Multimedia files – 10/13 Secondary instability of streamwise vortices in a 3D flow Contents: 1. Test model 2. Basic flow 3. Isolated vortices, mean flow.

Slides:



Advertisements
Similar presentations
Response of shear flows to external disturbances Contents: 1. Acoustic receptivity of laminar separating boundary layer 2. Acoustic receptivity of laminar.
Advertisements

Multimedia files – 9/13 Streak instability in adverse pressure gradient boundary layer Contents: 1. Test model 2. Basic flow 3. Varicose instability of.
Sinusoidal and varicose instabilities of streaks in a boundary layer
Contents: 1. Late stage of laminar-turbulent transition on a flat plate 2. Swept-wing boundary layer 3. Test model 4. Automated measurements 5. Controlled.
Formulation of linear hydrodynamic stability problems
/ /17 32/ / /
Reflection nurulquran.com.
Copyright 2011 Elsevier Inc. All rights reserved.
Multiplication X 1 1 x 1 = 1 2 x 1 = 2 3 x 1 = 3 4 x 1 = 4 5 x 1 = 5 6 x 1 = 6 7 x 1 = 7 8 x 1 = 8 9 x 1 = 9 10 x 1 = x 1 = x 1 = 12 X 2 1.
Division ÷ 1 1 ÷ 1 = 1 2 ÷ 1 = 2 3 ÷ 1 = 3 4 ÷ 1 = 4 5 ÷ 1 = 5 6 ÷ 1 = 6 7 ÷ 1 = 7 8 ÷ 1 = 8 9 ÷ 1 = 9 10 ÷ 1 = ÷ 1 = ÷ 1 = 12 ÷ 2 2 ÷ 2 =
Presenter Name(s) Issue date National Student.
Summative Math Test Algebra (28%) Geometry (29%)
Turbulent flow over groups of urban-like obstacles
THE PHYSICAL MODELLING OF FLOWS AFTER MOVING OBSTRUCTIONS E.Ya. Epik, T.T. Suprun Institute of Engineering Thermophysics of National Academy of Sciences.
HEAT TRANSFER Final Review # 1.
REVIEW: Arthropod ID. 1. Name the subphylum. 2. Name the subphylum. 3. Name the order.
EU Market Situation for Eggs and Poultry Management Committee 21 June 2012.
COMPUTER B Y : L K. WINDOWS INFORMATION B Y : L K.
Resistência dos Materiais, 5ª ed.
Two scale modeling of superfluid turbulence Tomasz Lipniacki
ENGINEERING MECHANICS CHAPTER 7
1 Linné Flow Centre KTH Mechanics Streak breakdown in bypass transition Dan Henningson Department of Mechanics, KTH Collaborators: Philipp Schlatter, KTH.
Stability of MHD Buoyancy Driven Flows Presented by Naveen Vetcha (UCLA) With contribution from: Sergey Smolentsev (UCLA) Rene Moreau (Prof., Lab. EPM,
Dynamics of Boundary Layer Transition: Measurement and Visualization C. B. Lee State Key Laboratory for Turbulence Research and Complex System, Peking.
External Flows.
Quantification of Laminar flow weakness … P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Instability Analysis of Laminar Flows.
Flow Over Immersed Bodies
L ehrstuhl für Modellierung und Simulation UNIVERSITY of ROSTOCK | CHAIR OF MODELLING AND SIMULATION Physics of turbulence Lecture 2.
6/29/20151 Stability of Parallel Flows. 6/29/20152 Analysis by LINEAR STABILITY ANALYSIS. l Transitions as Re increases 0 < Re < 47: Steady 2D wake Re.
Computational Modelling of Unsteady Rotor Effects Duncan McNae – PhD candidate Professor J Michael R Graham.
GEN-BL: Secondary Instability of Saturated CF-Vortices*
Computer Practical: Numerical Gasdynamics Richtmyer-Meshkov Instability Group 6 Comparison of Results with Different Grid Points 2 nd Order Roe Naseem.
Vortical Analysis of Secondary Flows in Turbine Cascades P M V Subbarao Professor Mechanical Engineering Department A Pictorial Fluid Mechanics for Complex.
The sliding Couette flow problem T. Ichikawa and M. Nagata Department of Aeronautics and Astronautics Graduate School of Engineering Kyoto University The.
Multimedia files - 5/13 Görtler Instability Contents: 1. The eldest unsolved linear-stability problem 2. Modern approach to Görtler instability 3. Properties.
1 Liquid-crystal thermography method for the study of stages of instability developing in the cross- flow on the leading edge of the oblique wing Tolkachev.
