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Titlebook: Scale Space and Variational Methods in Computer Vision; 7th International Co Jan Lellmann,Martin Burger,Jan Modersitzki Conference proceedi

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11#
發(fā)表于 2025-3-23 12:24:12 | 只看該作者
Pascal Peter,Jan Contelly,Joachim Weickert non-traditional beta plane a noticeable portion of incident inertial waves is not reflected at the inertial latitude but goes through; these waves propagate several hundred kilometers further poleward trapped in three narrowing waveguides. Most of the wave energy passing through becomes trapped int
12#
發(fā)表于 2025-3-23 17:09:02 | 只看該作者
13#
發(fā)表于 2025-3-23 20:22:42 | 只看該作者
non-traditional beta plane a noticeable portion of incident inertial waves is not reflected at the inertial latitude but goes through; these waves propagate several hundred kilometers further poleward trapped in three narrowing waveguides. Most of the wave energy passing through becomes trapped int
14#
發(fā)表于 2025-3-23 22:37:45 | 只看該作者
15#
發(fā)表于 2025-3-24 05:26:40 | 只看該作者
Charles-Alban Deledalle,Nicolas Papadakis,Joseph Salmon,Samuel Vaiternd dry friction. The analysed example is the wellknown Painlevé system (Painlevé, 1895). In particular we will focus on singularities of the dynamics in sliding regimes, i.e. configurations at which the contact force diverges to infinity. The problem of inconsistencies, that is configurations for wh
16#
發(fā)表于 2025-3-24 06:57:24 | 只看該作者
17#
發(fā)表于 2025-3-24 11:44:22 | 只看該作者
18#
發(fā)表于 2025-3-24 15:24:16 | 只看該作者
nd dry friction. The analysed example is the wellknown Painlevé system (Painlevé, 1895). In particular we will focus on singularities of the dynamics in sliding regimes, i.e. configurations at which the contact force diverges to infinity. The problem of inconsistencies, that is configurations for wh
19#
發(fā)表于 2025-3-24 19:59:00 | 只看該作者
20#
發(fā)表于 2025-3-25 00:49:13 | 只看該作者
Johannes Hertrich,Miroslav Ba?ák,Sebastian Neumayer,Gabriele Steidlfinite-volume version of the code ICARE/IMFT. The flow transition is studied for Reynolds numbers from 40 to 500, and for rotation rates α (ratio of the angular and the free-stream velocities) up to 6. For a fixed Reynolds number, different flow patterns are observed as α increases: Von-Kármán vorte
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