一大块 发表于 2025-3-25 04:03:40
An Investigation of Scalar Dispersion in Grid Turbulenceexperiment (., ., ., .). The instantaneous three-dimensional structure, however, reveals a rich topology of scalar structures that was found to persist in the volume interrogated, spanning a distance from the grid and release point between 22 and 30 grid mesh lengths, which is in the self-similar gr开玩笑 发表于 2025-3-25 11:09:19
http://reply.papertrans.cn/67/6660/665943/665943_22.pngintegrated 发表于 2025-3-25 14:00:25
Turbulent Drag Reduction with Surfactant Additives — Basic Research and Application to an Air Condit the other hand, the design system for surfactant solutions is not mature because drag-reducing flow phenomena are much more complicated than for Newtonian flow, for example, the friction factor for a surfactant solution depends not only on Reynolds number but also pipe diameter. In order to provideobstinate 发表于 2025-3-25 15:55:58
Numerical Studies of Flow Past Two Side-by-Side Circular Cylindersmulation. The Reynolds number based on free-stream velocity and cylinder diameter is 5 800, which is in the subcritical regime. The transverse pitch ratio . = 3 is investigated. Laminar boundary layer, transition in shear layer, flow separation, large vortex structures and flow interference in the w单调女 发表于 2025-3-25 21:53:46
Three-dimensional Evolution of the Flow Through a Curved Square Ductunderstand the properties of the traveling-wave solutions. It is worthy noting that dominant modes have the same phase velocity, which proves that the traveling-wave is unique under the calculations conducted here..Although the uniformity in the main-flow direction assumed in 2-D calculations does nAccede 发表于 2025-3-26 00:20:14
http://reply.papertrans.cn/67/6660/665943/665943_26.png表两个 发表于 2025-3-26 08:20:09
http://reply.papertrans.cn/67/6660/665943/665943_27.png护身符 发表于 2025-3-26 11:38:46
http://reply.papertrans.cn/67/6660/665943/665943_28.png支架 发表于 2025-3-26 12:58:56
http://reply.papertrans.cn/67/6660/665943/665943_29.pngHectic 发表于 2025-3-26 20:34:04
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