Influence of wall roughness on near wall turbulence structure by Haigermoser C.*, Vesely L.*, La Polla M., Onorato M., Politecnico di Torino XIV A.I.VE.LA.
Jacob Cohen 1, Ilia Shukhman 2 Michael Karp 1 and Jimmy Philip 1 1. Faculty of Aerospace Engineering, Technion, Haifa, Israel 2. Institute of Solar-Terrestrial.
Numerical study of flow instability between two cylinders in 2D case V. V. Denisenko Institute for Aided Design RAS.
DNS of Surface Textures to Control the Growth of Turbulent Spots James Strand and David Goldstein The University of Texas at Austin Department of Aerospace.
Multimedia files Nos. 9.1 – 9.10 Chapter 9. Combustion features of the propane round and plane jet at the low Reynolds number The results of researches.
CE 1501 Flow Over Immersed Bodies Reading: Munson, et al., Chapter 9.
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 8: BOUNDARY LAYER FLOWS
A Numerical Solution to the Flow Near an Infinite Rotating Disk White, Section MAE 5130: Viscous Flows December 12, 2006 Adam Linsenbardt.
Chapter 3. Instability of the free plane and near – wall plane jet
Chapter 2. Physical processes responsible for evolution and downstream breakdown of a subsonic round jet Multimedia files Nos. 2.1 – 2.8 The results of.
The Stability of Laminar Flows
Chapter 7. Parabolic round jet in a shear cross flow Multimedia files Nos. 7.1 – 7.5 The results of researches presented in presentation are published.
Evolution of vorticity from the endwall boundary layer P M V Subbarao Professor Mechanical Engineering Department Methods to Estimate Enhanced Losses along.
Multimedia files -3/13 Instability of plane parallel flows Contents: 1.Canonical basic velocity profiles 2.Critical Reynolds numbers for the canonical.
Transition to Tubulence in the Hartmann Layer A. Thess 1, D.Krasnov 1, E. Zienicke 1, O. Zikanov 2, T. Boeck 3 1-Ilmenau University of Technology 2-University.
An experimental study of bypass transition in plane Couette flow S. AMALFI, F. LAADHARI & J. F. SCOTT Laboratoire de Mécanique des Fluides et d’Acoustique.
DNS of Surface Textures to Control the Growth of Turbulent Spots James Strand and David Goldstein The University of Texas at Austin Department of Aerospace.
Spatial Evolution of Resonant Harmonic Mode Triads in a Blasius Boundary Layer 37th AIAA Fluid Dynamics Conference and Exhibit José B. Dávila Department.
ROUTES TO TRANSITION IN SHEAR FLOWS Alessandro Bottaro with contributions from: S. Zuccher, I. Gavarini, P. Luchini and F.T.M. Nieuwstadt.
Date of download: 7/7/2016 Copyright © ASME. All rights reserved. From: Modal Stability TheoryLecture notes from the FLOW-NORDITA Summer School on Advanced.
Date of download: 11/12/2016 Copyright © ASME. All rights reserved. From: Laminar-Turbulent Transition in Magnetohydrodynamic Duct, Pipe, and Channel Flows.
Date of download: 9/27/2017 Copyright © ASME. All rights reserved.
Date of download: 10/1/2017 Copyright © ASME. All rights reserved.
Ship Hydrodynamics - Resistance
An Analytical Model for A Wind Turbine Wake
Master Thesis in Mechanical Engineering
Subject Name: FLUID MECHANICS
Fluid Dynamic Analysis of Wind Turbine Wakes
Introduction 1 - Separation 1.1 What is separation?
Chapter 5. About mechanism of origin and evolution of the coherent structures in the laminar and turbulent round jet The results of researches presented.
VORTICITY AND CIRCULATION WITHIN TWIN JETS ISSUING INTO A CROSSFLOW
Experimental techniques of the study of vortex structures caused by point injection on the leading edge of the oblique wing Tolkachev S.N. Gorev V.N. Zharkova.
Background Trapezoidal sharp-edged wings common in today’s fighter aircraft. Little understanding of aerodynamic effects at sweeping angles between 30°
Chapter 9 Analysis of a Differential Fluid Element in Laminar Flow
Presentation transcript:

