samlerapport deepwind 2013
TRANSCRIPT
-
8/15/2019 Samlerapport DeepWind 2013
1/274
SINTEF Energy Research Electric Power Systems 2013 ‐06 ‐28
TR A7307 ‐ Unrestricted
Report
Deep Sea Offshore Wind R&D Conference 24 – 25 January 2013 Royal Garden Hotel, Trondheim
Author: John Olav Tande (editor)
-
8/15/2019 Samlerapport DeepWind 2013
2/274
-
8/15/2019 Samlerapport DeepWind 2013
3/274
PROJECT NO. 12X650
REPORT NO. TR A7307
VERSION 1.0
Document history VERSION DATE VERSION DESCRIPTION
1.0 2013 ‐06 ‐28
-
8/15/2019 Samlerapport DeepWind 2013
4/274
PROJECT NO. 12X650
REPORT NO. TR A7307
VERSION 1.0
Table of contents
1 Detailed Programme ........................................................................................................................ 6
2 List of Participants ............................................................................................................................ 9
3 Scientific Committee and Conference Chairs ................................................................................... 13
PRESENTATIONS
Opening session – Frontiers of Science and Technology Innovations in offshore wind technology, John Olav Tande, SINTEF/NOWITECH............................................................... 15Key research topics in offshore wind energy, Kristin Guldbrandsen Frøysa, CMR/NORCOWE............................................ 19Research at Alpha Ventus deep offshore wind farm, Stefan Faulstich, Fh IWES ..................................................................... 24WindFloat deep offshore wind operational experience, Pedro Valverde, EdP ......................................................................... 28HyWind deep offshore wind operational experience, Finn Gunnar Nielsen, Statoil................................................................. 32
A1 New turbine technologyDesign Optimization of a 5 MW Floating Offshore Vertical Axis WindTurbine, Uwe Schmidt Paulsen,Technical Uni of Denmark, DTU.............................................................................................................................................. 37Operational Control of a Floating Vertical Axis Wind Turbine, Harald Svendsen, SINTEF Energi AS................................. 44Control for Avoiding Negative Damping on Floating Offshore Wind Turbine, Prof Yuta Tamagawa, Uni. of Tokyo..... ..... 47Towards the fully-coupled numerical modelling of floating wind turbines, Axelle Viré, Imperial College, London..... ...... . 49Geometric scaling effects of bend-twist coupling in rotor blades, Kevin Cox, PhD stud, NTNU.......................................... 52
A2 New turbine technologyHigh Power Generator for Wind Power Industry: A Review, Zhaoqiang Zhang, PhD stud, NTNU..................................... 56Superconducting Generator Technology for Large Offshore Wind Turbines, Niklas Magnusson, SINTEF Energi AS..... . 60Laboratory Verification of the Modular Converter for a 100 kV DC Transformer-less Offshore Wind Turbine Solution,Sverre Gjerde, PhD stud, NTNU............................................................................................................................................ 63Multi-objective Optimization of a Modular Power Converter Based on Medium Frequency AC-Linkfor Offshore DC Wind Park, Rene A. Barrera, NTNU ................................................................................... ....................... 66
B1 Power system integrationWind Turbine Electrical Design for an Offshore HVDC Connection, Olimpo Anaya-Lara, Strathclyde Univ..... ..... ...... .... 73Frequency Quality in the Nordic system: Offshore Wind variability, Hydro Power Pump Storage and usage ofHVDC Links, Atsede Endegnanew, SINTEF Energi AS....................................................................................................... 78Coordinated control for wind turbine and VSC-HVDC transmission to enhance FRT capability, A. Luque,Uni. Strathclyde............................................................................................................................ ........................................... 81
North Sea Offshore Modeling Schemes with VSC-HVDC Technology: Control and Dynamic Performance Assessment,K. Nieradzinska, University of Strathclyde.......................................................................................................... ................... 84Upon the improvement of the winding design of wind turbine transformers for safer performance withinresonance overvoltages, Amir H Soloot, PhD, NTNU ......................................................................................... .................. 89
B2 Grid connectionPlanning Tool for Clustering and Optimised Grid Connection of Offshore Wind Farms, Harald G. Svendsen, SINTEF .... 93The role of the North Sea power transmission in realising the 2020 renewable energy targets - Planning and
permitting challenges, Jens Jacob Kielland Haug, SINTEF Energi AS.................................................................................. 96Technology Qualification of Offshore HVDC Technologies, Tore Langeland, DNV KEMA.............................................. 98Evaluating North Sea grid alternatives under EU’s RES-E targets for 2020, Ove Wolfgang, SINTEF Energi AS............... 104
-
8/15/2019 Samlerapport DeepWind 2013
5/274
PROJECT NO. 12X650
REPORT NO. TR A7307
VERSION 1.0
C1 Met-ocean conditionsWave-induce characteristics of atmospheric turbulence flux measurements, Mostafa Bakhoday Paskyabi, UiB.... ...... ...... .. 113Experimental characterization of the marine atmospheric boundary layer in the Havsul area, Norway,Constantinos Christakos, UiB....................................................................................................................................... ........... 118Buoy based turbulence measurements for offshore wind energy applications, M. Flügge, UiB ........................................... 121Effect of wave motion on wind lidar measurements - Comparison testing with controlled motion applied,Joachim Reuder, Univ of Bergen ................................................................................................ ........................................... 123Turbulence analysis of LIDAR wind measurements at a wind park in Lower Austria, Valerie-Marie Kumer, UiB ...... ...... 127
C2 Met-ocean conditionsWave driven wind simulations with CFD, Siri Kalvig, University of Stavanger / StormGeo .............................................. 133
New two-way coupled atmosphere-wave model system for improved wind speed and wave height forecasts,Olav Krogsæter, StormGeo / University of Bergen................................................................................................................ 136Measurement of wind profile with a buoy mounted lidar, Jan-Petter Mathisen, Fugro OCEANOR (presentation) ............... 142Measurement of wind profile with a buoy mounted lidar, Jan-Petter Mathisen, Fugro OCEANOR (paper)........................ 145 .
Numerical Simulation of Stationary Microburst Phenomena with Impinging Jet Model, Tze Siang Sim,
Nanyang Technological University ........................................................................................................... ........................... 155
Posters presentations .Magnetically Induced Vibration Forces in a Low-Speed Permanent Magnet Wind Generator with Concentrated Windings,Mostafa Valavi, PhD stud, NTNU.......................................................................................................................................... 161Stability in offshore wind farm with HVDC connection to mainland grid, Jorun I Marvik, SINTEF Energi AS................. 162A Markov Weather Model for O&M Simulation of Offshore Wind Parks, Brede Hagen, stud, NTNU............................... 163Turbulence Analysis of LIDAR Wind Measurements at a Wind Park in Lower Austria, Valerie-Marie Kumer, UiB..... .... 164Investigation of droplet erosion for offshore wind turbine blade, Magnus Tyrhaug, SINTEF.............................................. 165
NOWIcob – A tool for reducing the maintenance costs of offshore wind farms, Iver Bakken Sperstad, SINTEF Energi AS... 166Methodology to design an economic and strategic offshore wind energy Roadmap in Portugal, Laura Castro-Santos,Laboratório Nacional de Energia (LNEG) (poster) ................................................................................................................. 167Methodology to design an economic and strategic offshore wind energy Roadmap in Portugal, Laura Castro-Santos,Laboratório Nacional de Energia (LNEG) ( paper) ................................................................................................................. 168Methodology to study the life cycle cost of floating offshore wind farms, Laura Castros Santos,Laboratório Nacional de Energia (LNEG ) (poster) ............................................................................................................... 178Methodology to study the life cycle cost of floating offshore wind farms, Laura Castros Santos,Laboratório Nacional de Energia (LNEG ) (paper) ................................................................................................................ 179Two-dimensional fluid-structure interaction of airfoil, Knut Nordanger, PhD stud, NTNU ................................................. 187Experimental Investigation of Wind Turbine Wakes in the Wind Tunnel, Heiner Schümann, NTNU ................................. 188
Numerical Study on the Motions of the VertiWind Floating Offshore Wind Turbine, Raffaello Antonutti, EDF R&D ...... 189Coatings for protection of boat landings against corrosion and wear, Astrid Bjørgum, SINTEF Materials and Chemistry .. 190
Numerical model for Real-Time Hybrid Testing of a Floating Wind Turbine, Valentin CHABAUD, PhD stud, NTNU ... 191Advanced representation of tubular joints in jacket models for offshore wind turbine simulation,Jan Dubois, ForWind – Leibniz University Hannover ........................................................................................................... 192Comparison of coupled and uncoupled load simulations on the fatigue loads of a jacket support structure,Philipp Haselbach, DTU Wind Energy .................................................................................................................................. 193
Design Standard for Floating Wind Turbine Structures, Anne Lene H. Haukanes, DNV .................................................... 194 Nonlinear irregular wave forcing on offshore wind turbines. Effects of soil damping and wave radiation damping inmisaligned wind and waves, Signe Schløer, DTU ..................................................................................................... ........... 195
D Operation & maintenanceDevelopment of a Combined Operational and Strategic Decision Support Model for Offshore Wind,Iain Dinwoodie, PhD Stud, Univ Strathclyde ........................................................................................................................ 197Vessel fleet size and mix analysis for maintenance operations at offshore wind farms, Elin E. Halvorsen-Weare,SINTEF ICT/MARINTEK .......................................................................................................... .......................................... 200
