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Introduction Prediction of ITER loads and T retention A. Loarte

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Title: Edge Plasma Energy and Particle Fluxes in Divertor Tokamaks Author: Alberto Loarte Last modified by: ITER Created Date: 5/12/2002 4:38:06 PM – PowerPoint PPT presentation

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Title: Introduction Prediction of ITER loads and T retention A. Loarte


1
IntroductionPrediction of ITER loads and T
retentionA. Loarte
2
Specification of ITER Loads
  • Specification of ITER loads has been reviewed
    during ITER Design Review ? update to take into
    account present physics understanding
  • Particle/Power Fluxes to wall during diverted
    operation
  • Redefinition of divertor controlled ELM loads
  • Update of ELM divertor and wall power fluxes
  • Update of disruption and VDE thermal loads
  • Update of disruption and VDE EM loads
  • etc.
  • Revised load specifications will be used to
    redesign details of ITER PFCs (main wall) ?
    Advice from ITPA required
  • Uncertainties in load specifications is
    considerable ? judgment to specify reasonable
    and non-fluctuating values

3
Evaluation of T retention
in ITER
  • T retention is one of the key drivers for plasma
    facing materials choice in ITER ? PFM foreseen
    strategy based on present understanding of PWI
    in ITER
  • Change of CFC to W divertor to minimise T
    retention
  • Prediction of T retention in ITER is a complex
    and uncertain
  • Uncertain plasma fluxes and conditions
  • ITER-specific issues (high Tsurf/Gplasma,
    n-irradiation, etc.)
  • Formation of mixed-materials
  • etc.
  • Determination of fuel retention for ITER on
    present understanding, on-going RD and Hydrogen
    phase results crucial to decide on best timing
    for change of divertor plasma materials in ITER
    programme

4
QDT 10 steady plasma loads (I)
  • All divertor tomakaks measure plasma particle
    fluxes (II B) to the main wall
  • Extrapolated plasma flux to the main wall in
    ITER 1.0 - 5 .0 1023 s-1 (1-5 of Gdiv)

Lipschultz IAEA 2000
5
QDT 10 steady
plasma loads (II)
  • Plasma fluxes predominantly on outer side of
    first wall
  • Corresponding maximum IIB power densities up to
    5 MWm-2 (Upper X- point) to 1 MWm-2 near outer
    midplane and 0.4 MWm-2 near inner midplane

6
Tolerable ELM size
QSPA experiments on NB31 targets show
Tolerable ELM energy density 0.5 MJm-2 no
broadening 21 in/out asymmetry ? DWELM
1MJ fELM 20-40 Hz ? 8000-16000 ELMs/QDT10 shot
7
Wall ELM loads
Wall ELM power/particle deposition starting to be
characterised/understood ? extrapolation to
ITER uncertain
Uncontrolled ELMs in ITER? DWELM 20
MJControlled ELMs in ITER ? DWELM 1.0 MJ
Model by W. Fundamenski and R. Pitts
  • Uncontrolled ELMs ? DWELM,wall 2-4
    MJControlled ELMs ? DWELM,wall 0.05-0.1 MJ
  • tELM,wall ½ tELM,divertor
  • AIIELM lt Afil Nfil dpol dr 10 0.25 0.1
    0.25 m-2 (A. Kirk)
  • Uncontrolled ELMs ? EIIELM gt 8-16 MJm-2
    (ltqII,ELMgt 8-32 MWm-2 )
  • Ewall,ELM (4o) 0.6- 1.1 MJm-2
  • Controlled ELMs ? EIIELM gt 0.2-0.4 MJm-2
    (ltqII,ELMgt 4-16 MWm-2 )
  • Ewall,ELM (4o) 0.01-0.03 MJm-2
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