the Modal Acoustic Velocimetry (&lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/2014_triana_et_al_njp.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Triana et al, 2014&lt;/a&gt;; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/2020_su_et_al_ejmflu.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Su et al, 2020&lt;/a&gt;; &lt;a href=&#034;https://doi.org/10.1017/jfm.2019.1004&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;Vidal et al., 2020&lt;/a&gt;; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/2025_nataf_et_al_ef.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Nataf et al, 2025&lt;/a&gt;).&lt;/p&gt;
&lt;p&gt;Have a look at the &lt;a href=&#034;https://www.youtube.com/watch?v=g3LOZqAOni4&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;very clear presentation of the ZoRobot project&lt;/a&gt; by intern Gregory de Salaberry Seljak (2022)!&lt;/p&gt;
&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;Zonal jets&lt;/h3&gt;&lt;div class=&#034;col-un-un-un&#034;&gt;&lt;div&gt;&lt;center&gt;&lt;div class='spip_document_10631 spip_document spip_documents spip_document_image spip_documents_left spip_document_left spip_document_avec_legende' data-legende-len=&#034;176&#034; data-legende-lenx=&#034;xxx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L250xH250/jupiter_aurora_web-92608-f2b9e.jpg?1789506402' width='250' height='250' alt='' /&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;Jupiter and aurora
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;&lt;i&gt;Hubble Space Telescope&lt;/i&gt; &#8226; WFC3/UVIS &#8226; STIS&lt;br class='autobr' /&gt;
&lt;small&gt;&lt;i&gt;credits:&lt;/i&gt; NASA, ESA, and J. Nichols (University of Leicester)&lt;/small&gt;
&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;NASA, ESA, and J. Nichols (University of Leicester)
&lt;/div&gt;
&lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;
Strong alternating eastwards and westwards jets shape the surface of Jupiter and Saturn. They are fueled by convective motions in their atmospheres, which are converted into strong zonal jets under the action of the Coriolis force.
&lt;BR&gt;&lt;BR&gt;
What controls the number of jets and their velocities? This is not well understood yet. Numerical simulations reproduce such features, but planetary regimes remain out of reach.&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;center&gt;&lt;div class='spip_document_10636 spip_document spip_documents spip_document_image spip_documents_right spip_document_right spip_document_avec_legende' data-legende-len=&#034;186&#034; data-legende-lenx=&#034;xxx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L271xH250/guervilly_ee-8pre-1ra9rac_2018-85fcc-d2259.png?1789506402' width='271' height='250' alt='' /&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;Quasi-geostrophic numerical simulation of convective jets
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;View from the pole of convective zonal jets in a sphere. E=10&lt;sup&gt;-8&lt;/sup&gt;, Pr=0.1, Ra=9 Ra&lt;sub&gt;c&lt;/sub&gt;.&lt;br class='autobr' /&gt;
&lt;i&gt;credits:&lt;/i&gt; C&#233;line Guervilly
&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;C&#233;line Guervilly
&lt;/div&gt;
&lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt; &lt;/center&gt;&lt;/div&gt;&lt;/div&gt;&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;The ZoRo set-up&lt;/h3&gt;&lt;div class=&#034;col-un-un&#034;&gt;&lt;div&gt;&lt;center&gt;&lt;div class='spip_document_10625 spip_document spip_documents spip_document_image spip_documents_left spip_document_left spip_document_avec_legende' data-legende-len=&#034;63&#034; data-legende-lenx=&#034;x&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L389xH532/zoro2_small-6db4a.jpg?1789506402' width='389' height='532' alt='' /&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;The ZoRo experiment at ISTerre
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;&lt;i&gt;credits:&lt;/i&gt; M. Solazzo
&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;M. Solazzo
&lt;/div&gt;
&lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;
We built the ZoRo experiment to investigate the formation of convective zonal jets in a rapidly rotating gas-filled spheroid (a sphere flattened at the poles).
The inner equatorial radius of the spheroid is &lt;i&gt;r&lt;sub&gt;eq&lt;/sub&gt;&lt;/i&gt;=20 cm, while its polar radius is &lt;i&gt;r&lt;sub&gt;pol&lt;/sub&gt;&lt;/i&gt;=19 cm.