NOWIcob – A tool for reducing the maintenance costs of offshore wind farms, Iver Bakken Sperstad, SINTEF .............. 203WINDSENSE – a joint development project for add-on instrumentation of Wind Turbines, Oddbjørn Malmo,Kongsberg Maritime AS .................................................................................................................................................. ...... 207Long-term analysis of gear loads in fixed offshore wind turbines considering ultimate operational loadings,Amir Rasekhi Nejad, PhD stud, NTNU ............................................................................................................................... 211
-
8/15/2019 Samlerapport DeepWind 2013
6/274
PROJECT NO. 12X650
REPORT NO. TR A7307
VERSION 1.0
E Installation & sub-structuresStructures of offshore converter platforms - Concepts and innovative developments, Joscha Brörmann,Technologiekontor Bremerhaven GmbH ............................................................................................................................ 216Dynamic analysis of floating wind turbines during pitch actuator fault, grid loss, and shutdown,Erin E. Bachynski, PhD stud, NTNU .................................................................................................................. ................ 219Use of a wave energy converter as a motion suppression device for floating wind turbines, Michael Borg,Cranfield University .............................................................................................................................. .............................. 223Loads and response from steep and breaking waves. An overview of the ‘Wave loads’ project,Henrik Bredmose, Associate Professor, DTU Wind Energy ............................................................................................... 226Effect of second-order hydrodynamics on floating offshore wind turbines, Line Roald, ETH Zürich ............................... 235
F Wind farm modellingWind farm optimization, Prof Gunner Larsen, DTU Wind Energy ..................................................................................... 239Blind test 2 - Wind and Wake Modelling, Prof Lars Sætran, NTNU ................................................................................... 245A practical approach in the CFD simulations of off-shore wind farms through the actuator disc technique,Giorgio Crasto, WindSim AS ................................................................................................................................................ 250
3D hot-wire measurements of a wind turbine wake, Pål Egil Eriksen, PhD stud, NTNU .................................................... 255 Near and far wake validation study for two turbines in line, Marwan Khalil, GexCon AS ............................................... 258
Closing sessionDeep offshore and new foundation concepts, Arapogianni Athanasia, European Wind Energy Association ...... ...... ...... ... 262Optimal offshore grid development in the North Sea towards 2030, Daniel Huertas Hernando, SINTEF Energi AS ...... .. 265
New turbine technology, Svein Kjetil Haugset, Blaaster (no presentation available)
-
8/15/2019 Samlerapport DeepWind 2013
7/274
DeepWind 2013 - 10 th Deep Sea Offshore Wind R&D Conference24 - 25 January 2013, Royal Garden Hotel, Kjøpmannsgata 73, Trondheim, NORWAY
Thursday 24 January 09.00 Registration & coffee
Opening session – Frontiers of Science and Technology Chairs: John Olav Tande, SINTEF/NOWITECH and Trond Kvamsdal, NTNU/NOWITECH
09.30 Opening and welcome by chair 09.40 Innovations in offshore wind technology , John Olav Tande, SINTEF/NOWITECH
10.05 Key research topics in offshore wind energy, Kristin Guldbrandsen Frøysa, CMR/NORCOWE 10.30 Research at Alpha Ventus deep offshore wind farm, Stefan Faulstich, Fh IWES11.00 WindFloat deep offshore wind operational experience , Pedro Valverde, EdP 11.30 HyWind deep offshore wind operational experience , Finn Gunnar Nielsen, Statoil11.55 Closing by chair 12.00 Lunch
Parallel sessions A1) New turbine technologyChairs: Michael Muskulus, NTNU Prof Gerard van Bussel, TU Delft
B1) Power system integrationChairs: Prof Kjetil Uhlen, NTNU Prof Olimpo Anaya ‐Lara, Strathclyde Uni
C1) Met ‐ocean conditionsChairs: Prof J Reuder, Uni of Bergen Erik Berge, Kjeller Vindteknikk
13.00 Introduction by Chair Introduction by Chair Introduction by Chair13.10 Design Optimization of a 5 MW
Floating Offshore Vertical Axis Wind Turbine , Uwe Schmidt Paulsen, Technical Uni of Denmark, DTU
Wind Turbine Electrical Design for an Offshore HVDC Connection , Olimpo Anaya ‐Lara, Strathclyde Univ.
Wave ‐induce characteristics of atmospheric turbulence flux measurements , Mostafa Bakhoday Paskyabi, UiB
13.40 Operational Control of a Floating Vertical Axis Wind Turbine , Harald Svendsen, SINTEF Energi AS
Frequency Quality in the Nordic system: Offshore Wind variability, Hydro Power Pump Storage and usage of HVDC Links, Atsede Endegnanew, SINTEF Energi AS
Experimental characterization of the marine atmospheric boundary layer in the Havsul area, Norway , Constantinos Christakos, UiB
14.00 Control for Avoiding Negative Damping on Floating Offshore Wind Turbine, Prof Yuta Tamagawa, Uni. of Tokyo
Coordinated control for wind turbine and VSC ‐HVDC transmission to enhance FRT capability , A. Luque, Uni. Strathclyde
Buoy based turbulencemeasurements for offshore wind energy applications , M. Flügge, UiB
14.20 Towards the fully ‐coupled numerical modelling of floating wind turbines ,
Axelle Viré, Imperial College, London
North Sea Offshore Modeling Schemes with VSC ‐HVDC Technology: Control and Dynamic Performance Assessment , K. Nieradzinska, University of Strathclyde
Effect of wave motion on wind lidar measurements ‐ Comparison testing with controlled motion applied , Joachim Reuder, Univ of Bergen
14.40 Geometric scaling effects of bend ‐twist coupling in rotor blades , Kevin Cox, PhD stud, NTNU
Upon the improvement of the winding design of wind turbine transformers for safer performance within resonance overvoltages , Amir H Soloot, PhD, NTNU
Turbulence analysis of LIDAR wind measurements at a wind park in Lower Austria , Valerie ‐Marie Kumer, UiB
15.00 Refreshments A2) New turbine technology Chairs: Michael Muskulus Prof Gerard van Bussel, TU Delft
B2) Grid connectionChairs: Prof Kjetil Uhlen, NTNU Prof Olimpo Anaya ‐Lara, Strathclyde Uni
C2) Met ‐ocean conditionsChairs: J Reuder, Uni of Bergen Erik Berge, Kjeller Vindteknikk
15.30 Introduction by Chair Introduction by Chair Introduction by Chair15.35 High Power Generator for Wind Power
Industry: A Review, Zhaoqiang Zhang, PhD stud, NTNU
Planning Tool for Clustering and Optimised Grid Connection of Offshore Wind Farms, Harald G. Svendsen, SINTEF
Wave driven wind simulations with CFD, Siri Kalvig, University of Stavanger / StormGeo
15.55 Superconducting Generator Technology for Large Offshore Wind Turbines, Niklas Magnusson, SINTEF Energi AS
The role of the North Sea power transmission in realising the 2020 renewable energy targets ‐ Planning and permitting challenges , Jens Jacob Kielland Haug, SINTEF Energi AS
New two ‐way coupled atmosphere ‐wave model system for improved wind speed and wave height forecasts , Olav Krogsæter, StormGeo / University of Bergen
16.15 Laboratory Verification of the Modular Converter for a 100 kV DC Transformer ‐less Offshore Wind Turbine Solution , Sverre Gjerde, PhD stud, NTNU
Technology Qualification of Offshore HVDC Technologies , Tore Langeland, DNV KEMA
Measurement of wind profile with a buoy mounted lidar , Jan ‐Petter Mathisen, Fugro OCEANOR
16.35 Multi ‐objective Optimization of a Modular Power Converter Based on Medium Frequency AC ‐Link for Offshore DC Wind Park , Rene A. Barrera, NTNU
Evaluating North Sea grid alternatives under EU’s RES‐E targets for 2020 , Ove Wolfgang, SINTEF Energi AS
Numerical Simulation of Stationary Microburst Phenomena with Impinging Jet Model , Tze Siang Sim, Nanyang Technological University
16.55 Closing by Chair Closing by Chair Closing by Chair 17.00 Poster session with refreshments 19.00 Dinner
6
-
8/15/2019 Samlerapport DeepWind 2013
8/274
Thursday 24 January 17.00 Poster Session with refreshments
1. Aeroelastc analysis software as a teaching and learning tool for young and old students of wind turbines, Paul E. Thomassen, NTNU
2. Magnetically Induced Vibration Forces in a Low ‐Speed Permanent Magnet Wind Generator with Concentrated Windings, Mostafa Valavi, PhD stud, NTNU
3. Coupled 3D Modelling of Large ‐Diameter Ironless PM Generator , Zhaoqiang Zhang, PhD stud, NTNU 4. Stability in offshore wind farm with HVDC connection to mainland grid, Jorun I Marvik, SINTEF Energi AS 5. Perturbation in the acoustic field from a large offshore wind farm in the presence of surface gravity waves, Mostafa
Bakhoday Paskyabi, UiB 6. Autonomous Turbulence Measurements from a Subsurface Moored Platform, Mostafa Bakhoday Paskyabi, UiB 7. A Markov Weather Model for O&M Simulation of Offshore Wind Parks, Brede Hagen, stud, NTNU 8. Turbulence Analysis of LIDAR Wind Measurements at a Wind Park in Lower Austria, Valerie ‐Marie Kumer, UiB 9. Investigation of droplet erosion for offshore wind turbine blade, Magnus Tyrhaug, SINTEF 10. A Fuzzy FMEA Risk Assessment Approach for Offshore Wind Turbines, Fateme Dinmohammadi, Islamic Azad University 11. NOWIcob – A tool for reducing the maintenance costs of offshore wind farms, Iver Bakken Sperstad, SINTEF Energi AS 12. Long ‐term analysis of gear loads in fixed offshore wind turbines considering ultimate operational loadings, Amir
Rasekhi Nejad, PhD, NTNU 13. Methodology to design an economic and strategic offshore wind energy Roadmap in Portugal, Laura Castro ‐Santos,
Laboratório Nacional de Energia (LNEG) 14. Methodology to study the life cycle cost of floating offshore wind farms, Laura Castros Santos,Laboratório Nacional de
Energia (LNEG) 15. Two ‐dimensional fluid ‐structure interaction of airfoil , Knut Nordanger, PhD stud, NTNU 16. Experimental Investigation of Wind Turbine Wakes in the Wind Tunnel , Heiner Schümann, NTNU 17. Numerical Study on the Motions of the VertiWind Floating Offshore Wind Turbine, Raffaello Antonutti, EDF R&D 18. Coatings for protection of boat landings against corrosion and wear , Astrid Bjørgum, SINTEF Materials and Chemistry 19. Analysis of spar buoy designs for offshore wind turbines, C. Romanò, DIMEAS, Politecnico di Torino 20. Numerical model for Real ‐Time Hybrid Testing of a Floating Wind Turbine, Valentin CHABAUD, PhD stud, NTNU 21. Advanced representation of tubular joints in jacket models for offshore wind turbine simulation, Jan Dubois, ForWind –
Leibniz University Hannover 22. Comparison of coupled and uncoupled load simulations on the fatigue loads of a jacket support structure, Philipp
Haselbach, DTU Wind Energy 23. Design Standard for Floating Wind Turbine Structures , Anne Lene H. Haukanes, DNV
24.
