21
Moving fast in fusion reactors: ASCOT – race track for fast ions T. Kurki-Suonio, Aalto University for the ASCOT team O. Asunta, E. Hirvijoki, T. Koskela, J. Miettunen S. Sipilä, A. Snicker and S. Äkäslompolo

Moving fast in fusion reactors: ASCOT – race track for fast ions

  • Upload
    haile

  • View
    74

  • Download
    0

Embed Size (px)

DESCRIPTION

Moving fast in fusion reactors: ASCOT – race track for fast ions. T. Kurki-Suonio, Aalto University for the ASCOT team O. Asunta, E. Hirvijoki, T. Koskela, J. Miettunen S. Sipilä, A. Snicker and S. Äkäslompolo. MeV–range ions in reactors  MW/m2 on the wall?. Today’s tokamaks - PowerPoint PPT Presentation

Citation preview

Page 1: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Moving fast in fusion reactors: ASCOT – race track for fast ions

T. Kurki-Suonio, Aalto University

for the ASCOT team

O. Asunta, E. Hirvijoki, T. Koskela, J. MiettunenS. Sipilä, A. Snicker and S. Äkäslompolo

Page 2: Moving fast in fusion reactors:  ASCOT – race track for fast ions

MeV–range ions in reactors MW/m2 on the wall?

Today’s tokamaks– only mock-fuel: pure D ”no” fusion reactions

Tomorrow’s reactors:– Fusion reactions 3.5 MeV alphas– Neutral beams 1 MeV deuterons and/or

tritons– ICRH heating ions with several MeV

Page 3: Moving fast in fusion reactors:  ASCOT – race track for fast ions

How to confine hot ions so that ― they heat the plasma ― they do not destroy the wall?

In principle, charged particles are glued to the magnetic field lines

Page 4: Moving fast in fusion reactors:  ASCOT – race track for fast ions

But life is never so simple...

Fast ions can have large gyro radii and ENORMOUS banana widths

Page 5: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Engineering reality: no axisymmetry

An almost ideal situation:JET w/ 32 coils

Reactor reality: ITER w/ 18 coils

Only finite # of TF coils B-field becomes a ”toroidal sausage” = Toroidal Field Ripple

Page 6: Moving fast in fusion reactors:  ASCOT – race track for fast ions

ITER reality: There is more to life than the TF ripple...

Even the harmonic ripple structure is destroyed by things like

Presence of ferritic material in the walls* Ferritic inserts (FI) reduce the TF ripple* Ferritic structures can introduce strong local

perturbations. Prime example: TBMs in ITER* Also by lack of FIs (around NBI ports)

External coils can generate their own ’ripples’ at their will. * Prime example: ELM-mitigation coils in ITER

(and, today, at AUG, DIII-D, JET)

Page 7: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Example: BT (φ) at the edge of ITER

Toroidal ripple 0.25%,

Field bump due to NBI ports 0.57%

Field bump due to TBMs1,1%

Page 8: Moving fast in fusion reactors:  ASCOT – race track for fast ions

How to study fast ions today:

DT-experiments to produce 3.5MeV alphas?– few and far apart:

~TFTR (1993): Pfus = 10.6 MW~JET (1997): Pfus = 16.1 MW (Q ~ 0.7)

Externally produced fast ions?– Neutral beam injection: only up to about 100keV– ICRH: MeV range ions but only few

We are left at the mercy of simulations– Multitude of codes, but one appears quite far

ahead of the others...

Page 9: Moving fast in fusion reactors:  ASCOT – race track for fast ions

ASCOTFully 3D

– 3D magnetic field– 3D Wall

Realistic orbit tracing– Guiding center (fast)– gyro orbit (accurate)

Comprehensive interactions– Coulomb collisions– Turbulent transport– Models for relevant MHD:

• NTM-type magnetic islands• Alfven Eigenmodes

Page 10: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Some examples: 3D effects on fast ions a la ASCOT

TBM mock-up experiments at DIII-D– Effect on NBI-ions– Effect on neutrons from DD -> DT -fusion reactions

The effect of ELM-mitigation coils on wall loads:– NBI-ions in ASDEX Upgrade

ITER wall power loads due to fusion alphas:– The effect of ripple & Co– The effect of wall structure

Page 11: Moving fast in fusion reactors:  ASCOT – race track for fast ions

The effect of ferritic structures

Case Study: TBM mock-up experiments @ DIII-

D

Page 12: Moving fast in fusion reactors:  ASCOT – race track for fast ions

NBI-generated deuterons in DIII-D discharges w/ TBM mock-up

limiters

TBM mock-up coils

Page 13: Moving fast in fusion reactors:  ASCOT – race track for fast ions

DD DT 14 MeV n

Experimental neutron flux in the TBM mock-up exp’t

Fraction of confined tritium in the plasma as calculated by ASCOT

M. Schaffer & al, Nucl. Fusion 51 (2011) 103028

Page 14: Moving fast in fusion reactors:  ASCOT – race track for fast ions

The effect of ELM-mitigation Coils

Case study: B-coils in ASDEX Upgrade

Page 15: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Losses of 60keV NBI deuterons

Direct ripple well losses

Additional spot next to the coil

Page 16: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Fusion alphas in ITER

Advanced Scenario-4Ip = 9MA ’only’

Confined fast ions vulnerable

Page 17: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Axisymmetry vs ripple vs FI2-limiter case

Axisymmetric B-field With ’nude’ rippleRipple w/ FI’s

Page 18: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Also wall shape matters...

Original wall w/ 2 limiters Present wall design w/ poloidally extended ’continuous’ limiters

Page 19: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Future of fast stuff: full of work!

F4E task approved: – GRT-379: “Calculation of the TBM-induced

ripple in ITER, wall loads, impact on plasma and optimization”, 2012 – 2014; 777 500 €

ITPA-EP activity: expert group twice a yearTritium experiments at JET (2015?)

Page 20: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Thank you for your attention!

Page 21: Moving fast in fusion reactors:  ASCOT – race track for fast ions

Acknowledgements

For input data:• ITER Organization, IPP Garching, General Atomics

For computing resources:• The supercomputing resources of CSC – IT center for science• HPC-FF

For funding:• This work was partially funded by the Academy of Finland Projects No. 121371 and No. 134924• This work, supported by the European Communities under the contract of Association between Euratom/Tekes, was carried out within the framework of the European Fusion Development Agreement. The views and opinions expressed herein do not necessarily reflect those of the European Commission.