We can rotate ZoRo up to 50 rotation per seconds.
The spheroid can be filled with various gases in order to change the fluid flow parameters.
&lt;BR&gt;&lt;BR&gt;
Fluid flow is measured by an acoustic method.
We use 4 small loudspeakers to produce sounds, which are recorded by 14 tiny microphones.
All the electric signals pass from the rotating spheroid to the Lab through slip-rings.
&lt;BR&gt;&lt;BR&gt;
The spheroidal cavity has been machined with great precision.
Special care has been taken to limit the noise produced by the rotation of ZoRo.
All instrumentation respect symmetries about the axis of rotation and about the equator, in order to insure a balance down to a gram level (see &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/2020_su_et_al_ejmflu_drawings.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Su et al, 2020, technical drawings&lt;/a&gt; for more details).
&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;Acoustic modes in a sphere&lt;/h3&gt;&lt;div class=&#034;col-un-un&#034;&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;Just like sounds of various frequencies can be generated in a pipe or a flute, a gas-filled sphere can resonate at various frequencies.
Resonances occur at specific frequencies, which are produced by specific vibration patterns, called acoustic modes.
&lt;BR&gt;&lt;BR&gt;
In a sphere, the surface pattern of modes is given by spherical harmonics &lt;i&gt;Y&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;m&lt;/sup&gt;(theta,phi)&lt;/i&gt;, while their radial dependency involves spherical Bessel functions &lt;i&gt;j&lt;sub&gt;l&lt;/sub&gt;(k&lt;sub&gt;nl&lt;/sub&gt; r)&lt;/i&gt;.
The triplet of integer mode numbers &lt;i&gt;(n,l,m)&lt;/i&gt; defines an acoustic mode.
Mode numbers give the number of zero crossing of the vibration pattern: in radius for &lt;i&gt;n&lt;/i&gt;, at the surface for &lt;i&gt;l&lt;/i&gt;, and in azimuth &lt;i&gt;phi&lt;/i&gt; for &lt;i&gt;m&lt;/i&gt;.
Following seismological conventions, we label modes as &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;m&lt;/sup&gt;&lt;/i&gt;.
&lt;BR&gt;&lt;BR&gt;
In a perfect sphere, the frequency of &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;m&lt;/sup&gt;&lt;/i&gt; modes does not depend upon &lt;i&gt;m&lt;/i&gt;: modes are degenerate.
&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;center&gt;&lt;div class='spip_document_10628 spip_document spip_documents spip_document_image spip_documents_right spip_document_right spip_document_avec_legende' data-legende-len=&#034;353&#034; data-legende-lenx=&#034;xxxx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/jpg/spherical_harmonics.jpg' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/jpeg&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L344xH200/spherical_harmonics-08027-6af7b.jpg?1789506402' width='344' height='200' alt='' /&gt;&lt;/a&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;Pattern of spherical harmonics Y&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;m&lt;/sup&gt;
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;From top to bottom, mode number &lt;i&gt;l&lt;/i&gt; increases from 0 to 4. Azimuthal mode number &lt;i&gt;m&lt;/i&gt; increases from &lt;i&gt;-l&lt;/i&gt; to &lt;i&gt;+l&lt;/i&gt; from left to right. The central column corresponds to axisymmetric acoustic modes &lt;i&gt;(m=0)&lt;/i&gt;.&lt;br class='autobr' /&gt;
&lt;BR&gt;&lt;BR&gt;
&lt;i&gt;credits:&lt;/i&gt; Florian T. Pokorny, KTH Royal Institute of Technology.
&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;Florian T. Pokorny, KTH Royal Institute of Technology
&lt;/div&gt;
&lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;
&lt;/center&gt;&lt;/div&gt;&lt;/div&gt;&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;Modal Acoustic Velocimetry&lt;/h3&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;Modal Acoustic Velocimetry is a new experimental technique introduced by &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/pdf/2014_triana_et_al_njp.pdf' class=&#034;spip_in&#034; type='application/pdf'&gt;Triana et al, 2014&lt;/a&gt;. It relies on the Doppler effect. &lt;BR&gt;&lt;BR&gt;
Acoustic modes can be regarded as resulting from the constructive interference of waves travelling in opposite directions.