Nonlinear irregular
wave
forcing
on
offshore
wind
turbines.
Effects
of
soil
damping
and
wave
radiation
damping
in
misaligned wind and waves, Signe Schløer, DTU
19.00 Dinner
7
-
8/15/2019 Samlerapport DeepWind 2013
9/274
DeepWind 2013 - 10 th Deep Sea Offshore Wind R&D Seminar
24-25 January 2013, Royal Garden Hotel, Kjøpmannsgata 73, Trondheim, NORWAY Friday 25 January
Parallel sessions D) Operations & maintenance Chairs: Matthias Hofmann, SINTEF Stefan Faulstich, Fh IWES
E) Installation & sub ‐structuresChairs: Hans ‐Gerd Busmann, Fh IWES Jørgen Krogstad, Statkraft
F) Wind farm modellingChairs: Prof Trond Kvamsdal, NTNU Thomas Buhl, DTU Wind Energy
08.30 Introduction by Chair Introduction by Chair Introduction by Chair08.35 Development of a Combined Operational and Strategic Decision Support Model for Offshore Wind, Iain Dinwoodie, PhD Stud, Univ Strathclyde
Structures of offshore converter platforms ‐ Concepts and innovative developments , Joscha Brörmann, Technologiekontor Bremerhaven GmbH
Wind farm optimization , Prof Gunner Larsen, DTU Wind Energy
09.05 Vessel fleet size and mix analysis for maintenance operations at offshore wind farms , Elin E. Halvorsen ‐Weare, SINTEF ICT/MARINTEK
Dynamic analysis of floating wind turbines during pitch actuator fault, grid loss, and shutdown , Erin E. Bachynski, PhD stud, NTNU
Blind test 2 ‐ Wind and WakeModelling , Prof Lars Sætran, NTNU
09.25 NOWIcob – A tool for reducing the maintenance costs of offshore wind
farms, Iver Bakken Sperstad, SINTEF
Use of a wave energy converter as a motion suppression device for floating
wind turbines , Michael Borg, Cranfield University
A practical approach in the CFD simulations of off ‐shore wind farms
through the actuator disc technique , Giorgio Crasto, WindSim AS 09:45 WINDSENSE – a joint development
project for add ‐on instrumentation of Wind Turbines , Oddbjørn Malmo, Kongsberg Maritime AS
Loads and response from steep and breaking waves. An overview of the ‘Wave loads’ project, Henrik Bredmose, Associate Professor, DTU Wind Energy
3D hot ‐wire measurements of a wind turbine wake , Pål Egil Eriksen, PhD stud, NTNU
10:05 Long ‐term analysis of gear loads in fixed offshore wind turbines considering ultimate operational loadings, Amir Rasekhi Nejad, PhD stud, NTNU
Effect of second ‐order hydrodynamics on floating offshore wind turbines , Line Roald, ETH Zürich
Near and far wake validation study for two turbines in line , Marwan Khalil, GexCon AS
10.35 Closing by Chair Closing by Chair Closing by Chair
10.40 Refreshments Closing session – Strategic Outlook Chairs: John Olav Tande, SINTEF/NOWITECH and Michael Muskulus, NTNU/NOWITECH
11.00 Introduction by Chair 11.05 Deep offshore and new foundation concepts , Arapogianni Athanasia, European Wind Energy Association 11.35 Optimal offshore grid development in the North Sea towards 2030, Daniel Huertas Hernando, SINTEF Energi AS12.05 New turbine technology , Svein Kjetil Haugset, Blaaster 12.35 Poster award and closing 13.00 Lunch
8
-
8/15/2019 Samlerapport DeepWind 2013
10/274
List of participants
Name
Institution
Anaya‐Lara, Olimpo Strathclyde University
Antonutti, Raffaello EDF R&D LNHEArapogianni, Athanasia European Wind Energy AssociationBachynski, Erin CeSOS/NTNU
Bardal, Lars Morten NTNUBarrera ‐Cardenas, Rene Alexander NTNUBerge, Erik Kjeller VindteknikkBergh, Øivind Institute of Marine ResearchBjørgum, Astrid SINTEF Materials and ChemistryBolleman, Nico Blue H Engineering BVBorg, Michael Cranfield UniversityBredmose, Henrik DTU Wind EnergyBrörmann, Joscha Teknologiekontor BremerhavenBuhl, Thomas DTU Wind EnergyBusmann, Hans‐Gerd Fraunhofer IWESCastro Santos, Laura University of A CoruñaChabaud, Valentin NTNUChristakos, Konstantinos University of Bergen
Cox, Kevin NTNUCrasto, Giorgio WindSim ASDe Laleu, Vincent EDF R&Dde Vaal, Jabus NTNUDelhaye, Virgile SINTEF M&C
Deng, Han NTNUDinwoodie, Iain University of StrathclydeDubois, Jan Leibniz Universitaet Hannover Stahlbau
Dufourd, Frederic EDFEecen, Peter ECNEgeland, Håkon Statkraft Energi ASEndegnanew, Atsede SINTEF Energi ASEriksen, Pål Egil NTNUEriksson, Kjell Det Norske VeritasFaulstich, Stefan Fh IWESFlügge, Martin University of Bergen
9
-
8/15/2019 Samlerapport DeepWind 2013
11/274
Fredriksen, Tommy HiT
Frøyd, Lars 4Subsea ASFrøysa, Kristin Gulbrandsen NORCOWE / CMRGao, Zhen CeSOS/NTNUGjerde, Sverre Skalleberg NTNUGrønsleth, Martin Kjeller Vindteknikk ASHaarr, Geirr Statoil HywindHagen, Brede NTNUHalvorsen‐Weare, Elin Espeland SINTEF IKTHaselbach, Philipp Ulrich DTU Wind Energy
Haugset, Svein Kjetil ChapdriveHofmann, Matthias SINTEF EnergiHopstad, Anne Lene DNVHuertas Hernando, Daniel SINTEF EnergiIversen, Viggo ProneoJakobsen, Tommy Kongsberg MaritimeJohnsen, Trond MARINTEK ASKalvig, Siri Storm GeoKamio, Takeshi The University of TokyoKarlsson, Sara Hexicon AB
Kastmann, Pål Arne Innovation Norway / Norwegian Embassy in Beijing Khalil, Marwan GexCon ASKielland Haug, Jens Jakob SINTEF EnergiKjerstad, Einar Fiskerstrand BLRT
Kocewiak, Lukasz DONG Energy Wind PowerKorpås, Magnus SINTEF EnergiKrogsæter, Olav Storm GeoKrokstad, Jørgen StatkraftKumer, Valerie‐Marie University of BergenKvamme, Cecilie Institute of Marine ResearchKvamsdal, Trond NTNUKvittem, Marit Irene CeSOS/NTNULangeland, Tore DNVLarsen, Gunner DTU Wind EnergyLauritzen, Tore Lennart Access Mid‐NorwayLjøkelsøy, Kjell SINTEF EnergiLund, Berit Floor Kongsberg MaritimeLund,Per Christer Norwegian Embassy in TokyoLunde, Knut‐Ola NTNU
Luque, Antonio University of StrathclydeLynum, Susanne NTNU
10
-
8/15/2019 Samlerapport DeepWind 2013
12/274
Magnusson, Niklas SINTEF Energi
Malmo, Oddbjørn Kongsberg MaritimeManger, Eirik Acona Flow TechnologyMartinussen, Mads BlaasterMarvik, Jorun SINTEF EnergiMathisen, Jan‐Petter Fugro OCEANORMidtsund, Tarjei Statnett SFMuskulus, Michael NTNUNatarajan, Anand DTU Wind EnergyNejad, Amir R. NTNUNiedzwecki, John Texas A/M UniversityNieradzinska, Kamila Strathclyde UniversityNilsen, Finn Gunnar Statoil ASANodeland, Anne Mette NTNUNordanger, Knut NTNUNysveen, Arne NTNU/ElkraftteknikkOggiano, Luca IFEOma, Per Norman Kongsberg Maritime ASOng, Muk Chen MARINTEKPaskyabi, Mostafa Bakhoday Geophysical Institute/NORCOWE
Paulsen, Uwe Schmidt DTU Wind EnergyRebours, Yann EDF R&DReuder, Joachim UiBRoald, Line ETH Zürich
Schaumann, Peter Leibniz Universitaet Hannover Stahlbau
Schløer, Signe DTU Wind EnergySchramm, Rainer Subhydro ASSchümann, Heiner NTNUSeterlund, Anne Marie Statkraft DevelopmentSim, Tze Siang Nanyang Technological UniversitySingstad, Ivar Innovation Norway
Skaare, Bjørn Statoil ASASoloot, Amir Hayati NTNU
Sperstad, Iver Bakken SINTEF EnergiStenbro, Roy IFESvendgård, Ole VIVA ‐ Testsenter for vindturbinerSvendsen, Harald SINTEF EnergiSæter, Camilla NTNUSætran, Lars NTNU
Sørheim, Hans Roar CMRTamagawa, Yuta Tokyo University
11
-
8/15/2019 Samlerapport DeepWind 2013
13/274
Tande, John Olav SINTEF Energi
Thomassen, Paul NTNUTveiten, Bård Wathne SINTEF
Tyrhaug, Magnus NTNUUhlen, Kjetil NTNUUndeland, Tore NTNUValverde, Pedro EDP Inovação, S.A.
