Assessment of Drift Loss in ITER with Pellet Fuelling and ELM Pace Making A' Polevoi, A' Loarte, A' - PowerPoint PPT Presentation

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Assessment of Drift Loss in ITER with Pellet Fuelling and ELM Pace Making A' Polevoi, A' Loarte, A'

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Requirements for ELM pace making pellets (l = Dped ?) Background ... height (n,T) and width (Dped ) are rather uncertain. R&D: Pedestal parameters? 8 ... – PowerPoint PPT presentation

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Title: Assessment of Drift Loss in ITER with Pellet Fuelling and ELM Pace Making A' Polevoi, A' Loarte, A'


1
Assessment of Drift Loss in ITER with Pellet
Fuelling and ELM Pace MakingA. Polevoi, A.
Loarte, A. Kukushkin, W. Houlberg, S. Maruyama,
D. Campbell, V. ChuyanovITER Organization,
Cadarache, France
  • Pellet injection in ITER
  • Model description
  • Model validation
  • Additional loss due to ELM pace making
  • Possible RD

2
Pellet fuelling is required in ITER
fuelling from the edge saturates at low level
16 Pa m3/s
3
ELM mitigation is required in ITER
  • Predicted natural ELM energy loss
  • in ITER DWELM20 MJ (DWELM/Wped 20)
  • Permissible ELM energy loss
  • DWELM 1 MJ (DWELM/Wped 1 )
  • Background
  • - Erosion is negligible for QELM lt 0.5 MJ/m2
  • Zhitlukhin et al, JNM 2007
  • - Strong in/out asymmetry Pout/Pin 1 2
  • Eich et al, JNM 2007
  • - ELM affected area Sin 1.3 m2
  • DWELM QELM x Sin x (1 Pout/Pin)
  • 0.5 MJ/m2 x 1.3 m2 x 1.5 ? 1 MJ

Permissible ELM energy loss DWELM
Maximal Load gt x
ELM affected surface x Peaking factor
4
ELM mitigation by pellet injection is possible
  • Background
  • reduction of ELM loss DWELM for high ELM
    frequency fELM (JET, ASDEX-U)
  • DWELM (0.20.4) x Psep/ fELM gt
  • Hermann , 2002 Urano et al, 2004
  • full ELM control by pellet pace making with
    reduced DWELM is demonstrated
  • (ASDEX-U)
  • fELM fpel 20- 40 Hz gt
  • Lang et al, 2005
  • gt fpel fELM 20- 40 Hz (ITER)
  • RD
  • - Confinement degradation with high-frequency
    pace making?

5
Independent HFS pellet fuelling and LFS ELM pace
making in ITER is possible Polevoi et al, 34th
EPS, 2007
ITER HFS and LFS Injection Flight Tubes Layout
6
Requirements for ELM pace making pellets (l
Dped ?)
  • Background
  • For ELM pace making pellet size, dpel and speed,
    vpel must provide penetration to the top of
    pedestal
  • l Dped ASDEX-U, Lang et al, 2005
  • (for penetration to the half of pedestal l 0.5
    Dped )
  • DIII-D, Baylor et al,35th EPS, 2008
  • Ablation depth, l depends on the pellet size,
    dpel, speed vpel and plasma parameters, n, T
    along the path. It is higher for higher dpel,
    vpel and for lower n, T along the pellet paths.

ASDEX-U, Lang et al, 2005
RD Real requirements for pellet for ELM
triggering?
7
Requirements for ELM pace making pellets
(pedestal?)
  • ITER pedestal
  • Reference ITER parameters
  • n, T along the pellet paths. Top of pedestal
    is assumed to be located at 95 of poloidal
    magnetic flux
  • NB predicted pedestal parameters
  • height (n,T) and width (Dped )
  • are rather uncertain.
  • RD
  • Pedestal parameters?

