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Transport

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ITER Physics R&D. Modelling. ... ITER walls will be considerably more sensitive to ELMS than the walls in present ... emphasis on ITER relevance and ... – PowerPoint PPT presentation

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Title: Transport


1
Transport
  • Jan Weiland
  • Recent results from
  • IAEA Geneva October 2008
  • TF-T JET February 2009
  • ITPA Naka March-April 2009
  • RU work 2008-2009

2
Main areas in International transport research
  • Momentum transport
  • Particle transport
  • Transport barriers
  • Transient transport
  • Scaling studies
  • These areas are all covered in the new Transport
    Topical Group, chaired by Carlos Hidalgo

3
TTG-overview
4
ITER Physics RD
  • Modelling. Substantial advances in the
    theoretical understanding of plasma behaviour and
    modelling capabilities are still needed in order
    to complement the present semi empirical
    extrapolations to ITER
  • Gyrokinetic codes are now in use and have been
    rather successful in comparison with experiment.
    However, they can still not be run on the
    transport timescale. Apparent succes running on
    shorter timescales still needs to be understood
  • Significant progress has been made on momentum
    transport, both toroidal and poloidal. Prandtl
    numbers (ratio of toroidal momentum and ion heat
    diffusivities) agree roughly with experiments
    both for diagonal and effective diffusivities.
    Also the anomalous spinup of poloidal rotation in
    JET is recovered by theory based models.

5
Hybride mode
  • A strong interest in the Hybrid mode scenario
    (Hybride mode is an H-mode with a broad q profile
    everywhere above 1). Hybride modes have slightly
    better confinement than usual H-modes but show
    degradation of confinement with beta. They have
    higher beta than ordinary H-modes because the
    lowest order NTM mode has been stabilized.
    However, higher order NTM modes are still
    present, making simulations with drift wave
    models difficult.

6
ITER issues
  • New issues in ITER modelling are the current
    rampup and current rampdown phases. They may be
    critical since large ELMs (Edge Localized Modes)
    or even disruptions may be difficult to avoid.
    ITER walls will be considerably more sensitive to
    ELMS than the walls in present day tokamaks.
  • Since present theory based transport models
    have problems with the current dependence,
    empirical models are mainly used.

7
Current ramping
  • Simulations using the empirical Coppi-Tang model
    have indicated that the current ramp rate should
    be below 0.5 MA/s for impurity, electron
    temperature and inductance control.
  • The fastest density drop was found to be t_p 5
    t_E and the slowest the same rate as the current
    in order to maintain the same ratio (0.85) to the
    Greenwald density.
  • Density pump-out was needed in order to
    control the H-L transition during rampdown as
    well as for avoiding radiative collapse.
  • Hidalgo emphasized the need to understand the
    L-H transition better for the current rampup
    phase.

8
Fluid - Kinetic models
  • Generally accepted that kinetic models can still
    not be run on the transport timescale, i.e. can
    not be used in predictive transport codes.
  • It seems that nonlinear frequency shifts often
    detune kinetic resonances on a shorter timescale.
    However, it is difficult to give general criteria
    for this and when this happens also a reactive
    fluid model must be valid.
  • What can be proven is that also the strongly
    nonlinear perpendicular dynamics relaxes on the
    confinement timescale in the case of maximum
    phase mixing.
  • Thus we need to assume that the fact that
    nonlinear effects initially are stronger (more
    coherent state) will phase mix all kinetic
    resonances before the turbulence is phase mixed
    since then the timescale increases to the
    confinement timescale.
  • The actual times for these different phase
    mixings are complicated functions of the strength
    of the instabilities, the correlation length,
    frequency mismatches in the mode coupling, level
    of first maximum etc.

