1 / 32

Topological issues and relationships with turbulence in the edge region

Topological issues and relationships with turbulence in the edge region. Presented by Matteo Agostini. Outline. Edge region: magnetic and kinetic point of view. Magnetic boundary, edge profiles and confinement properties.

lecea
Download Presentation

Topological issues and relationships with turbulence in the edge region

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. Topological issues and relationships with turbulence in the edge region Presented by Matteo Agostini

  2. Outline • Edge region: magnetic and kinetic point of view • Magnetic boundary, edge profiles and confinement properties • Interplay between magnetic boundary and turbulence in the density limit • Link between magnetic modes and turbulence

  3. Introduction • In the Reversed Field Pinch configuration q exhibits a decreasing profile • In the edge region q = 0 (reversal surface) RFX-mod R = 2 m a = 0.46m Ip = 0.3 – 1.5 MA • In the reversal surface all the m = 0 modes resonate

  4. Edge: Gradients • The edge region is characterised by strong radial gradients • They are source of free energy for the development of instabilities which could degrade the confinement

  5. The edge region plays a fundamental role in the plasma confinement Edge: Gradients • The edge region is characterised by strong radial gradients • They are source of free energy for the development of instabilities which could degrade the confinement

  6. Dt=0.4 ms Dt=1.2 ms Dt=0.8 ms Dt=0 f [mm] f [mm] f [mm] f [mm] r [mm] r [mm] r [mm] r [mm] Edge: Turbulence • In the region outside the reversal surface turbulence is responsible for the greatest part of the particle transport • It is caused mainly by coherent structures: density blobs • They are filaments elongated in the direction of the magnetic field • Blobs can interact with the magnetic islands

  7. Edge: Magnetic Topology Magnetic topology of the edge is dominated by m = 0 islands due to modes resonating on the reversal surface Multiple Helicity Quasi Single Helicity Large spectrum of m=1 modes is destabilised Mode m=1 n = -7 dominates Do the magnetic islands influence the edge properties and the transport?

  8. Magnetic Field & Edge Properties • HeI light emission in the plasma edge is modulated by the radial magnetic field • The maximum of emission is correlated with Brm=1

  9. ISIS Magnetic Field & Edge Properties • HeI light emission in the plasma edge is modulated by the radial magnetic field • The maximum of emission is correlated with Brm=1 • Floating potential measured by probes array shows the same spatial periodicity of the radial magnetic field Indication of the interaction between plasma edge and local magnetic field

  10. Islands & Profiles F= -0.2 #20367 Temperature profile flattens in the region inside the m = 0 island Temperature is constant on conserved magnetic lines Similar behaviour observed in tokamaks during NTM

  11. Islands & Profiles • Flow velocity and radial shear vary during the discharge evolution

  12. Islands & Profiles • Flow velocity and radial shear vary during the discharge evolution Higher velocity on conserved surface around the island

  13. Islands & Profiles • Flow velocity and radial shear vary during the discharge evolution Lower velocity on X-point where magnetic field lines intercept the wall

  14. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology

  15. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology • The wall locking is the local source of density

  16. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology • The wall locking is the local source of density • m = 0 island charges the wall with electrons

  17. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology • The wall locking is the local source of density • m = 0 island charges the wall with electrons • Accumulation point where vf= 0

  18. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology • The wall locking is the local source of density • m = 0 island charges the wall with electrons • Accumulation point where vf= 0 • Formation of high density toroidally localised region

  19. n/nG > 0.4 Br > 0 Br < 0 Density Limit Density limit is due to the interplay between edge toroidal flow and magnetic topology • The wall locking is the local source of density • m = 0 island charges the wall with electrons • Accumulation point where vf= 0 • Formation of high density toroidally localised region • Edge cooling and soft landing of the plasma current

  20. TS 0.78 < r/a < 0.87 TS 0.78 < r/a < 0.87 Temperature gradient at the edge become steeper Electron thermal conductivity decreases Scaling With m = 1 Modes Confinement improves with the improvement of the magnetic boundary control

  21. THB 0.9 < r/a < 0.98 m = 1 & Turbulence The decrease of the secondary modes is correlated with an improvement of the pressure gradient at the far edge Pressure gradient is commonly recognised as a source of free energy for the edge turbulence Lp = pressure radial scale length

  22. THB 0.9 < r/a < 0.98 THB 0.9 < r/a < 0.98 m = 1 & Turbulence The decrease of the secondary modes is correlated with an improvement of the pressure gradient at the far edge Lp = pressure radial scale length Lb = toroidal scale length of edge blobs

  23. THB 0.9 < r/a < 0.98 Link With Other Devices • Correlation between edge blobs and pressure gradient is not a peculiar characteristic of RFX-mod Alcator C-mod and NSTX points reflect the same scaling

  24. Conclusions Magnetic islands are found to exist around the reversal surface interacting with the edge plasma • Modify the edge profiles • Play a role in the density limit • Interact with the edge blobs • Modify the edge transport and confinement

  25. Conclusions Magnetic islands are found to exist around the reversal surface interacting with the edge plasma • Modify the edge profiles • Play a role in the density limit • Interact with the edge blobs • Modify the edge transport and confinement Open issues: Study the mechanism of interaction between islands and edge turbulence Clarify the role of islands and turbulence in the density limit

  26. Edge Parameters THB 0.9 < r/a < 0.98 THB 0.9 < r/a < 0.98

  27. Turbulence Scaling

  28. Common Properties NSTX Alcator C-mod

  29. Density Limit Radiation pattern in the poloidal plane

  30. Density Limit

  31. ~ 4% of the total B(a) SHAx

More Related