van Bussel, Gerard TU DelftVan Der Pal, Aart ECNVire, Axelle Imperial College LondonWolfgang, Ove SINTEF EnergiZhang, Zhaoqiang NTNUØstbø, Niels Peter SINTEF ICTÖfverström, Anders Hexicon ABØyslebø, Eirik Norges vassdrags ‐ og energidirektorat
12
-
8/15/2019 Samlerapport DeepWind 2013
14/274
PROJECT NO. 12X650
REPORT NO. TR A7307
VERSION 1.0
3 Scientific Committee and Conference Chairs
An international Scientific Committee was established with participants from leading research institutes anduniversities for reviewing submissions and preparing the conference programme. The members of theScientific Committee of DeepWind'2013 are listed below.
Anaya-Lara, Olimpo, Strathclyde UniversityBerge, Erik, Kjeller VindteknikkBuhl, Thomas, DTUBusmann, Hans-Gerd, Fraunhofer IWESBussel, Gerard J.W. van, TU DelftFaulstich, Stefan, Fraunhofer IWESKrokstad, Jørgen, StatkraftKvamsdal, Trond, NTNULangen, Ivar, UiSLeithead, William, Strathclyde UniversityMadsen, Peter Hauge, DTUMoan, Torgeir, NTNUMolinas, Marta, NTNUMuskulus, Michael, NTNU
Nielsen, Finn Gunnar, Statoil Nygaard, Tor Anders, IFEReuder, Jochen, UiBSirnivas, Senu, NRELTande, John Olav, SINTEFUhlen, Kjetil, NTNUUndeland, Tore, NTNU
The conference chairs were
- John Olav Giæver Tande, Director NOWITECH, senior scientist SINTEF Energy Research- Trond Kvamsdal, Chair NOWITECH Scientific Committee, Associate Professor NTNU- Michael Muskulus, Vice Chair NOWITECH Scientific Committee, Professor NTNU
13
-
8/15/2019 Samlerapport DeepWind 2013
15/274
Opening session ‐ Frontiers of Science and technology
Innovations in offshore wind technology, John Olav Tande, SINTEF/NOWITECH
Key research
topics
in
offshore
wind
energy,
Kristin Guldbrandsen Frøysa, CMR/NORCOWE
Research at Alpha Ventus deep offshore wind farm , Stafan Faulstich, Fh IWES
WindFloat deep offshore wind operational experience,
Pedro Valverde, EdP
HyWind deep offshore wind operational experience, Finn Gunnar Nielsen, Statoil
14
-
8/15/2019 Samlerapport DeepWind 2013
16/274
-
8/15/2019 Samlerapport DeepWind 2013
17/274
7
Exciting floating concepts
BlueH (2007, 80 kW)HiPRwind
(2009, 2,3 MW)
NREL/MIT
(2011, 2,3 MW)
New generator concept allowsfor direct HVDC connection toshore and avoiding costlyoffshore sub-station
New support structure avoidcostly transition piece betweentubular tower and jacket
NOWITECH 10 MW reference turbine
The NOWITECH 10 MW referenceturbine introduces a newgenerator and support st ructureconcept
100 kV
8
Innfarm
Con
10
Courtesy AMSC
100 times the current density compared to copper
More than doubles the achievable magnetic field
Eliminates rotor losses
Operating at 20-50 K
New materials give new electromagnetic designs
Possible step-changing technology
Activity in new FP7 project: InnWind
Superconducting generators reduce weight
11
Optimization of the offshore gridInside and between wind farmsNew market solutions are requiredNew technology (HVDC VSC, multi-terminal, hybrid HVDC/HVAC, .. )Protection, Fault handling, Operation,Control, Cost, Security of Supply
0 5 10 15 20 25 30100
1020
1040
1060
1080
10100
10120
10140
Number of nodes
N u m
b e r o
f c a
b l e c o n
f i g u
r a t i o n s
R
-
8/15/2019 Samlerapport DeepWind 2013
18/274
Best poster at EOW 2011
Integrating str uctural dynamics, control and electric model
75 77 79 81 830
0.25
0.5
0.75
1
Time[s]
U g
r i d [ p u
]
70 75 80 85 90 95 1003.43.63.8
44.24.4
X [ M N m
]
70 75 80 85 90 95 1000
0.20.40.60.8
1
Y [ M N m
]
Time[s]
xy
14
Reducing uncertainties by better models
Integrated models simulate the behavior of the completeturbine with substructure in the marine environment:SIMO-RIFLEX (MARINTEK) and 3DFloat (IFE)Model capability includes bottom fixed and floating conceptsCode to code comparison in IEA Wind OC3 and OC4
Model to measurements comparison in progress
SECmMdpR
pu
Users:Research & Industry
Main Objectives:Industrial value creation, and morecost-effective offshore wind farmsBuild competence and gain newknowledgeDevelop and validate numericaltools and technical solutions
16
SmartGridRenewable
Energy SystemLab
EFOWI &NOWERI
(in cooperation
withNORCOWE)
Ocean Basinlab
Wind tunnel++
Mobiletest labETEST
Strong research infrastructure in development
EFOWI
NOWERI
From Idea to Commercial Deployment
Prototype
Technology Focus
Cost Focus
Commercial and Market Focus
Model test
Concept
LargeParks
Pilot Park
2001
2005
2009
2014-16
Graphic is copy from Statoil presentation on HyWindat WindPower R&D seminar; 20-21 January 2011, Trondheim, Norway
N
-
8/15/2019 Samlerapport DeepWind 2013
19/274
19
Rounding upRemarkable results are already achieved by industry and R&Dinstitutes on deep offshore wind technologyTechnology still in an early phase – Big potential provided technicaldevelopment and bringing cost downResearch plays a significant role in providing new knowledge asbasis for industrial development and cost-effective offshore wind
farms at deep seaCooperation between research and industry is essential for ensuringrelevance, quality and value creationTest and demonstration, also in large scale, is vital to bring researchresults into the market place
Offshore wind is a multidisciplinary challenge – internationalcollaboration is the answer!Outlook is demanding, but prosperous with a growing global market
20
NOWITECH is a joint 40M€research effort on offshorewind technology.
Integrated numericaldesign toolsNew materials forblades and generators.Novel substructures(bottom-fixed andfloaters)Grid connection andsystem integrationOperation andmaintenance
Ass essm ent o f no velconcepts
www.NOWITECH.no
We make it possib le
Questions?
-
8/15/2019 Samlerapport DeepWind 2013
20/274
Key research topics in offshorewind energy
DeepWind 2013
Kristin Guldbrandsen FrøysaDirector NORCOWE
Outline
• Motion compensation• Measurements and database• Wind farm layout• Wind farm power control and prediction
Slide 2/ 31-Jan-13 Source: http
Description of wind shear
• Empirical power law description of the vertical wind shear:
• The logarithmic wind profile
ref ref z
zu zu )(
0
* ln)( z z
k u
zu
Wind profiles and stability
• Measurements at high towers show, that these windprofiles based on surface-layer theory and Monin-Obukhovscaling are only valid up to ca. 50-80 m
J. ReuInstitu
O
F
MSh
-
8/15/2019 Samlerapport DeepWind 2013
21/274
J. Reuder, GeophysicalInstitute, University of Bergen
Satellite data (SAR, QuickScat)Ocean wind speed map from ERSSAR from Horns Rev in the NorthSea, Denmark observed 6 October2004. The Horns Rev offshorewind farm is located in thetrapezoid.
• Source: http://galathea3.emu.dk/satelliteeye/projekter/wind/back_uk.html
Shortcomings:limited temporal resolutionuncertainty in determinationof relevant wind speed overthe rotor disk
Lidar going offshore
• Why?– Poor information on the offshore wind field in the relevant height
interval (30..200 m)– Corresponding mast structures are expansive and rather inflexible
• Challenges– Motion avoidance or motion correction– Adaptation to harsh marine environment– Energy for long term deployments
SeaZe(Natu
Zephspareleg bu
Li
Stewart platform
• Application of 55 different motion patterns on a 6-DOF motion platform, 3hours each
Lidar movement testing
source: Final Report of the project “Measurements of Wind Profile from a Buoy using Lidar” in cooperation between Fugro OCEANOR, Statoil,University of Bergen, Uni Research, Christian Michelsen Research (CMR) and Marintek
Offshore comparison E
•••
Source: M
-
8/15/2019 Samlerapport DeepWind 2013
22/274
HMF 2200-K4 Loader Crane
• 2012:– Foundation– Instrumentation
– Modeling & Simulation– (Real Time Simulation)
• Future work (2013):– Control System– Experimentation
Source: Magnus B Kjelland, UiA
Real Time Simulation
Real Time PC Simulation Model
Human Operator
Control System
Source: Magnus B Kjelland, UiA
A nof wmod
Strengths of model reduction technics
• Physical– The method solves the non-linear flow equations in a reduced space.
