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Superconducting Generators for Large Wind Turbines Markus Mueller Ozan Keysan – Joe Burchell Institute for Energy.

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Presentation on theme: "Superconducting Generators for Large Wind Turbines Markus Mueller Ozan Keysan – Joe Burchell Institute for Energy."— Presentation transcript:

1 Superconducting Generators for Large Wind Turbines Markus Mueller Ozan Keysan – Joe Burchell markus.mueller@ed.ac.uk o.keysan@ed.ac.uk Institute for Energy Systems The University of Edinburgh 19/03/2012

2 Motivation BARD 5MW Global Offshore Wind Energy Markets and Strategies,2009 In 2020, 85% of offshore wind turbine installations will be larger than 5 MW

3 Wind Turbines: Constantly Growing  How big?  UpWind Project: A 20 MW Wind Turbine is Feasible www.upwind.eu

4 Mass of Direct-Drive Generators Harakosan 1.5MW,18 rpm,47 tonnes (*) D. Bang et.al. “Review of Generator Systems for Direct-Drive Wind Turbines,” 2008, All data available at goo.gl/ZZivv goo.gl/ZZivv Enercon 4.5 MW, 13 rpm 220 tonnes

5 All data available at goo.gl/ZZivv goo.gl/ZZivv Mass of Direct-Drive Generators

6 Reliability of Wind Turbines Hahn, B., & Durstewitz, M. (2007). Wind Energy-Reliability of Wind Turbines. ~1MW, 1500 onshore turbines

7 Types of HTS Machines  Rotating DC Superconducting Field  Most Common Type  Transient Torques on HTS wire  Cryocooler Coupler + Electrical Brushes  Low Reliability + Maintenance  Magnetized Bulk HTS  Very Difficult to Handle  Demagnetization?  All Superconducting Machines  AC Losses on HTS wire

8 Reliability?  Cooling System  Cryogenic Couplers  Electric Brushes  Transient torques on SC  Demagnetization for Bulk SC  AC losses on SC wire Issues with Superconducting Generators SeaTitan AMSC, 10 MW, 10 rpm Direct-drive superconducting generator

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10 Homopolar HTSG

11  Pros  Stationary SC Field  No Brushes  No Transient Torque on SC  Simplified Cooling, Isolation

12 Homopolar HTSG  Cons  Uni-directional flux density  Reduced power density

13 Bipolar HTSG

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15  Pros  Bidirectional Flux  Increased Power Density  Cons  Double SC field winding  Mechanical Issues

16 Transverse Flux HTSG

17  Pros  Single Stationary SC Coil  Bidirectional flux  High Torque Density  Cons  Magnetic Attraction Forces  3D Flux (Soft magnetic composites needed) Transverse Flux HTSG

18 3D FEA Verification

19 Main Specifications Power Output70 kW Speed100 rpm Diameter1.3 m Axial Length0.5 m SC Wire Current216 A SC Wire Length880 m

20 Next Stage: Linear Prototype

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22 Some Publications  "A Homopolar HTSG Topology for Large Direct-Drive Wind Turbines", Keysan O., and Mueller M., 2011. IEEE Transactions on Applied Superconductivity, 21(5), 3523 - 3531. doi:10.1109/TASC.2011.2159005.A Homopolar HTSG Topology for Large Direct-Drive Wind Turbines  "Superconducting Generators for Renewable Energy Applications", Keysan O., and Mueller M., 2011, IET Renewable Power Generation Conference, Edinburgh.Superconducting Generators for Renewable Energy Applications  "A Transverse Flux High-Temperature Superconducting Generator Topology for Large Direct Drive Wind Turbines", Keysan O., and Mueller M., 2011. Superconductivity Centennial Conference, 2011, Den Haag, The Netherlands.A Transverse Flux High-Temperature Superconducting Generator Topology for Large Direct Drive Wind Turbines THANKS


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