For instance, modes &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;+m&lt;/sup&gt;&lt;/i&gt; and
&lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;-m&lt;/sup&gt;&lt;/i&gt; result from the interference of waves traveling in the prograde and retrograde azimuthal directions.
These two waves will experience an opposite Doppler effect when an azimuthal flow is present. This lifts the &lt;i&gt;&#177;m&lt;/i&gt;-degeneracy: the &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;&#177;m&lt;/sup&gt;&lt;/i&gt; doublet will split into two peaks at distinct frequencies.
More surprisingly, the simple rotation of the fluid and its container can produce a splitting, under the effect of the Coriolis force, even in the absence of differential flow.
&lt;BR&gt;&lt;BR&gt;
A similar method has been used by helioseismologists to unravel azimuthal flows within the Sun!
&lt;/div&gt;&lt;/div&gt;&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;Exciting and recording acoustic modes&lt;/h3&gt;&lt;div class=&#034;col-un-un-un&#034;&gt;&lt;div&gt;&lt;center&gt;&lt;div class='spip_document_10637 spip_document spip_documents spip_document_image spip_documents_center spip_document_center spip_document_avec_legende' data-legende-len=&#034;84&#034; data-legende-lenx=&#034;xx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/png/linear-chirp.svg.png' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/png&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L373xH250/linear-chirp.svg-abc71-9b0fd.png?1789506402' width='373' height='250' alt='' /&gt;&lt;/a&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;An example of linear chirp
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;&lt;i&gt;credit:&lt;/i&gt; Georg-Johann / &lt;a href=&#034;https://creativecommons.org/licenses/by-sa/3.0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;CC BY-SA&lt;/a&gt;
&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;Georg-Johann / &lt;a href=&#034;https://creativecommons.org/licenses/by-sa/3.0&#034; class=&#034;spip_out&#034; rel=&#034;external&#034;&gt;CC BY-SA&lt;/a&gt;
&lt;/div&gt;
&lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;Acoustic modes are excited successively by letting ZoRo's loudspeakers play a linear chirp from 500 to 5000 Hz. &lt;BR&gt;&lt;BR&gt;
Check by yourself what the chirp sounds like!
&lt;BR&gt;&lt;BR&gt;
Microphones record the response of ZoRo to this excitation. The frequency spectrum of these records reveals the resonance peaks of the acoustic modes.
&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;center&gt;&lt;div class=&#034;spip_document_10639 spip_document spip_documents spip_document_audio spip_documents_center spip_document_center spip_document_avec_legende&#034; data-legende-len=&#034;64&#034; data-legende-lenx=&#034;xx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;div class=&#034;audio-wrapper&#034; style='width:400px;max-width:100%;'&gt; &lt;audio class=&#034;mejs mejs-10639 &#034; data-id=&#034;84732e8871f555948a57115d8193cc2e&#034; src='https://www.isterre.fr/sites/www.isterre.fr/IMG/wav/chirp_for_web.wav' type=&#034;audio/x-wav&#034; preload=&#034;none&#034; data-mejsoptions='{&#034;iconSprite&#034;: &#034;plugins-dist/medias/lib/mejs/mejs-controls.svg&#034;,&#034;alwaysShowControls&#034;: true,&#034;loop&#034;:false,&#034;audioWidth&#034;:&#034;100%&#034;,&#034;audioHeight&#034;:&#034;200&#034;,&#034;duration&#034;:45}' controls=&#034;controls&#034; &gt;&lt;/audio&gt; &lt;/div&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;45s-long linear chirp from 500 to 5000 Hz
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;&lt;i&gt;credits:&lt;/i&gt; Ph. Cardin.