• Fast– The method provides CFD quality results within seconds of
computational time (single CPU).
• Power production– Individual turbine production calculated.
• Turbulence– 3D flow fields for both velocity and turbulent kinetic energy are
computed.
• Transfer– The model reduction technique can take advantage of improvements in
the CFD tool, such as improved turbine and turbulence models.
Illustration of int erfaceR
•
-
8/15/2019 Samlerapport DeepWind 2013
23/274
Irregular grid
• Non-regular layout: investigate selected non-regularlayouts. What is the energy yield compared to a regularlayout setup?
Power production sensitivity
• Regular / non-regular layout: What is thesensitivity of the power production on variationsof the wind rose?
• This could highlight how changes in the inflow conditions dueto nearby wind farms potentially would affect the powerproduction of the downstream wind farm.
W
•
Wind farm power control and prediction
Slide 22/ 31-Jan-13
Source: Torben Knudsen, AAU
Can a dynamic controlled power setpoint control of all turbines improvetotal production further?
Slide 23/ 31-Jan-13
Source: Torben Knudsen, AAU
•
Slide
Ccle
Source: T
-
8/15/2019 Samlerapport DeepWind 2013
24/274
Thank you for
your attention!
www.norcowe.no
Slide 25/ 31-Jan-13
-
8/15/2019 Samlerapport DeepWind 2013
25/274
Funding Body Supervisor Coordination
Research at alpha ventusJoint research at Germany’s first offshore
wind farm
Stefan Faulstich, Michael Durstewitz, Bernhard Lange, Eva OttoFraunhofer Institute for Wind Energy and Energy System TechnologyIWES, Kassel, Germany
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway2
Content
Alpha ventus,…
– milestones
– layout
…RAVE…
– Objectives
– Measurements
– Exemplary results
…and beyond
– Continuation of RAVE
– Technology monitoring
TE
3
© Fraunhofer
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
Competence CenterRotor Blade
Climate chamber 200 metermeasuring mast
The Fraunhofer IWES – experimental facilitiesExemplary Highlights
www.fraunhofer.iwes.de
4
© Fraunhofer IWES
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
alpha ventus and RAVE
• 2007 in Germany: – Very ambitious offhore plans, but no offshore turbine – German sites: far out and in „deep“ water
5
A
•
•
•
•
•
6
-
8/15/2019 Samlerapport DeepWind 2013
26/274
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
© DOTI www.alpha-ventus.de
REpower 5M AREVA Wind M5000
Fino 1
• North Sea• 45 km north
of Borkum• Water depth:
30 m• 12 turbines• 5 MW class
-AREVAWind M5000-Repower 5M
Alpha ventus: project details
7Research atalpha ventus – Stefan Faulstich
24.01.2013, DeepWind 2013, Trondheim, Norway
Alpha ventus / results 2011
• Production (2011): 267 GWh4,450 full load hours
8 9
R
•
••••
•
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
Main objectives of RAVEDemonstration Development Investigation of OWP issues
Expand research, experience & expertise
10
© DOTI 2009; Boris Valov, FraunhoferIWES; DEWI; Sebastian Fuhrmann;Fraunhofer IWES
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
measurement service
11
RAVE – R&D contents
12
R
-
8/15/2019 Samlerapport DeepWind 2013
27/274
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway13
• Detailed Load and turbine data fromfour wind turbines
• SCADA data of all turbines
• Geological, oceanographic andenvironmental data
• LiDAR (upwind and downwind)
RAVE – measurements
© DOTI
• Electrical data from substations
• Meteorological data from FINO1 AREVA Wind
M5000
REpower 5M
© GL
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway14
Structuraldynamics
Meteoro-logy
RAVE – measurements
Wave water pressure
Corrosion
Soundemmission
Operationaldata
Hydrology /Geology
Birdobservation
In total about 1300 Sensors!Data Warehouse: 10 Tbyte, 85 accredidated users
R
15
•
•
•
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
RAVE 2012: exemplary research results
• Lidar based control can improve theenergetic output of a turbine by 1-2 %
• Progress in turbulence and wakesimulation and in understandingturbulence interaction betweenoffshore wind farms
• An operation and failure statisticsdata base is of high relevance – progress is underway
16
© G L G a r r a
d H a s s a n
© R E p o w e r
S y s
t e m s
S E
© D O T I
, 2 0 0 9
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
RAVE 2012: exemplary research results
• Operational sound is of lowerecological relevance
• Social acceptance increased2011 compared to 2009;
17
• Bubble curtains reduce piledriving noise emissioneffectively
© H y d r o
t e c h n i
k L ü b e c k
G m
b H
© M a r
t i n - L u t
h e r -
U n i v e r s
i t ä t H a l
l e - W
i t t e n
b e r g
R
18
•
•
-
8/15/2019 Samlerapport DeepWind 2013
28/274
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
RAVE
RAVE has achieved its goals:• Proven the offshore-capability of the 5 MW turbine class• Facilitated further development of offshore wind technology in many
areas• Improved the knowledge about offshore wind utilisation• Produced an invaluable and unique data set of measurements
RAVE will continue, but the focus will move:• from design and erection to operation and maintenance• from demonstration to research
19Research atalpha ventus – Stefan Faulstich
24.01.2013, DeepWind 2013, Trondheim, Norway
What is RAVE today?
• A research lab in the middle of the North Sea
• A huge unique set of measurement data
• A research community dedicated to OWP
• An interdisciplinary knowledge base for
OWP topics
20
© Fraunhofer IWES; LeibnizUniversität Hannover; REpowerSystems; Reinhold Hill; KlausLucke; BSH
S ci
R
T
Le
T
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
Technology Monitoring
22
12
34
56
78
910
1
2
3
4
5
0,00,20,40,60,81,01,21,41,61,82,02,22,42,62,83,03,23,43,63,84,0
m e a n a
n n u a
l f a i l u r e
f r e q u e n c y
year of operation year ofproduction
Research atalpha ventus – Stefan Faulstich24.01.2013, DeepWind 2013, Trondheim, Norway
To answer fundamentalquestions ondevelopment of windpower offshore
General monitoring
To optimize operationand maintenance
Systematic collectionand evaluation ofoperational experiences
23
Technology Monitoring
24
T
W
W
R“C
Al
-
8/15/2019 Samlerapport DeepWind 2013
29/274
-
8/15/2019 Samlerapport DeepWind 2013
30/274
-
8/15/2019 Samlerapport DeepWind 2013
31/274
The WindFloat Project 13
Pre-assembly of the columns
outside the Dry-dock in Setúbal
The WindFloat Project 14
Columnsmoved to Dry-dock
The WindFloat
The WindFloat Project 16
Mooring Pre-Lay in parallel
with the fabrication
The WindFloat Project 17
Turbine Installation in the Dry Dock using the
shipyard’sgantrycrane
The WindFloat
Tow from S
same vessel
-
8/15/2019 Samlerapport DeepWind 2013
32/274
The WindFloat Project 19
Hook-up at final location
The WindFloat Project 20
In Operation since December2011!
The WindFloat
The WindPrelim
The WindFloat Project 22
Survivability and performance proved in normal and extreme conditionsPreliminary performance analysis
22 Oct2011Installation complete
01 Nov201115 meterswave
20 Dec 2011FirstElectron produced
03 Jan 2012Operation in Hs=6m andHmax=12,6m
The WindFloat Project 23
• The fabrication and installation were successfully complete despite all the challenges faced
• The technical results of the first 6 months of operation of the WindFloat are very promising
• The testing and monitoring of the WindFloat will continue during the next years
• WindPlus will start to prepare the Pre Commercial phase
• One step towards the development of deep offshore wind
Conclusions
The WindFloat
T
-
8/15/2019 Samlerapport DeepWind 2013
33/274
Hywind. Deep offshore windoperational experience.Finn Gunnar Nielsen, Statoil RDI
The starting point -2001
• Inspired by floating sailing marks.
“Seawind” matured during 2002
Tong, K.C. OWEMES seminar , Atena,Rome,Feb. 1994
2
Ke
Co
De
”St
Wa
Ass
Re
Flo
Ele
On
Th
3
From idea to commercial concept
Demo
Pilot park
Model test
Concept & theory
Onshoreconnectedparks
2002
2005
2009
Technical Focus
Cost Focus
Market Focus
2013
Idea
2003
4
Onshoreconnectedparks
What does it take?
Demo
Pilot park
Model test
Concept & theory
Onshoreconnectedparks
2002
2005
2009
Technical Focus
Cost Focus
Market Focus
2013
Idea
2003
5
Onshoreconnectedparks
•Creativity•Competence & experience•Endurance•Business understanding•Professional project execution•Management commitment•Timing•Funding
M• De• Val• Mo• Irre
6
-
8/15/2019 Samlerapport DeepWind 2013
34/274
Assembly and installation of Hywind Demo Summer 2009
7
Operation in harsh environment
• Max wind velocity: 40 m/sec
• Max sign wave height: 10.5 m
8
Fu
9
Hywind Operation and monitoring
10
Databases and datamanagement
•Integration of people process and technology
•Use of data, collaborative technology and multidisciplinary work
Integrated Operations – implementing O&Gexperience
11
A b
12
-
8/15/2019 Samlerapport DeepWind 2013
35/274
Hywind performance in 2012
• 2 stops in Q1 due to external grid faults, total 57 days. Production loss of ~1,5 GWh
• Production 2012 is 7,4 GWh(8,9 GWh without grid error)
• 11% lower than normal wind speed
• Capacity factor 2012: 37% (would be 44% without grid error)
• September production 1,1 GWh, Capacity factor 54%.
