Clique
发表于 2025-3-21 16:03:29
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附录
发表于 2025-3-21 22:01:50
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anachronistic
发表于 2025-3-22 03:19:32
Laminar Two-Dimensional Flowes in motion, allowing for the formation of two-dimensional velocity fields. The flows may be steady or unsteady. We discuss a selection of classical flows with generic relevance for technical applications, as represented in other books as well [., ., ., .]. We add the discussion of a flow relevant
动物
发表于 2025-3-22 06:09:54
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磨碎
发表于 2025-3-22 10:06:30
Boundary-Layer Flowtions of the momentum equation in boundary-layer form. The boundary-layer character of the flows is brought about by the superimposition of convective momentum transport in the main flow direction and diffusive (or turbulent) transport in the direction transverse to it. This type of flow occurs not
模仿
发表于 2025-3-22 14:56:25
Flows with Interfacesd two-phase flows, such as sprays and bubbly flows. We are interested in the instability of liquid sheets and jets submerged in another, immiscible fluid. For transport processes across the interface, oscillations of drops and bubbles may have a significant influence. We also look at the behaviour o
调整
发表于 2025-3-22 19:33:15
Heat Transfer diffusion equation as the underlying differential equation for the spatiotemporal evolution of temperature. As far as convective processes are concerned, the intention to have analytical descriptions clearly puts the restriction to laminar flow in simple geometries.
NUL
发表于 2025-3-22 22:40:40
Mass Transferffusion, which involves the diffusion equation as the underlying differential equation for the spatiotemporal evolution of the species concentration. As far as convective processes are concerned, the intention to have analytical descriptions clearly puts the restriction to laminar flow in simple geo
预防注射
发表于 2025-3-23 05:06:50
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defuse
发表于 2025-3-23 06:49:12
The Non-absoluteness of Christianitywo-dimensional momentum equation with the velocity components given as spatial derivatives of the stream function. The stream function is defined such that its derivatives yield a solenoidal velocity field. The analyses of the flows discussed in Part I of this book are based on this function. In vie