8
Requirements for pellets for ELM pace making
maximal speed
  • RD
  • Dependence of intact pellet speed on size of
    the bore of a guide tube
  • Dependence of intact pellet speed on
    accumulation of residual gas in the tube for
    multiple frequent injection

9
Requirements for pellets for ELM pace making
minimal size
  • RD
  • - Validation of ablation model for 2 4 mm
    pellets for vp, 300-1000 m/s and n, T similar to
    ITER pedestal
  • - Accumulation of residual gas in the tube for
    multiple frequent injection (10 loss per pellet)

10
Compatibility of Pumping/Fuelling/Pace making
11
Pellet model description
  • Simplified Mass Ablation and Relocation
    Treatment
  • Polevoi, Shimada, PPCF, 43 (2001) p.15
  • - Ablation model by Kuteev
  • Kuteev B, 1995, Nucl. Fusion 35 431
  • Cloud size by Parks, et al
  • Parks P B, Sessions W D and Baylor L R 2000
    Phys. Plasmas 7 1968
  • - Mass relocation by Strauss, Parks
  • Strauss H R and Park W, 1998, Phys. Plasmas 5
    2676
  • RD
  • Model validation for ablation, cloud size and
    relocation
  • No time evolution target state gt final state

12
No time evolution target state gt final state
  • Input/Output parameters
  • Electron and electron temperatures, Te, Ti, keV
  • Ion species density, nH, (H pellet) nD,
    nT,(D,T,DT pellet) 1019 m-3
  • Electron density, ne, 1019 m-3
  • Input solid lines gt
  • Output dashed lines

HFS pellet injection in ITER-like plasma
13
Model validation (examples)
  • ASDEX-U HFS injection DIII- D LFS
    injection

Satisfactory agreement
14
Model validation (examples)
  • JT-60U HFS (Vert) injection DIII- D
    HFS injection
  • Takenaga et al, 2006, 33rd EPS
    Polevoi, Shimada, 2001

Satisfactory agreement
15
Additional loss due to ELM pace making(particle
loss in ELM)
RD Minimal pellet size for positive fuelling
16
Additional loss due to ELM pace making(energy
loss due to drift of LFS pellet)
  • Background
  • Cooling starts before ELM triggering
  • ASDEX-U, G. Kocsis, 2008, 35th EPS
  • Energy drop after pellet is
  • higher for LHS than for HFS
  • DWHFS/W 1 gt
  • DWLFS/W 8
  • DIII-D, L. Baylor et al, 2000, PoP
  • RD
  • Comparison of loss energy
  • for HFS/LFS injection to
  • extract drift loss

Energy loss triggered by pellet DIII-D, L.
Baylor et al, 2000, PoP
17
Additional loss due to ELM pace making(energy
loss due to drift of LFS pellet)
  • ITER
  • Assumption
  • LFS pellet is marginal for ELM triggering gt
  • ELM starts after ablation and cooling
  • Calculation with SMART
  • - Energy drop after pellet is higher for LHS
    than for HFS
  • DWHFS/Wped 1 (ELM)
  • DWLFS/ Wpedlt 2.3 (ELMdrift)
  • - Extra loss due to drift
  • Pdrift fLFS DWdrift
  • RD Comparison of loss energy for HFS/LFS
    injection to extract drift loss

Energy loss due to drift of LFS pellet
18
Possible RD
  • Injection system
  • Dependence of intact pellet speed on size of the
    bore of a guide tube and on accumulation of
    residual gas in the tube for multiple frequent
    injection
  • Accumulation of residual gas in the tube for
    multiple frequent injection
  • (10 loss per pellet)

19
Possible RD
  • Plasma transport
  • Pedestal parameters prediction
  • Confinement degradation with high-frequency pace
    making
  • Real requirements for pellet for ELM triggering
  • Influence of pellet induced modes
  • - Scaling DW (0.2 -0.4??) P/f

20
Possible RD
  • Pellet physics
  • Validation of ablation, cloud size and relocation
    models for 2 5 mm pellets with vp, 300 1000
    m/s for n, T similar to ITER pedestal
  • Minimal pellet size for positive fuelling
  • Comparison of lost energy for HFS/LFS injection
    to extract drift loss

21
Summary
  • Pellet injection system is considered as the most
    prospective technique for fuelling and ELM
    mitigation in ITER
  • Present estimates of pellet injection for plasma
    fuelling and ELM pace making suggest that for
    safe operation without confinement degradation
    and negligible additional load on the divertor
    target the speed of LFS pellet have to be
    increased to 1000 m/s.
  • RD is required to validate extrapolation of
    present day experiments assumed for the ITER
    pellet injection system design.
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