• Focus on improvements, lower O&M cost
Grid faults
13
Production during a storm condition
• 24 hour period duringstorm “Dagmar”, Dec2011
• Avg. wind speed 16m/sec
• Max wind speed 24m/sec
• Max significant waveheight 7.1m
• Power production 96.7%of rated
14
MeWind
WEST
15
Data interpretation and validation
0 100 200 3000
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Amplitude[ton 2-s -1]
F r e q u e n c y
[ H z
]
Hull_MoorForceX_Pos1_Backup- Black curveis generatorspeed[RPM/1e4]
Time
F r e q u e n c y
[ H z
]
Oct/100
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1Gen. below800Gen. above800
3P
Surge
Pitch
Poor/No data
• Spectrogram of mooringline force
• 1 month of data shown
• Used for:
Error detection
Identification ofnaturalfrequencies.
16
Full scale versus computations• Wind speed 17.5 m/sec, Significant wave height 4.0m, Current 0.4 m/sec
• Estimated wave time history.
• Computed motion response
• Wind forces included from measured wind spectrum
• Visualization
Tower pitch motion
17
Be
• Me
• Ea
00
1
2
3
4
5
6
7
8x
b e n
d i n g m o m e n
t [ ( k N m ) 2 s
]
18
-
8/15/2019 Samlerapport DeepWind 2013
36/274
Importance of motion controller
50 100 150 200 250 300 350 400 450 500 550-6
-4
-2
0
2
4
6
time [s]
t o w e r p
i t c
h a n g
l e [ d e g
]
Conventional controller
Motion stabilizing controller
Shut down
19
Hywind evolutionUse of experience - Improved design
Hywind Demo Hywind II
• Bigger turbine
• Smaller hull• Lower costs• Site specific
20 21
Floasolu
The next step
22
Presentation title
Presenters namePresenters titleE-mail address ……@statoil.comTel: +4700000000
www.statoil.com
Thank You23
-
8/15/2019 Samlerapport DeepWind 2013
37/274
A1 New turbine technology
Design Optimization of a 5 MW Floating Offshore Vertical Axis Wind
Turbine, Uwe Schmidt Paulsen, Technical Univ. of Denmark, DTU
Operational Control of a Floating Vertical Axis Wind Turbine,
Harald Svendsen, SINTEF Energi AS
Control for Avoiding Negative Damping on Floating Offshore Wind Turbine,
Prof Yuta Tamagawa, Uni. of Tokyo
Towards the fully ‐coupled numerical modelling of floating wind turbines,
Axelle Viré, Imperial College, London
Geometric scaling effects of bend ‐twist coupling in rotor blades,
Kevin Cox, PhD stud, NTNU
36
-
8/15/2019 Samlerapport DeepWind 2013
38/274
Design Optimization of a 5MW FloatingVertical-Axis Wind Turbine
DeepWind’2013-10 th Deep Sea Offshore Wind R&D Conference24-25 January 2013 Trondheim, No
Uwe Schmidt Paulsen [email protected]
bHelge Aagård Madsen, Per Hørlyck NielsencJesper Henri Hattel, Ismet Baran
a,b DTU Department of Wind Energy, Frederiksborgvej399 Dk-4000 Roskilde Denmark c DTU Department of Mechanical Engineering, ProduktionstorvetBuilding 425 Dk-2800 Lyngby Denmark
DTU Wind Energy, Technical University of Denmark
DeepWindContents• DeepWind Concept• 1 st Baseline 5 MW design outline• Optimization process• Results• Conclusion
2 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU W
DeepWConte• Deep• 1 st B• Optim• Resu• Conc
3
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept
• No pitch, no yawsystem
• Light weight rotorwith pultrudedblades
4 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept
• No pitch, no yawsystem
• Floating androtating tube as aspar buoy
• Light weight rotorwith pultrudedblades
• Long slender androtating underwatertube with littlefriction
5 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU W
DeepWThe C
• No pitcsystem
• Floatingrotating tuspar buoy
• C.O.G. counter wbottom of
6
-
8/15/2019 Samlerapport DeepWind 2013
39/274
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept
• No pitch, no yawsystem
• Floating androtating tube as a
spar buoy• C.O.G. very low –counter weight atbottom of tube
• Safety system
• Light weight rotorwith pultrudedblades
• Long slender androtating underwatertube with littlefriction with littlefriction
• Torque absorptionsystem
7 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept
• No pitch, no yawsystem
• Floating androtating tube as a
spar buoy• C.O.G. very low –counter weight atbottom of tube
• Safety system
• Light weight rotorwith pultrudedblades
• Long slender androtating underwatertube with littlefriction
• Torque absorptionsystem
• Mooring system
8 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU W
DeepWThe Co
• The b
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept- Blades technology
• The blade geometry is constant along the blade length
• The blades can be produces in GRP
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 201310 DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept -Blades technology
• The blade geometry is constant along the blade length
• The blades can be produces in GRP
• Pultrusion technology:
outlook- 11 m chord, several 100 m long blade length
11Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU W
DeepWThe Co
• The b
• The b
• Pultru
• Pultruat sit
outlo
-
8/15/2019 Samlerapport DeepWind 2013
40/274
DTU Wind Energy, Technical University of Denmark
DeepWindThe Concept- Blades technology
• The blade geometry is constant along the blade length
• The blades can be produces in GRP
• Pultrusion technology:
• Pultrusion technology could be performed on a shipat site
• Blades can be produced in modules
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
13
outlook- 11 m chord, several 100 m long blade length
DTU Wind Energy, Technical University of Denmark
DeepWind
Concept- Generator configurations• The Generator is at the bottom end of the tube; several configuration
are possible to convert the energy
14Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU W
DeepW
Conce• The G
are p
• Three
DTU Wind Energy, Technical University of Denmark
DeepWind
Concept- Generator configurations• The Generator is at the bottom end of the tube; several configuration
are possible to convert the energy
• Three selected to be investigated first:1. Generator fixed on the torque arms, shaft rotating with the tower
1
16Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
DTU Wind Energy, Technical University of Denmark
DeepWind
Concept- Generator configurations• The Generator is at the bottom end of the tube; several configuration
are possible to convert the energy
• Three selected to be investigated first:1. Generator fixed on the torque arms, shaft rotating with the tower2. Generator inside the structure and rotating with the tower. Shaft
fixed to the torque arms
1 2
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
17 DTU W
DeepW
Conce• The G
are p
• Three1.2.
3.
-
8/15/2019 Samlerapport DeepWind 2013
41/274
-
8/15/2019 Samlerapport DeepWind 2013
42/274
DTU Wind Energy, Technical University of Denmark
DeepWind2 nd iteration 5 MW Design Rotor
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
25
0
1
2
3
4
5
6
0.0 0.5 1.0 1.5 2.0 2.5H/(2R 0)
Sref/R02demo
Sref/(sR0) demo
Sref/R0**2
(Sref/sR0)
1 st DeepWind 5 MW
2 nd DeepWind 5 MWEOLE 4 MW (1.5,25)
GeometryRotor radius (R 0 ) [m] 58.5H/(2R 0 ) [-] 1.222
Nc/R 0 ) [-] 0.15Swept Area (S ref ) [m 2 ] 12318
DTU Wind Energy, Technical University of Denmark
DeepWind2 nd iteration 5 MW Design Rotor
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
26
0
1
2
3
4
5
6
0.0 0.5 1.0 1.5 2.0 2.5H/(2R 0)
Sref/R02demo
Sref/(sR0) demo
Sref/R0**2
(Sref/sR0)
1 st DeepWind 5 MW
2 nd DeepWind 5 MWEOLE 4 MW (1.5,25)
GeometryRotor radius (R 0 ) [m] 58.5 (-8%)H/(2R 0 ) [-] 1.222
Nc/R 0 ) [-] 0.15 (-33%)Swept Area (S ref ) [m 2 ] 12318(+15%)
DTU W
DeCP
DTU Wind Energy, Technical University of Denmark
0 0.01 0.02 0.03 0.04 0.05 0.060.3
0.35
0.4
0.45
0.5
0.55
Ixx /t w/c 3 %
Cp
AH93W145 AH93W174
AH93W215
DU00W2401
DU91W2250
DU97W300
FX84W218
NACA0009NACA0012 NACA0015
NACA0018 NACA0020
NACA0024 NACA0025
NACA0028 NACA0030
NACA0032
NACA0034
NACA0038
NACA0040
NACA0042
NACA23015
NACA4409
NACA4412
NACA643618
StandardaerofoilsOptimisationresults
DeepWind
CP vs dimensionless flapwise Inertia(bending stiffness )
CP
0.4
0,5
0.30.02 0.04 0.060.0
I xx /t c3 c©DeepWind,TUDelft
DTU Wind Energy, Technical University of Denmark
DeepWind2 nd iteration 5 MW Design Rotor
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
29
• uniform blade profiles NACA00xx, constant chord
• piecewise uniform profilesNACA0025,18,21, constant chord, Case-1,Case-2
DTU W
DeepWConte• Deep• 1 st B• Optim• Resu• Conc
30
-
8/15/2019 Samlerapport DeepWind 2013
43/274
DTU Wind Energy, Technical University of Denmark
DeepWindResults uniform profiles Case-1
31 Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
- Highest stiffness in NACA0025 profile leading the smallest displacement field andlinear elastic strain level
- NACA0015 has the highest weight- The tips of the rotor are fully constrained in all directions. Therefore, the maximum
elastic strain occurs close to the tips.- Apart from in the area of the tips, smaller strains, i.e. smaller than 5000 /m
strain are obtained.DTU Wind Energy, Technical University of Denmark
DeepWindResults-Constant blade chord withdifferent profile thickness Case-2
Section-1 (Bottom)
Section-2 (Middle)
Section-3 (Top)
Case-1 NACA0025 NACA0021 NACA0018 Case-2 NACA0025 NACA0018 NACA0021
- Similar strain distribution for Case-2 as compared to the one obtained for the uniformrotor having the NACA0025 profile except at the middle section. are obtained.
