REP
发表于 2025-3-23 12:24:12
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
Incorporate
发表于 2025-3-23 17:09:02
http://reply.papertrans.cn/87/8611/861088/861088_12.png
padding
发表于 2025-3-23 20:22:42
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
心胸狭窄
发表于 2025-3-23 22:37:45
http://reply.papertrans.cn/87/8611/861088/861088_14.png
Carminative
发表于 2025-3-24 05:26:40
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
Hla461
发表于 2025-3-24 06:57:24
http://reply.papertrans.cn/87/8611/861088/861088_16.png
Ebct207
发表于 2025-3-24 11:44:22
http://reply.papertrans.cn/87/8611/861088/861088_17.png
细微差别
发表于 2025-3-24 15:24:16
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
chassis
发表于 2025-3-24 19:59:00
http://reply.papertrans.cn/87/8611/861088/861088_19.png
Myocyte
发表于 2025-3-25 00:49:13
Johannes Hertrich,Miroslav Bačák,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