1 / 19

Francisco A. Calderon University of Warwick

Francisco A. Calderon University of Warwick. Outline. Brief introduction to fusion High confinement and instabilities: ELMs What is needed for?  ITER … demo Description and results Further work. Section 1. Brief introduction to Fusion. Controlled thermonuclear fusion reactions.

zared
Download Presentation

Francisco A. Calderon University of Warwick

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Francisco A. Calderon University of Warwick

  2. Outline • Brief introduction to fusion • High confinement and instabilities: ELMs • What is needed for?  ITER … demo • Description and results • Further work

  3. Section 1 Brief introduction to Fusion Controlled thermonuclear fusion reactions Inertial confinement Magnetically confined plasma Tokamak Stellerator

  4. High confinement: ELMs 1Asdex-Upgrade tokamak

  5. Why do we need to study ELMs?

  6. ITER • Is a Tokamak • Lab for burning plasma • Prove DEMO feasibility • Been built in: • Caradache, Les Bouches du Rhône, southernFrance. • Further info: www.iter.org • Check for ITER newsletter!

  7. Section 3 Work andResults

  8. Experimental data

  9. Analysis • Use time ocurrence(see figure) as new time series {tn}. • We define the inter-ELM time interval as [6]: • dtn= tn – tn-1. • Construct delay plots. • Make PDF of the inter- ELMs time intervals.

  10. Delay plots • Are not a phase space reconstruction as we used here • Example: single pendulum, with a period p.

  11. Threshold scheme There are a few ELMs per time series, and they ranges from 67 - 196.

  12. Gas puffing rate Reproduced from Calderon et al. (2013) [9]

  13. First set with lower gas puffing rate Reproduced from Ref. [9]

  14. Second set with higher gas puffing rate The population in the sharp peak increases with the gas puffing rate. Reproduced from Ref. [9]

  15. Conclusions

  16. Section 4 Further Work • Webster et al. (2013)has recently found signs of Resonant behaviour in JET plasmas. - We see this as Stripes on Delay plots • Are ELMs coupling with Coils?

  17. Why is this been seen now?

  18. The End

  19. References • [1] A Loarteet al., Plasma Phys. Control. Fusion 45, 1549 (2003) • [2] K Kamiyaet al., Plasma Phys. Control. Fusion 49, S43 (2007) • [3] R J Hawryluk et al., Nucl. Fusion 49, 065012 (2009) • [4] www.iter.orgRetrieved 15th june 2013. • [5] J Greenhough, S C Chapman, R O Dendy, and D J Ward, Plasma Phys. Control. Fusion 45, 747 (2003) • [6] T Schreiber and A SchimdtPhysicaD 142346–382, (2000) . • [7] A Degeling, Y Martin, P E Bak, J B Lister, and X Llobet, Plasma • Phys. Control. Fusion 43, 1671 (2001) • [8] Webster et al. “Time-resonant tokamak plasma edge instabilities?” (2013), In press. • [9] F A Calderon, R O Dendy, S C Chapman, A J Webster, B Alperet al., Phys. Plasmas 20, 042306 (2013)

More Related