&lt;/div&gt; &lt;/figcaption&gt;&lt;div class=&#034;base64javascript15351669996aa9b3624dd226.73951992&#034; title=&#034;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&#034;&gt;&lt;/div&gt; &lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;/div&gt;&lt;hr class=&#034;spip&#034; /&gt;&lt;h3 class=&#034;spip&#034;&gt;The music of ZoRo&lt;/h3&gt;&lt;div class='spip_document_10640 spip_document spip_documents spip_document_image spip_documents_center spip_document_center spip_document_avec_legende' data-legende-len=&#034;232&#034; data-legende-lenx=&#034;xxx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/png/data_spectrum_0.png' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/png&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L500xH155/data_spectrum_0-cd37f-7af8b.png?1789506402' width='500' height='155' alt='' /&gt;&lt;/a&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;Part of the acoustic spectrum of ZoRo at rest
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;f0 = 0 Hz : recorded spectrum from 1200 to 2200 Hz. The vertical lines mark the frequencies of the expected resonances of acoustic modes. The names of the nSl multiplets are indicated.
&lt;/div&gt; &lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;&lt;div class=&#034;col-un-un&#034;&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;Because ZoRo is a spheroid rather than a sphere, the &lt;i&gt;m&lt;/i&gt;-degeneracy of the acoustic modes is partly lifted: the resonance frequency of an &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;&#177;m&lt;/sup&gt;&lt;/i&gt; doublet depends on |m| (colored vertical bars give their predicted frequencies).
&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;center&gt;&lt;div class=&#034;spip_document_10627 spip_document spip_documents spip_document_audio spip_documents_center spip_document_center spip_document_avec_legende&#034; data-legende-len=&#034;56&#034; data-legende-lenx=&#034;x&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;div class=&#034;audio-wrapper&#034; style='width:400px;max-width:100%;'&gt; &lt;audio class=&#034;mejs mejs-10627 &#034; data-id=&#034;81fb86fbfbf2ac4c63363516ab182779&#034; src='https://www.isterre.fr/sites/www.isterre.fr/IMG/wav/third_trial_0.wav' type=&#034;audio/x-wav&#034; preload=&#034;none&#034; data-mejsoptions='{&#034;iconSprite&#034;: &#034;plugins-dist/medias/lib/mejs/mejs-controls.svg&#034;,&#034;alwaysShowControls&#034;: true,&#034;loop&#034;:false,&#034;audioWidth&#034;:&#034;100%&#034;,&#034;duration&#034;:20}' controls=&#034;controls&#034; &gt;&lt;/audio&gt; &lt;/div&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;part of the acoustic record of ZoRo at rest
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;H-C. Nataf
&lt;/div&gt;
&lt;/figcaption&gt;&lt;div class=&#034;base64javascript15351669996aa9b3624dd226.73951992&#034; title=&#034;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&#034;&gt;&lt;/div&gt; &lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;
Exercise your ear: try to identify all the resonances displayed in the spectrum.
&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class='spip_document_10641 spip_document spip_documents spip_document_image spip_documents_center spip_document_center spip_document_avec_legende' data-legende-len=&#034;261&#034; data-legende-lenx=&#034;xxxx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;a href='https://www.isterre.fr/sites/www.isterre.fr/IMG/png/data_spectrum_15.png' class=&#034;spip_doc_lien mediabox&#034; type=&#034;image/png&#034;&gt; &lt;img src='https://www.isterre.fr/sites/www.isterre.fr/local/cache-vignettes/L500xH154/data_spectrum_15-d60c2-17c82.png?1789506402' width='500' height='154' alt='' /&gt;&lt;/a&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;Part of the acoustic spectrum of ZoRo spinning at 15 rotations per second
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_descriptif '&gt;f0 = 15 Hz : recorded spectrum from 1200 to 2200 Hz. The vertical lines mark the frequencies of the expected resonances of acoustic modes. The names of the nSl multiplets are indicated.
