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1 14 June 2011 14 June 2011 Session III (P2) Session III (P2) General Meeting of AERONET General Meeting of AERONET Polish Academy of Sciences Institute of Fluid Flow Machinery Piotr Doerffer Transonic flow control by streamwise vortices. Research offer Cooperation between science and aerospace industry 1) Start-up of research – EPFL first investigations and patent applic. 2) Research at Gdansk 3) Inclusion of AJVG into AITEB2 project (coord. RRD), patent applic. 4) Inclusion of AJVG into UFAST project (coord. IMP PAN) 5) Further research in the FACTOR project 6) New concept of RVG, patent applic., research projects 2001/3 2003/4 2005/9 2005/9 2010/1 3 2011/1 4
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Page 1: AJVG-Aeronet-2011.ppt

114 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Piotr DoerfferTransonic flow control by streamwise vortices.

Research offer

Cooperation between science and aerospace industry

1) Start-up of research – EPFL first investigations and patent applic.

2) Research at Gdansk

3) Inclusion of AJVG into AITEB2 project (coord. RRD), patent applic.

4) Inclusion of AJVG into UFAST project (coord. IMP PAN)

5) Further research in the FACTOR project

6) New concept of RVG, patent applic., research projects

2001/3

2003/4

2005/9

2005/9

2010/13

2011/14

Page 2: AJVG-Aeronet-2011.ppt

214 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

One of very important flow cases In transonic compressor cascades shock waves are formed

These shock waves interact with boundary layers and cause: -shock induced separation -unsteady effects of shock-boundary layer interaction

To limit these negative effects different flow control methods were tested, mainly for external aerodynamics

Page 3: AJVG-Aeronet-2011.ppt

314 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Reaearch idea from MIT ALSTOM Project for EPFL Lausanne

Transonic compressor blades are:

- very thin

- strong spanwise variation

Page 4: AJVG-Aeronet-2011.ppt

414 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Flow control concept – Stream-Wise Vortices (SV)Methods of SV Generation

Vane Vortex Generators Air Jet Vortex Generators

Page 5: AJVG-Aeronet-2011.ppt

514 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Test Model and Measurement Techniques

pressure measurement through wall taps

PSP – pressure sensitive paint schlieren visualisation of shock

system oil visualisation

EFMC 2003, Toulouse,

Shock Wave – Boundary Layer Interaction Control by Stream-Wise Vortices

Piotr Doerffer – IMP PAN, Gdansk, Poland

Albin Bölcs, Klaus Hubrich - EPFL, Lausanne, Switzerland

Page 6: AJVG-Aeronet-2011.ppt

614 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

20º 20º 20º 20º 20º

60° 60° 60° 60° 60° 60°

= 1 mm = 1 mm = 1 mm = 1 mm = 1 mm = 1 mm

= 0.4 mm = 0.4 mm

ALSTOM Patent

The Patent Application bears following data:

Our. Ref.: B03/172-0 DETitle of invention: Verfahren zur Verbesserung der Strömungsverhältnisse in einem Axialkompressor sowie Axialkompressor zur Durchführung des Verfahrens

Application No.: 103 55 108.5Filing Date: 24.11.2003

Legal Owner/Applicant: ALSTOM Technology Ltd,CH-5400 Baden

Page 7: AJVG-Aeronet-2011.ppt

714 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Own research at IMP PAN

0 540 X [mm]

Pivoted wall

Flat wall

Supply cavity

shock wave

Plate withthe AJVG

Location of AJVG

Traverse upstream the shock, 25 mm

Traverses downstream the shock, 30 and 55 mm

Measurement nozzle

Page 8: AJVG-Aeronet-2011.ppt

814 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Experimental investigations

Plate with the AJVG

VG holesStatic pressure holes

Main measurement:• Static pressure along the wall• Boundary layers in 3 traverses• Schlieren pictures• Oil visualisation• Oscillations of the shock wave

Mach numbers: 1.25, 1.35, 1.45, 1.55

Page 9: AJVG-Aeronet-2011.ppt

914 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Boundary layers 30 mm downstream

u/u_delta = F(y/y_delta), M=1.35

0.00

0.20

0.40

0.60

0.80

1.00

1.20

1.40

0 0.2 0.4 0.6 0.8 1

u/u_delta

y/y_

delta

BL for No JetsBL for Jets

u/u_delta = F(y/y_delta), M=1.45

0.00

0.20

0.40

0.60

0.80

1.00

1.20

1.40

0 0.2 0.4 0.6 0.8 1

u/u_delta

y/y_

delta

BL for No JetsBL forJets

Page 10: AJVG-Aeronet-2011.ppt

1014 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Shock wave oscillations

Power spectrum, M=1.35, Rear Shock

0.00

0.05

0.10

0.15

0.20

0.25

0 10 20 30 40 50 60

f [Hz]

Am

plitu

de

No JetsJets

RMS Rear shockM No Jets Jets

1.35 0.95473 0.79997

1.45 1.13944 1.02838

1.55 2.18671 1.97621

Main shock

Rear shock

Page 11: AJVG-Aeronet-2011.ppt

1114 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

AITEB-2

Coordinator RRD

Page 12: AJVG-Aeronet-2011.ppt

1214 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

pitch/chord = 1.11 pitch/chord = 1.13

Increased blade load – increased pitchGeometry: IGG Mesh:

Chord: 120 mm 208,288 cells (y+ ~1)Axial Chord: 76.1 mm Numerical scheme:Central Difference Scheme: SPARC, FINE2nd Order Upwind: FLUENTTurbulence model: Spalart-Almaras