- It should be noted that the total weight of the sectionized rotor in Case-2 is lower thanthe uniform rotor having the NACA0025 profile which has the highest stiffness.
- Using a thicker blade profile at the top (Case-2) decreases the strain values as
compared to Case-1 in which a thicker profile is used at the middle
DTU W
DeepWResul
33
DTU Wind Energy, Technical University of Denmark
DeepWindResults case-2
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
34 DTU Wind Energy, Technical University of Denmark
DeepWindResults case-2+ 1iteration
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
35 DTU W
DeepWConte• Deep• 1 st B• Optim• Resu• Conc
36
-
8/15/2019 Samlerapport DeepWind 2013
44/274
DTU Wind Energy, Technical University of Denmark
DeepWindConclusion• Demonstration of a optimized rotor design
Stall controlled wind turbine Pultruded sectionized GRF blades 2 Blades with 2/3 less weight than 1 st baseline 5MW design Less bending moments and tension during operation
Potential for less costly pultruded blades
• Use of moderate thick airfoils of laminar flow family with smaller CD 0 andgood CP
• Exploration of potential for joints• Investigation for edgewise vibrations due to deep stall behavior
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
37 DTU Wind Energy, Technical University of Denmark
DeepWindConclusion
Thank YouQuestions?
Design Optimization of a 5 MW Floating OffshoreVertical-Axis Wind Turbine 24/1 2013
38
Thanks to the DeepWind consortium & EU
-
8/15/2019 Samlerapport DeepWind 2013
45/274
12/02/2013
1
Technology for a better society
10 th Deep Sea Offshore Wind R&D conferenceTrondheim, 24 – 25 Jan 2013
1
Harald G Svendsen
Karl O Merz
Operational Control of a Floating Vertical Axis Wind Turbine – start ‐up and shut ‐down
Technology for a better society
• Control system for the DeepWind turbine• Start ‐up and shut ‐down scheme
2
Overview
Technology for a better society
• Floating VAWT• Rotating spar buoy• Stall ‐regulated• No pitch, no yaw, no gearbox• Simple blade geometry, simple installation
• EU FP7‐project led by DTU ("DeepWind") – www.deepwind.eu
3
The DeepWind concept
Technology for a better society
• Objectives• Maximise energy capture• 2p variations• Limit over ‐speed and over ‐torque• Start and stop
• How?• Via generator torque
4
Control system
Technology for a better society
• Basic structure:
5
Control architecture
Rotor speed
Notchfilter
LP
LP
Electricaltorque
Lookuptable Ref.
speed
PIDElectricaltorque set ‐point
2p damping
Aerodynamic efficiencySpeed limitation
Technology for a better society
• Aerodynamics: Fourier approximation that includes 2p and 4p variations
, ,Ω cos 2 cos 4 • = turbine azimuth angle relative to the wind speed• , , , , given by look ‐up tables for wind = and rotor speed = Ω,
computed by a BEM model and includes dynamic stall effects (Merz)• Hydrodynamics and mooring system: Bottom end assumed fixed except in yaw
• Magnus lift force• torque absorption (one degree of freedom) spring–damper mooring system
• Structural mechanics: Spring–damper representations of tower twisting and tilting• Electrical system: Generator torque = controller set ‐point
6
Simulation model
44
-
8/15/2019 Samlerapport DeepWind 2013
46/274
12/02/2013
2
Technology for a better society
• Achieved by adjusting the speed reference value• Start: 0 → target value• Stop: present value → 0
• Avoid conflict between normal/start/stop/parked operation by defining operational states
7
Turbine start ‐up and shut ‐down
Technology for a better society 8
Operational states
Technology for a better society
0 5 10 15 20 25 30 35 40 45 500
0.1
0.2
0.3
0.4
0.5
0.6
• Torque–speed map
• High wind: Reduced reference speed (storm control)• Based on wind measurements• Limit torque• Capture more energy
9
Normal operation
0 5 10 150
0.1
0.2
0.3
0.4
0.5
0.6
Optimal speed
Limited speed
Rated torque
R e f . s p e e d ( r a d
/ s )
R e f . s p e e d ( r a d
/ s )
Wind speed (m/s)
Torque (MNm)
Cut ‐in
Storm control
Cut ‐out
(Use torque–speed map)
Technology for a better society
• Speed ramp ‐up profile with end ‐point determined from slow ‐filtered wind measurement
• Cross ‐fade to speed reference given by torque–speed map (normal speed control)
10
Start ‐up
Start ‐up profile
Target speed – torque mapTarget speed – wind map
Cross ‐fade
completed
time
R e f . s p e e d
Technology for a better society
• Smooth start• Critical: Transition from ramp ‐
up to steady speed• Increased integral gain for
faster response during start
11
Start ‐up: Example (high wind)
Wind threshold
Start ‐up initiated
W i n d ( m / s )
speed (pu)
torque (pu)power (pu)
G e n e r a t o r o u t p u t
Time (s)
Time (s)
Technology for a better society
• Speed ramp ‐down to zero• Extra torque needed to initiate shut ‐down• Parked state: Reference speed = 0, integral path in PI control disabled
12
Shut ‐down
Shut ‐down profile
Normal operation speed reference
completed
time
R e f . s p e e d
45
-
8/15/2019 Samlerapport DeepWind 2013
47/274
12/02/2013
3
Technology for a better society
• Critical: Wind gust at the same time as braking is initiated
large torque
13
W i n d ( m
/ s )
Storm controlShut ‐down
S p e e d ( r a d
/ s )
G e n e r a t o r
( p u ) torque (pu)
power (pu)
Parked
Shut ‐down:
Example (high wind)
Technology for a better society
• Baseline control system for the Deepwind floating VAWT turbine has been completed• Damps 2p variations• Minimises stress on mooring system• Maximises energy capture• Safe start ‐up and shut ‐down procedures
14
Conclusions
Technology for a better society
Technology for a better society
15 Technology for a better society 16
Basic parameters – initial 5 MW design
Parameter Value
Under ‐water length 108 m
Darrieus rotor height 130 m
Darrieus rotor radius 64 m
Rated wind speed 14 m/s
Rated rotational speed 0.52 rad/s (5 rpm)
Rated torque 9 ·106 Nm
Technology for a better society 17
Control architecture
46
-
8/15/2019 Samlerapport DeepWind 2013
48/274
2013/2/12
1
Control for Avoiding Negative Dampingon Floating Offshore Wind Turbine
2013/1/24Yuta Tamagawa, Tokyo univ.
Makoto Iida, Tokyo univ.Chuichi Arakawa, Tokyo univ.
Toshiki Chujo, NMRI
Introduction• Demand for renewable energy is increasing
Securing laying area for wind farmWind is consistent and strong over the sea
Establish offshore wind turbine technology – Floating Wind Turbine
• Able to use on Deep Water • Unstable foundation
2013/2/12J.M.Jonkman. (2007). Dynamics Modeling and Loads Analysis of anOffshore Floating Wind Turbine. Technical Report. NREL/TP-500-41958.November 2007
Verification test casesHywind (statoil, Norway)Small test turbine (Nagasaki Japan)
Negative damping of Floating Wind Turbine
•
Pitch ControlChange blade pitch depend on the wind speed variation. – Torque Constant Thrust Vary
• Relative wind speed vary dew to the motion of tower. – Lean to the front (back) Relative wind speed increase decrease
Thrust decrease (increase)Negative damping
2013/2/12
Thrust
Wind
Wind
ThrustWind load
Wind load Thrust
Rotor disk
Rotor diskPitch angle
Pitch angle
Torque
Torque
Purpose of research
2013/2/12
Applying conventional pitch control
Motion of float is negative damped
Reducing rated power Power decrease
Increasing fatigue load
We needs to develop new pitch controlcorresponding to floating wind turbine
Larsen, T. J., & Hanson, T. D. (2007). A method to avoid negative dampedlow frequent tower vibrations for a floating, pitch controlled wind turbine.Journal of Physics: Conference Series , 75
1)
We propose a new control method for floating turbine tosuppress the negative damping with power kept to rate.