Multimedia files – 10/13 Secondary instability of streamwise vortices in a 3D flow Contents: 1. Test model 2. Basic flow 3. Isolated vortices, mean flow 4. Isolated vortices, secondary oscillations 5. Interacting vortices, mean flow and secondary oscillations 6. Relevant publications

1. Test model Experimental model: plane view (a), elongated and circular roughness elements used for generation of the controlled stationary vortices (b) (see page of notes)

Mean-velocity distributions of the unperturbed boundary layer: velocity profiles measured in the upstream part of the model at x/c = 0.3 (left) and in the downstream sections of the wing (right); solid lines are Falkner–Skan–Cooke similarity solutions (see page of notes) 2. Basic flow

3. Isolated vortices, mean flow (I) Stationary boundary-layer disturbances generated by the elongated roughness element, amplitude levels are -6% (green) and +6% (yellow) of U 0 ; Vortex 1 (left) and Vortex 2 (right) (see page of notes)

Isosurfaces of the stationary disturbance of streamwise velocity U induced by Vortex 1 (bottom) and its cross section at x/c = 0.64 (top) 3. Isolated vortices, mean flow (II)

Secondary disturbances behind the elongated roughness element, amplitude levels are ± 0.5% (green and yellow) of U 0 : high-frequency perturbations with their maximum amplitudes u'/U 0 in the reference section x/c = 0.58 as high as 0.8 and 1.5% riding on Vortex 1 (left) and Vortex 2 (right) (see page of notes) 4. Isolated vortices, secondary oscillations (I)

Isosurfaces of the secondary oscillations riding on Vortex 1 behind of the elongated roughness element (bottom) and their cross section at x/c = 0.66 (top) 4. Isolated vortices, secondary oscillations (II)

A video clip by Chernoray V.G., Dovgal A.V., Kozlov V.V., Löfdahl L. (2005) 4. Isolated vortices, secondary oscillations (III) Click to play

Boundary layer perturbed by the circular roughness element: stationary disturbance (left) and secondary oscillations (right) with u'/U 0 = 0.4% at x/c = 0.58, amplitude levels are +1.2% and ± 0.1% of U 0, respectively (see page of notes) 5. Interacting vortices, mean flow and secondary oscillations

