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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Sánchez, P.
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Topics
Publications (7/7 displayed)
- 2015Actin filament turnover drives leading edge growth during myelin sheath formation in the central nervous system.citations
- 2014Cohesion, granular solids, granular liquids, and their connection to small near-Earth objects
- 2014Cohesive Self-Gravitating Aggregates and Their Path of Disruption
- 2014The strength of regolith and rubble pile asteroidscitations
- 2014A smog chamber comparison of a microfluidic derivatisation measurement of gas-phase glyoxal and methylglyoxal with other analytical techniquescitations
- 2011Rotation and Reshaping of Self-gravitating Aggregates
- 2011Rotational Reshaping and Yield Stress of Rubble-Pile Asteroids
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document
Rotation and Reshaping of Self-gravitating Aggregates
Abstract
Using a Soft-Sphere DEM code we simulate the reshaping and disruption of a self-gravitating 3D granular aggregate by increasing its spin rate. During the process, we monitor the evolution of the internal stresses in the aggregate to find its yield stress using the Maximum Stress, Von Mises and Drucker-Prager yield criteria. In the simulations we either increase the number of particles or their density to increase the total mass of the aggregate and find an increment in the yield stress. In addition, once a reshaping spin rate (density dependent) has been reached, its further increase causes further reshape (ultimately fission) and a decrease in the spin rate itself....