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   <dc:identifier>https://dx.doi.org/10.35097/1550</dc:identifier>
   <dc:creator>Moriche, Manuel</dc:creator>
   <dc:creator>Hettmann, Daniel</dc:creator>
   <dc:creator>García-Villalba, Manuel</dc:creator>
   <dc:creator>Uhlmann, Markus</dc:creator>
   <dc:title>Supplementary animations "On the clustering of low-aspect-ratio oblate spheroids settling in ambient fluid"</dc:title>
   <dc:publisher>Karlsruhe Institute of Technology</dc:publisher>
   <dc:date>2023</dc:date>
   <dc:subject>Engineering</dc:subject>
   <dc:type>dataset</dc:type>
   <dc:subject>Dataset</dc:subject>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:rights>https://creativecommons.org/licenses/by-nc-nd/4.0/legalcode</dc:rights>
   <dc:description>ANIMATIONS FROM "On the clustering of low-aspect-ratio oblate spheroids settling in ambient fluid" by Manuel Moriche, Daniel Hettmann, Manuel García-Villalba and Markus Uhlmann. J. Fluid Mech., 963:A1, 2023. DOI; 10.1017/jfm.2023.261&#xD;
&#xD;
# Many-particle cases&#xD;
&#xD;
## Flow configuration&#xD;
&#xD;
The animations correspond to the cases G111 and G152 described in table 1 from the&#xD;
original article. In these cases a set of many particles settle under gravity in a&#xD;
triply periodic configuration. The particles considered are oblate spheroids of&#xD;
aspect ratio 1.5 and the number of them is such that the solid volume fraction is 0.5%,&#xD;
which corresponds to the dilute regime. The cases differ from each other in the Galileo&#xD;
number: `G=sqrt((rhop/rhof-1)*g*D**3)/nu=110.56` and 152.02 for cases G111 and G152,&#xD;
respectively. The size of computational domain is approximately `[55x55x220]D**3`,&#xD;
where D is the diameter of a sphere with the same volume as the spheroids and the&#xD;
resolution used (`D/dx`) is approximately 21.&#xD;
&#xD;
The time is indicated in the videos is expressed in `D/Ug` units, where&#xD;
`Ug=sqrt((rhop/rhof-1)*abs(g)*D)` is a gravitationally scaled velocity.&#xD;
&#xD;
## Content &#xD;
&#xD;
For each case there are different videos of the initial or converged state, or different&#xD;
representations of the flow/particles.&#xD;
&#xD;
The case, part of the video and representation is contained in the name of each video:&#xD;
1. Case:&#xD;
 - `G111`: Galileo 110.56.&#xD;
 - `G152`: Galileo 152.02.&#xD;
2. Time interval of the simulation:&#xD;
 - `INITIAL`: First simulated time, including the time before releasing the particles (t&lt;0).&#xD;
 - `CONVERGED`: Statistically stationary part of the simulation.&#xD;
3. Point of view: `bottom`, `iso`, `side` and `side_zoomed`.&#xD;
4. Representation. In every video particles are always represented in pink and wakes with&#xD;
   transparency isocontours of Q criterion. Additionally, isocontours of filtered vertical&#xD;
   velocity are represented in two ways:&#xD;
 - `low_speed`: The value to define the isocontour is similar to that of the mixture. In this&#xD;
   representation the regions in which particles are located in clustering/non-clustering&#xD;
   regions are easily identified. Dark blue face points to non-clustering, slow regions and&#xD;
   light blue face points to clustering, fast regions.&#xD;
 - `high_speed`: The value to define isocontour is approximately 50% larger than the average&#xD;
   velocity of the mixture. Therefore, the isocontours (in yellow) indicate regions of&#xD;
   where the downward velocity is greatly enhanced.&#xD;
 - `only_wakes`: No flow velocity is represented. Only side zoomed view is available for&#xD;
   this representation.&#xD;
&#xD;
# Drafting-kissing-tumbling&#xD;
&#xD;
For illustration purposes one animation is included (`DKT_animation.mp4`) of the &#xD;
drafting-kissing-tumbling simulations. The simulations have been performed &#xD;
for Galileo 110.56 with density ratio 1.5. The size of the computational domain &#xD;
measures `[10.66 x 10.66 x 21.33] D**3`. Four configurations are considered:&#xD;
&#xD;
 - Free-to-rotate spheres (angular motion enabled).&#xD;
 - Rotationally-locked spheres (angular motion suppressed).&#xD;
 - Free-to-rotate spheroids of aspect ratio 1.5 (angular motion enabled).&#xD;
 - Rotationally-locked spheroids of aspect ratio 1.5 (angular motion suppressed).&#xD;
&#xD;
In the animation the four configurations are shown for a single initial condition, namely&#xD;
the relative position of the trailing particle with respect to the leading particle is  `[0.625, 7.5] D`.&#xD;
The particles are represented in green with a mesh that helps to visualize the rotation and&#xD;
contours of vertical velocity are shown in grey scale.&#xD;
&#xD;
# References:&#xD;
&#xD;
Manuel Moriche, Daniel Hettmann, Manuel García-Villalba and Markus Uhlmann,&#xD;
_"On the clustering of low-aspect-ratio oblate spheroids settling in ambient fluid"_,&#xD;
accepted in J. Fluid Mech.&#xD;
&#xD;
# History:&#xD;
&#xD;
__04.10.2022__ Creation and data added&#xD;
__06.02.2023__ DKT animation added&#xD;
# Contact&#xD;
&#xD;
[Manuel Moriche](mailto:manuel.guerrero@kit.edu)&#xD;
[Markus Uhlmann](mailto:markus.uhlmann@kit.edu)</dc:description>
   <dc:identifier>10.5445/IR/1000151148</dc:identifier>
   <dc:identifier>KITopen-DOI</dc:identifier>
   <dc:relation>https://publikationen.bibliothek.kit.edu/1000151148</dc:relation>
   <dc:format>application/x-tar</dc:format>
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