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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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Hogg, Andrew J.
University of Bristol
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2023Obstructed free-surface viscoplastic flow on an inclined planecitations
- 2023Viscoplastic flow between hinged platescitations
- 2022Flow of a yield-stress fluid past a topographical featurecitations
- 2021The converging flow of viscoplastic fluid in a wedge or conecitations
- 2016Sustained axisymmetric intrusions in a rotating systemcitations
- 2009Slumps of viscoplastic fluids on slopescitations
- 2007Two-dimensional dam break flows of Herschel-Bulkley fluids: The approach to the arrested statecitations
- 2002Experimental constraints on shear mixing rates and processescitations
Places of action
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article
The converging flow of viscoplastic fluid in a wedge or cone
Abstract
Converging flows of viscoplastic fluids, driven steadily through wedges and axisymmetric cones, are studied analytically and numerically.When the yield stress is relatively large, the bulk of the fluid flows plastically apart from within thin layers where the fluid is strongly sheared in order to achieve no-slip at the boundary.Conversely, when the yield stress is relatively small, the motion is viscously-dominated with weak corrections to the velocity and stress fields due to viscoplastic effects. For both regimes, viscoplasticity induces a weak angular velocity, directed away from the boundaries, and purely radial flow is not possible.The structure of the flow is calculated using asymptotic methods, confirmed by finite element numerical simulations.Flows of both Bingham and Herschel-Bulkley fluids are analysed, and both planar and axisymmetric geometries are considered. Although these cases differ in their details, they share the same qualitative structure. In particular, the viscoplastic boundary layers that emerge when the yield stress is relatively large, ensure not only that no-slip is enforced, but also, through an intermediate matching layer, that the shear rates remain bounded.