6. Relevant publications (I) Boiko A.V., Kozlov V.V., Sova V.A., Scherbakov V.A. (2000) Generation of streamwise structures in a boundary layer of a swept wing and their secondary instability. Thermophysics and Aeromechanics, 7, Carpenter A.L., Saric W.S., Reed H.L. (2009) Roughness receptivity studies in a 3-D boundary layerflight tests and computations. In Seventh IUTAM Symp. on Laminar–Turbulent Transition, Book of abstracts. Royal Institute of Technology, Stockholm, pp. 120–121. Chernoray V.G., Dovgal A.V., Kozlov V.V., Löfdahl L. (2005) Experiments on secondary instability of streamwise vortices in a swept-wing boundary layer. J. Fluid Mech., 534, Chernoray V.G., Dovgal A.V., Kozlov V.V., Löfdahl L. (2010) Secondary instability of a swept-wing boundary layer disturbed by controlled roughness elements. J. Visualization, 13(3), Deyhle H., Bippes H. (1996) Disturbance growth in an unstable three-dimensional boundary layer and its dependence on environmental conditions. J. Fluid Mech., 316, Elofsson P., Kawakami M., Alfredsson P. (1999) Experiments on the stability of streamwise streaks in plane Poiseuille flow. Phys. Fluids, 11, Fischer T.M., Dallmann U. (1991) Primary and secondary stability analysis of a three-dimensional boundary-layer flow. Phys. Fluids A, 3, Hoögberg M., Henningson D. (1998) Secondary instability of crossflow vortices in Falkner–Skan–Cooke boundary layers. J. Fluid Mech., 368, Janke E., Balakumar P. (2000) On the secondary instability of three-dimensional boundary layers. Theor. Comput. Fluid Dyn., 14, Kawakami M., Kohama Y., Okutsu M. (1999) Stability characteristics of stationary crossflow vortices in three- dimensional boundary layer. AIAA Paper Koch W. (2002) On the spatio-temporal stability of primary and secondary crossflow vortices in a three-dimensional boundary layer. J. Fluid Mech., 456, Koch W., Bertolotti F., Stolte A., Hein S. (2000) Nonlinear equilibrium solutions in a three-dimensional boundary layer and their secondary instability. J. Fluid Mech., 406,

6. Relevant publications (II) Koch W., Bertolotti F., Stolte A., Hein S. (2000) Nonlinear equilibrium solutions in a three-dimensional boundary layer and their secondary instability. J. Fluid Mech., 406, Kohama Y., Saric W., Hoos W. (1991) A high-frequency, secondary instability of crossflow vortices, that leads to transition. In Proc. RAS Conf. on Boundary-Layer and Control, Cambridge, Kohama Y., Onodera T., Egami Y. (1996) Design and control of crossflow instability field. In Duck P, Hall P (eds) IUTAM Symp. on Nonlinear Instability and Transition in Three-Dimensional Boundary Layers. Kluwer, Manchester, Kozlov V., Sova V., Scherbakov V. (2001) Experimental investigation of the development of secondary perturbations on a swept wing. Fluid Dyn., 36, Litvinenko Yu.A., Grek G.R., Kozlov V.V., Löfdahl L., Chernoray V.G. (2004) Experimental investigations of a streaky structure varicose instability in a swept wing boundary layer. Thermophisics and Aeromechanics, 11(1), Malik M., Li F., Choudhari M., Chang C.-L. (1999) Secondary instability of crossflow vortices and swept-wing boundary-layer transition. J. Fluid Mech., 399, Matsson O., Alfredsson P. (1990) Curvature- and rotation-induced instabilities in channel flow. J. Fluid Mech., 210, Matsubara M., Alfredsson P. (2001) Disturbance growth in boundary layers subjected to free-stream turbulence. J. Fluid Mech., 430, Nitschke-Kowsky P., Bippes H. (1988) Instability and transition of a three-dimensional boundary layer on a swept flat plate. Phys. Fluids, 31, Poll D.I.A. (1979) Transition in the infinite swept attachment line boundary layer. Aeronaut. Q, 30, Saric W., Reed H., White E. (2003) Stability and transition of three-dimensional boundary layers. Annu. Rev. Fluid Mech., 35, 413–440. Wassermann P., Kloker M. (2002) Mechanisms and passive control of crossflow-vortex-induced transition in a three- dimensional boundary layer. J. Fluid Mech., 456, White E., Saric W. (2005) Secondary instability of crossflow vortices. J. Fluid Mech., 525, White E., Saric W., Gladden R., Gabet P. (2001) Stages of swept-wing transition. AIAA Paper