2002
DOI: 10.1007/978-3-662-04765-1
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The Origin of Turbulence in Near-Wall Flows

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Cited by 118 publications
(46 citation statements)
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“…In the classical linear theory of stability of quasi-parallel shear flows, this is explained by the formation in the zone of detachment of the profiles of average velocity with the inflection point, which are more unstable with respect to oscillations of small amplitudes than the local velocity distributions in the attached boundary layer (see the monograph [13] and original works, [14][15][16]). Theoretical conclusions are consistent with the results of experimental studies and direct numerical simulation of flow in local detachment areas, including behind two-dimensional elements of unevenness in a streamlined surface; literary references to numerous publications on this subject are given in [17].…”
Section: Introductionsupporting
confidence: 77%
“…In the classical linear theory of stability of quasi-parallel shear flows, this is explained by the formation in the zone of detachment of the profiles of average velocity with the inflection point, which are more unstable with respect to oscillations of small amplitudes than the local velocity distributions in the attached boundary layer (see the monograph [13] and original works, [14][15][16]). Theoretical conclusions are consistent with the results of experimental studies and direct numerical simulation of flow in local detachment areas, including behind two-dimensional elements of unevenness in a streamlined surface; literary references to numerous publications on this subject are given in [17].…”
Section: Introductionsupporting
confidence: 77%
“…Additionally, they observed reduction of the LSB size from both upstream and downstream directions. Similarly to and Boiko et al (2002), they suggested a feedback loop process to explain the bubble size reduction due to controlled disturbances. More specifically, a disturbance input alters the flow in the aft part of the bubble, resulting in a global change of pressure gradient due to viscous-inviscid interactions.…”
Section: Introductionmentioning
confidence: 85%
“…The disturbance length (200 ms) is equal to the length of pulse, which moves the membrane upward. This structure is corresponding to the longitudinal localized streaky structures, or so-called "puff" structures, which are in more detail investigated at [3][4][5][6][7][8][9][10][11]. Going downstream, the flow pulsations of this structure (u min and u max ) become weaker.…”
Section: Resultsmentioning
confidence: 99%
“…This method makes it possible detailed investigations of characteristics for artificially introduced perturbations with saving of phase information, to trace the dynamics of the development of a concrete perturbation at all its stages. In addition to the widely used suction-injection technique [4,5], another method is also used where the boundary layer disturbances are generated by vibrations of a local surface area. Experimental investigation of the origin and development of disturbances, generated by vibration of three-dimensional surface in the Blasius boundary layer is shown in [6] and for the straight wing boundary layer in [7].…”
Section: Introductionmentioning
confidence: 99%