Control method
2013/2/12
PID Blade PitchRotorSpeed
Pitch Control
PIDTower anglevelocity θ tower
Motion Control
Pitch Control
θ tower
Combining two control Mixed controlPitch Control (Make rotational speed constant)Motion Control (Suppress tower motion θ tower )
Experiment and Simulation• Set floating wind turbine model on
test tank with fan.Cooperated with NMRI : National
Maritime Research Institute)
• Software for numerical simulation FASTDeveloped by NREL (National Renewable Energy
Laboratory)Able to compute floating wind turbine
NREL 5MW
2013/2/12
Test tank and turbine model
OC3-Hywind des gnJ.M.Jonkman. (2007). Model Development and Analysis of an OffshoreWind Turbine on a Tension Leg Platform, with a Comparison to OtherFloating Turbine Concepts. Subcontract Report. NREL/SR-500-45891.February 2010
Tenson eg platform
47
-
8/15/2019 Samlerapport DeepWind 2013
49/274
2013/2/12
2
Turbine and condition
Wind turbine Blade Length 600mmNumber 3Ro tor di ame ter 1 30 0mm
Nacelle Weight 1150gTower Hub height 900mm
Float Float Diameter 160mmDraft 1270mmDisplacedvolume of water
23kg
Mooring line Number 6
2013/2/12
830
5deg. Nacelle
Tower
Blade
Hub
1220
φ160 t7
Wind speed [m/s] 3.9
Wave (regular) Height [cm] 4.22 6.3 8 8.7
Period [s] 3.0 2.5 1.8 1.4
Validation of simulation
• Aero dynamic force of blade and float response to thewave are generally consistent
2013/2/12
0
0,2
0,4
0,6
0,8
1
1,2
1,4
0 2 4 6 8
C t
Tip speed ratio
E xp F AS T
0
10
20
30
40
50
60
0,5 1 1,5 2
T o w e r P i t c h a m p l i t u d e
Wave eriod [s]
FASTExp FAST
Tower amplitude of floating test turbine with wave and nowind.
Tower amplitude is non-dimensionalizedby wave height andwave number )
Thrust coefficient of test turbine in onshore.
Blade load (Thrust) Float response to the wave
Change blade pitch on wind speed 3.9 m/s )
Negative damping on experiment(Wind speed:3.9m/s, Wave period:2.5s, Wave height:6cm)
• Tower pitch amplitude : increase rotor speed vibration : decrease• Negative damping has occurred on experiment
2013/2/12
0
2
4
6
8
10
12
14
16
18
20
0 5 10 15 20
T o w e r p i t c h a n g l e [ d e g ]
Time[s]
250
270
290
310
330
350
370
390
0 5 10 15 20
R o t o r s p e e d [ r p m ]
Time[s]
Tower pitch angle of test turbine on experiment Rotor speed of test turbine on experiment
Negative damping on simulation(Wind speed:3.9m/s, Wave period:2.5s, Wave height:6cm)
• Tower motion and rotor speed vibration are smallerthan experiment.
• Trends of parameter are matched with experiment.
2013/2/12
10
12
14
16
18
20
100 105 110 115 120
T o w e r p i t c h a n g l e [ d e g ]
Time[s]
Pitch C on tro le d No Control
300
305
310
315
320
325
330
335
340
345
350
100 105 110 115 120
R o t o r s p e e d [ r p m ]
Time[s]
Pitch C on tr ol ed N o Control
Tower pitch angle of test turbine on simulation Rotor speed of test turbine on simulation
Mixed control on simulation(Wind speed:3.9m/s, Wave period:2.5s, Wave height:6cm)
• Kp: Control parameterof motion controller onmixed control.
• Basis of rate on rightside is parameter onconventional control.(when K p=0)
2013/2/12
Controlparameter
Kp
Θ tower Amplitude(deg)
Rotor speed average(rpm)
0 5.51 (100%) 336 (100%)0.0001 5.38 (97.6%) 336 (99.97%)
0.001 5.24 (95.1%) 335 (99.7%)
0.01 3.70 (67.2%) 326 (97.1%)
0.1 5.01 (91.0%) 239 (71.3%)
1 5.32 (96.6%) 74.7 (22.2%)
As K p=0.01, Tower motion is much suppressedthough rotor speed is not so much changed.
Mixed control can suppress the negativedamping with little affect to the rotor speed.
Conclusion• On simulation aero dynamic force of blade and float response to
the wave are generally match to experiment.• We confirmed that tower motion is amplified by onshore pitch
control on experiment and simulation.• We proposed the new control, mixed control, and shows that
mixed control can reduce the tower motion with maintaining rotorspeed.
• Improving simulation model, we will apply this control to practicalturbine, verification test turbine or full scale turbine and investigatethe applicability and effectiveness of this control in actual seas.
2013/2/12
48
-
8/15/2019 Samlerapport DeepWind 2013
50/274
Towards the fully-coupled numericalmodelling of oating wind turbines
Axelle Vir é, J Xiang, M Piggott, C Cotter, J Latham, C Pain
[email protected] Modelling and Computation Group (AMCG)
Department of Earth Science and Engineering
10th Deep Sea Offshore Wind R&D Conference – 24 January 2013
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
MotivationScope of a 2-year Marie Curie Intra-European Fellowship
Couple two nite-element models for modelling uid-structure interactions Apply them to the various components of a oating wind turbine
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
Outline
1. Modelling uid-solid interations for oating solids
2. Parameterisation of wind turbines
- Actuator-disk modelling- Results for a xed turbine
3. Tracking of an interface between two uids
- Conservative advection method- Results for a oating pile
4. Future work
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interationsCoupling between two unstructured nite-element models
Mesh adaptivity tore ne the solidconcentration eld
A.Viré,Reviews in Environmental Science and Bio/Technology (2012)
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interationsCoupling between two unstructured nite-element models
ACTION=
REACTION
The uid and solid models use different spatial and temporal discretisations
Mesh adaptivity tore ne the solid
concentration
eld
A.Viré,Reviews in Environmental Science and Bio/Technology (2012)
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interationsFluid-dynamics model: Fluidity-ICOM
Solid-dynamics model: Y3D-Femdem
The equations are solved for a monolithic velocity: ū = α f ū f + α s ū s
∇̄ · ū = 0
An additional force accounts for the presence of the solids:
β = fctρf ∆ t
, ν L 2
DDt
(ρs ū s ) = ∇̄ · ¯̄τ s + F̄ s
F̄ f = β (α s ū s − α s ū) = F̄ 2 − F̄ 1
ρf ∂ ̄u∂t
+ ρf ū · ∇̄ ū = − ∇̄ p + ∇̄ · ¯̄τ + F̄ f
F̄ s = F̄ 1 − F̄ 2
Conservation V
F f dV = − V s
F s dV s
(ρf = constant)
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
49
-
8/15/2019 Samlerapport DeepWind 2013
51/274
1. Modelling uid-solid interationsFluidity-ICOM
Solid meshSolid meshFluid mesh
in
Sub-timestep i = 0
Compute F n = F n1 − βu n+ i
s
outCompute F n1 = βα
n
s un
1 F 1
o ve or u s= + 1
o ve or un = n +
Time-averaged solid velocity ¯ u s2
Y3D - Femdem
Compute F = − F 1 + F 2
Viré et al. , Ocean Dynamics, Vol. 62 (2012)
Time step n : (u, α s )n Time step n : (x s , u s )n
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interations
.
1
0 0.5 1
.
− .
Solid element s
Fluid element
Galerkin projectionfrom solid to uid mesh
V s
F s2 dV s = V
F f 2 dV
F s2
F f 2
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interationsFluidity-ICOM
Solid meshSolid meshFluid mesh
in
u -timestep i =
Compute F n = F n1 − βu n + is
outCompute F n1 = βα
n
s un F n1 1
o ve or u s= + 1
o ve or un = n + 1
ime-average so i ve ocity ¯ u s
Y3D - Femdem
Viré et al. , Ocean Dynamics, Vol. 62 (2012)
F n2Compute F = − F 1 + F 2
Minimally-diffusiveGalerkin projection
Time step n : (u, α s )n Time step n : (x s , u s )
n
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interations
.
1
.5 1
.
− 0.25
Solid element s
Fluid element
. 1
Solid element s
Fluid element
0.5
1
0
Galerkin projectionfrom solid to uid mesh
Galerkin projectionfrom uid to solid mesh
.
1
V s
F s2 dV s = V
F f 2 dV
F s2
F f 2
F f 1
F s
1
V ∩ V s
F f 1 dV ∩ = V s
F s1 dV s
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
1. Modelling uid-solid interationsFluidity-ICOM
Solid meshSolid meshFluid mesh
in
u -timestep i =
Compute F n = F n1 − βu n + is
outF 1
o ve or u s= + 1
o ve or un = n + 1
ime-averaged solid velocity ¯ u s2
Y3D - Femdem
Compute F = − F 1 + F 2
Minimally-diffusiveGalerkin projection
Supermesh
n
1 = βαn
s un
Fluid mesh
Solid mesh
Portion of a supermesh
Viré et al. , Ocean Dynamics, Vol. 62 (2012)
Time step n : (u, α s )n Time step n : (x s , u s )n
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
2. Parameterisation of wind turbines
The turbine is parameterised through an actuator-disk model
The thrust force is spread uniformly across a thin disk
u 0 u1A1A0T
uhub Ahub
(Conway, J Fluid Mech, 1995)
The disk is meshed separately from the uid domain
The uid mesh is adapted dynamically in time
The reference velocity is computed from and
T = 12
ρu 20 Ahub C T
a = 1 − u hub
u 0=
12
1 − 1 − C T u 0 C T uhub
Dr Axelle Vir éTowards the fully-coupled numerical modelling of oating wind turbines
50
-
8/15/2019 Samlerapport DeepWind 2013
52/274
2. Parameterisation of wind turbinesUniform ow past a 3D turbine of constant thrust coefcient and Re D = 1000
The size of the uid domain is 25 D × 10 D × 10 D
The disk thickness is 2 % of the disk diameter D
The uid mesh adapts to the curvatures of the velocity and pressure elds
Reference: Potential ow past an actuator disk with constant loading(J. Conway, J. Fluid Mech. 297, 327–355, 1995)
C T = 0 .2
C T = 0 .