Boundary conditions for pitch/chord =1.13:Inlet: Outlet:Total pressure 27983 Pa Static pressure 15840 Pa Total temperature 303.3 KInlet angle 48.6 degViscosity ratio 10

Page 13: AJVG-Aeronet-2011.ppt

1314 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Final adjustment of the shock location and smoothing of the blade shape

Page 14: AJVG-Aeronet-2011.ppt

1414 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Reference case experimental results

Maximum Mach number reached

Obtained reduction of M upstream of the shock

Smaller -foot in experiment

Same shock location

Page 15: AJVG-Aeronet-2011.ppt

1514 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Films with reference shock and with cooling and AJVG

Stabilisation of the shock wave

Page 16: AJVG-Aeronet-2011.ppt

1614 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Cooling + AJVG

oil visualisation

Page 17: AJVG-Aeronet-2011.ppt

1714 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

y= f(PP/P0), X=128, Theta=45 alfa=90

02468

101214161820

0.45 0.55 0.65 0.75 0.85 0.95

PP/P0

y [m

m]

reference Shock X=114Cooling on VG off Shock X=114Cooling on VG on Shock X=114

y= f(PP/P0), X=171, Theta=45 alfa=90

02468

101214161820

0.45 0.55 0.65 0.75 0.85 0.95

PP/P0y

[mm

]

reference Shock X=114Cooling on VG off Shock X=114Cooling on VG on Shock X=114

Stagnation pressure

Application of cooling increases b.l. thickness considerablyAJVG decreases the effect

X = 128 X = 171

Page 18: AJVG-Aeronet-2011.ppt

1814 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Objective function: maximum of vorticity X-component at the section 50mm downstream of the jet

Variables: jet skew angles „alfa” jet pitch angles „theta”

Optimisation of AJVG parameters

Page 19: AJVG-Aeronet-2011.ppt

1914 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

The invention submission EM 70518 by Rolls-Royce

dated 04th December 2008,

Title: “Method and apparatus to passively control flow separation on turbine airfoils by means of streamwise vortices generated by air jets”

Page 20: AJVG-Aeronet-2011.ppt

2014 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Project starting date: 1st of December, 2005

Project duration: 3,5 years

Unsteady effects of shock wave induced separation

Coordinated by IMP PAN

Page 21: AJVG-Aeronet-2011.ppt

2114 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Interaction types considered in UFAST:

Transonic interaction Nozzle flow Oblique shock reflection

Possibly wide representation of characteristic physical cases

of shock wave boundary layer interaction

Page 22: AJVG-Aeronet-2011.ppt

2214 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

No. Participant name Short name1 Institute of Fluid Flow Machinery, Gdansk

PLIMP PAN

2 CNRS Lab. IUSTI, UMR 6595, Marseille F IUSTI3 ONERA: ( DAFE, DAAP) F ONERA4 University of Cambridge, Dept. of Engineering UK UCAM-DENG5 Queens University Belfast, School of Aero. Eng. UK QUB6 Russian Academy of Science, Siberian Branch,

Novosibirsk, Inst. of Theor. App. Mech. RUSITAM

7 Delft University of Technology, Aerodyn. Lab. NL TUD8 INCAS, Romanian Institute for Aeronautics RO INCAS9 University of Southampton, (SES) UK SOTON

10 University of Rome "La Sapienza", I URMLS11 University of Liverpool, Dept. of Aero. Engin. UK LIV12 NUMECA, Belgium, SME B NUMECA14 Institute Mécanique des Fluides de Toulouse F IMFT16 FORTH/IACM, Found. for Res. and Techn.-Hellas GR FORTH17 Ecole Centrale de Lyon F LMFA19 EADS-M, Deutschland GmbH Military Aircraft D EADS-M20 Institute of Aviation, Warsaw PL IoA

Large tunnels

Large tunnels

SME

New partnerUkraine

CFD

IND

Page 23: AJVG-Aeronet-2011.ppt

2314 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Observer Name

1 Rolls-Royce Germany, RRD

2 Dassault Aviation

3 Alenia

4 Ansys Germany GmbH

Observer Group

Page 24: AJVG-Aeronet-2011.ppt

2414 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

PM=638

Transonic interaction Channel flow Shock reflection

Page 25: AJVG-Aeronet-2011.ppt

2514 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

ALTERNATIVE SOLUTION TO AJVG ALTERNATIVE SOLUTION TO AJVG

STREAMWISE VORTICITY CONTOURS

MEMS – sub-layer device ~ δ1

Rod Vortex Generator

Page 26: AJVG-Aeronet-2011.ppt

2614 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Full Aero-thermal Combustor-Turbine interactiOn ResearchFACTOR

Zastosowanie AJVG w gorącym środowisku

2010 - 2013

Page 27: AJVG-Aeronet-2011.ppt

2714 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

Laminar – turbulent transition effects on unsteady behaviour

of shock wave induced separation

New project topic:

UFAST TUFAST SWIFT?Przemysł: Dassault Aviation, Rolls-Royce Germany,

AVIO, AIRBUS

Page 28: AJVG-Aeronet-2011.ppt

2814 June 201114 June 2011 – – Session III (P2)Session III (P2)

General Meeting of AERONET General Meeting of AERONET

Polish Academy of SciencesInstitute of Fluid Flow Machinery

THE PEOPLE PROGRAMME – Marie-Curie

Industry-Academia Partnerships and PathwaysSTA-DY-WI-CO (LMS Belgium - IMP PAN Poland)

STAtic and DYnamic piezo-driven StreamWIse vortexgenerators for active flow Control

Initial Training NetworksIMESCON

Innovative MEthods of Separated Flow CONtrol in Aeronautics


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