&lt;/div&gt; &lt;/figcaption&gt;&lt;/figure&gt;
&lt;/div&gt;&lt;div class=&#034;col-un-un&#034;&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;
When ZoRo is spinning, acoustic modes are split under the action of the Coriolis force. Now the &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;-m&lt;/sup&gt;&lt;/i&gt; and &lt;i&gt;&lt;sub&gt;n&lt;/sub&gt;S&lt;sub&gt;l&lt;/sub&gt;&lt;sup&gt;+m&lt;/sup&gt;&lt;/i&gt; singlets show up at slightly different frequencies (pairs of colored vertical bars indicate their expected splitting).
The same is observed for the seismic modes of the Earth!
&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;center&gt;&lt;div class=&#034;spip_document_10630 spip_document spip_documents spip_document_audio spip_documents_center spip_document_center spip_document_avec_legende&#034; data-legende-len=&#034;84&#034; data-legende-lenx=&#034;xx&#034;
&gt;
&lt;figure class=&#034;spip_doc_inner&#034;&gt; &lt;div class=&#034;audio-wrapper&#034; style='width:400px;max-width:100%;'&gt; &lt;audio class=&#034;mejs mejs-10630 &#034; data-id=&#034;17b809ba6a0264f5bcd78be62e1e48f0&#034; src='https://www.isterre.fr/sites/www.isterre.fr/IMG/wav/third_trial_15.wav' type=&#034;audio/x-wav&#034; preload=&#034;none&#034; data-mejsoptions='{&#034;iconSprite&#034;: &#034;plugins-dist/medias/lib/mejs/mejs-controls.svg&#034;,&#034;alwaysShowControls&#034;: true,&#034;loop&#034;:false,&#034;audioWidth&#034;:&#034;100%&#034;,&#034;duration&#034;:20}' controls=&#034;controls&#034; &gt;&lt;/audio&gt; &lt;/div&gt;
&lt;figcaption class='spip_doc_legende'&gt; &lt;div class='spip_doc_titre '&gt;&lt;strong&gt;part of the acoustic record of ZoRo spinning at 15 rotations per second
&lt;/strong&gt;&lt;/div&gt; &lt;div class='spip_doc_credits '&gt;H-C. Nataf
&lt;/div&gt;
&lt;/figcaption&gt;&lt;div class=&#034;base64javascript15351669996aa9b3624dd226.73951992&#034; title=&#034;PHNjcmlwdD4gdmFyIG1lanNwYXRoPSdwbHVnaW5zLWRpc3QvbWVkaWFzL2xpYi9tZWpzL21lZGlhZWxlbWVudC1hbmQtcGxheWVyLm1pbi5qcz8xNzg4MzUwNTc2JyxtZWpzY3NzPSdwbHVnaW5zLWRpc3QvbWVkaWFzL2xpYi9tZWpzL21lZGlhZWxlbWVudHBsYXllci5taW4uY3NzPzE3ODgzNTA1NzYnOwp2YXIgbWVqc2xvYWRlcjsKKGZ1bmN0aW9uKCl7dmFyIGE9bWVqc2xvYWRlcjsidW5kZWZpbmVkIj09dHlwZW9mIGEmJihtZWpzbG9hZGVyPWE9e2dzOm51bGwscGx1Zzp7fSxjc3M6e30saW5pdDpudWxsLGM6MCxjc3Nsb2FkOm51bGx9KTthLmluaXR8fChhLmNzc2xvYWQ9ZnVuY3Rpb24oYyl7aWYoInVuZGVmaW5lZCI9PXR5cGVvZiBhLmNzc1tjXSl7YS5jc3NbY109ITA7dmFyIGI9ZG9jdW1lbnQuY3JlYXRlRWxlbWVudCgibGluayIpO2IuaHJlZj1jO2IucmVsPSJzdHlsZXNoZWV0IjtiLnR5cGU9InRleHQvY3NzIjtkb2N1bWVudC5nZXRFbGVtZW50c0J5VGFnTmFtZSgiaGVhZCIpWzBdLmFwcGVuZENoaWxkKGIpfX0sYS5pbml0PWZ1bmN0aW9uKCl7ITA9PT1hLmdzJiZmdW5jdGlvbihjKXtqUXVlcnkoImF1ZGlvLm1lanMsdmlkZW8ubWVqcyIpLm5vdCgiLmRvbmUsLm1lanNfX3BsYXllciIpLmVhY2goZnVuY3Rpb24oKXtmdW5jdGlvbiBiKCl7dmFyIGU9ITAsaDtmb3IoaCBpbiBkLmNzcylhLmNzc2xvYWQoZC5jc3NbaF0pO2Zvcih2YXIgZiBpbiBkLnBsdWdpbnMpInVuZGVmaW5lZCI9PQp0eXBlb2YgYS5wbHVnW2ZdPyhlPSExLGEucGx1Z1tmXT0hMSxqUXVlcnkuZ2V0U2NyaXB0KGQucGx1Z2luc1tmXSxmdW5jdGlvbigpe2EucGx1Z1tmXT0hMDtiKCl9KSk6MD09YS5wbHVnW2ZdJiYoZT0hMSk7ZSYmalF1ZXJ5KCIjIitjKS5tZWRpYWVsZW1lbnRwbGF5ZXIoalF1ZXJ5LmV4dGVuZChkLm9wdGlvbnMse3N1Y2Nlc3M6ZnVuY3Rpb24oYSxjKXtmdW5jdGlvbiBiKCl7dmFyIGI9alF1ZXJ5KGEpLmNsb3Nlc3QoIi5tZWpzX19pbm5lciIpO2EucGF1c2VkPyhiLmFkZENsYXNzKCJwYXVzaW5nIiksc2V0VGltZW91dChmdW5jdGlvbigpe2IuZmlsdGVyKCIucGF1c2luZyIpLnJlbW92ZUNsYXNzKCJwbGF5aW5nIikucmVtb3ZlQ2xhc3MoInBhdXNpbmciKS5hZGRDbGFzcygicGF1c2VkIil9LDEwMCkpOmIucmVtb3ZlQ2xhc3MoInBhdXNlZCIpLnJlbW92ZUNsYXNzKCJwYXVzaW5nIikuYWRkQ2xhc3MoInBsYXlpbmciKX1iKCk7YS5hZGRFdmVudExpc3RlbmVyKCJwbGF5IixiLCExKTsKYS5hZGRFdmVudExpc3RlbmVyKCJwbGF5aW5nIixiLCExKTthLmFkZEV2ZW50TGlzdGVuZXIoInBhdXNlIixiLCExKTthLmFkZEV2ZW50TGlzdGVuZXIoInBhdXNlZCIsYiwhMSk7Zy5hdHRyKCJhdXRvcGxheSIpJiZhLnBsYXkoKX19KSl9dmFyIGc9alF1ZXJ5KHRoaXMpLmFkZENsYXNzKCJkb25lIiksYzsoYz1nLmF0dHIoImlkIikpfHwoYz0ibWVqcy0iK2cuYXR0cigiZGF0YS1pZCIpKyItIithLmMrKyxnLmF0dHIoImlkIixjKSk7dmFyIGQ9e29wdGlvbnM6e30scGx1Z2luczp7fSxjc3M6W119LGUsaDtmb3IoZSBpbiBkKWlmKGg9Zy5hdHRyKCJkYXRhLW1lanMiK2UpKWRbZV09alF1ZXJ5LnBhcnNlSlNPTihoKTtiKCl9KX0oalF1ZXJ5KX0pO2EuZ3N8fCgidW5kZWZpbmVkIiE9PXR5cGVvZiBtZWpzY3NzJiZhLmNzc2xvYWQobWVqc2NzcyksYS5ncz1qUXVlcnkuZ2V0U2NyaXB0KG1lanNwYXRoLGZ1bmN0aW9uKCl7YS5ncz0hMDthLmluaXQoKTtqUXVlcnkoYS5pbml0KTtvbkFqYXhMb2FkKGEuaW5pdCl9KSl9KSgpOzwvc2NyaXB0Pg==&#034;&gt;&lt;/div&gt; &lt;/figure&gt;
&lt;/div&gt;&lt;/center&gt;&lt;/div&gt;&lt;div&gt;&lt;div class=&#034;encartgris&#034;&gt;
Exercise your ear: can you hear the small differences from the record at rest?
&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;
		
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