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Titlebook: Laminar-Turbulent Transition; IUTAM Symposium Toul D. Arnal,R. Michel Conference proceedings 1990 Springer-Verlag, Berlin Heidelberg 1990 G

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樓主: 可樂
41#
發(fā)表于 2025-3-28 18:07:01 | 只看該作者
Kenneth S. Breuer temperature (RT). AlO. is easily formed by oxidizing a pre-deposited Al layer. The MTJ with FM/I/FM sandwich core structure and the spin-dependent tunneling transport properties drew a wide range of interest resulting the so far largest magnetoresistance (MR) ratio of 81% at RT and 107% at 4.2 K in
42#
發(fā)表于 2025-3-28 21:45:23 | 只看該作者
Experimental Investigation of Tollmien Schlichting Instability and Transition in Similar Boundary La= ?0.14) under natural disturbance conditions. At 23 streamwise stations, mean velocity profiles, power spectra, power distributions across the boundary layer and amplification spectra are measured and compared with boundary layer- and linear stability calculations.
43#
發(fā)表于 2025-3-28 23:21:55 | 只看該作者
44#
發(fā)表于 2025-3-29 04:21:13 | 只看該作者
45#
發(fā)表于 2025-3-29 08:36:00 | 只看該作者
Nonlinear Breakdowns in Boundary Layer Transitionakdowns and scales. The article notes in particular truly nonlinear theories for which the mean-flow profile is completely altered from its original state. Two- and three-dimensional flow theory and conjectures on turbulent boundary-layer structures are included. Specific recent findings noted, and
46#
發(fā)表于 2025-3-29 11:47:00 | 只看該作者
47#
發(fā)表于 2025-3-29 18:18:39 | 只看該作者
48#
發(fā)表于 2025-3-29 22:31:57 | 只看該作者
Effect of Controlled Resonant Interactions and Mode Detuning on Turbulent Transition in Boundary Lay study the growth of three-dimensional disturbances in a Blasius boundary layer. This was accomplished using a computer controlled array of line heaters to produce time periodic, spanwise-phase-varying velocity perturbations. Conditions for subharmonic resonance with a TS mode (α,0) and symmetric ob
49#
發(fā)表于 2025-3-30 00:12:18 | 只看該作者
50#
發(fā)表于 2025-3-30 07:49:04 | 只看該作者
The Evolution of a Localized Disturbance in a Laminar Boundary Layerious results, the evolving disturbance consists of two parts; an advective portion which reflects the structure of the initial disturbance and which travels at approximately the local mean velocity, and a dispersive wave portion which grows or decays according to Tollmien-Schlichting instability the
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