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

基因组

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

NAIVE

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.

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门闩

HEED

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

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Jogging

残暴

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

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来就得意

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