9
Fluid kinetic models cont.
  • A new gyrofluid model, TGLF uses quasilinear
    kinetic theory, normalized to nonlinear kinetic
    simulations (Gyro). Also this model has problems
    with particle pinches. Results close to
    quasilinear kinetic.
  • Improved quasilinear kinetic models are under
    development

10
Particle transport
  • Particle transport
  • Very good agreement between our model and Gyro
    for particle transport in ITER-like plasmas.
    (Candy Nordman Fülöp et. al, IAEA 2008) (see
    below)
  • This indicates again that nonlinear gyrokinetic
    codes may relax linear kinetic resonances on
    timescales shorter than the confinementtime as
    discussed above.

11
Databases, physical mechanisms, methods and
general fusion physics
  • It is important to further develop the
    comprehensive understanding of fusion physics and
    the theoretical-computational tools
  • The further elucidation of physical mechanisms
    such as reconnection, non-local transport and
    turbulence suppression has high importance for
    key questions on fusion plasmas and needs to be
    compared with experiments on a range of fusion
    devises with a sufficiently broad range of
    parameters
  • An expansion of the first principle basis of
    modelling codes would enhance the confidence in
    their use for extrapolating from present day
    devices towards a reactor

12
Transient transport
  • Electron transport
  • Mantica Our model better than GLF 23 and GS2
    for several JET discharges studied
  • Momentum transport, Torq modulation
  • Tala Studies of diagonal Prandtl numbers and
    peaking factors for GS2 indicates good agreement
    with JET experiments.
  • We have made full simulations which now give good
    agreement with modulation phases and amplitudes
    in the inner 50

13
Frameworks for international collaboration
  • EFDA-JET Transport work at JET is mainly
    organized by Task Force T (transport)
    (participation from Chalmers) Activities on Core
    heat transport, Transport of main particle
    species, Impurities, Transient transport, Edge
    turbulence
  • ITPA (International Tokamak Physics Activities)
  • Swedish RU participates in several groups.
    Within Confinement and Modelling and also in
    Transport we have participation from Chalmers.
    This activity is a continuation of the previous
    ITER Expert Group activities and is focused on
    problems of special interest for the next step
    large tokamak.

14
Frameworks, cont
  • ITM (European Task Force on Integrated Modelling,
    TFL Pär Strand) A new well funded project is
    EUFORIA.
  • TTG The accompanying programmes in the
    associations are focusing on more basic aspects
    of the high priority tasks
  • In particular Momentum transport and Particle
    transport

15
Simulation of Transport barrier dynamics
  • A new model for toroidal momentum transport
    has been derived from fluid theory including
    toroidal effects from the stress tensor (J.
    Weiland, R. Singh, H. Nordman et. al. Proc. IAEA
    2008 TH/P8.29) Accepted for Nuclear Fusion)
  • With the new model it has been possible to
    simulate four channels simultaneously, Ion and
    Electron temperatures and Poloidal and Toroidal
    momentum
  • Using all these channels the formation of a
    transport barrier could be simulated from initial
    profiles without barrier. The agreement with
    experiment was good including also the strong
    spinup of poloidal momentum (J. Weiland, P.
    Mantica, T.Tala et al. Presentation at the ITPA
    meeting in Naka March-April 2009)

16
Drift Waves in Tokamaks and Stellarators
  • Study of ion-temperature gradient (ITG) modes
    in 3D configurations
  • Disagreements found between numerical and
    analytical equilibria
  • The growthrate of the ITG mode is smaller in
    Stellarators than in tokamaks
  • Also electron trapping included 2008

17
Intrinsic Rotation
A. Kritz, G. Bateman, F. Halpern et. al. US TTF
2009
  • Nine time slices from four DIII-D discharges are
    plotted
  • NBI torque is varied from co to counter with
    other parameters fixed
  • MMM08 model reproduces observed angular momentum
    variation of with torque
  • Positive toroidal angular momentum at zero torque
    (intrinsic rotation) is observed
  • Caused by inward convection of momentum from
    boundary to plasma core
  • Negative torque is needed to produce zero total
    angular momentum

Discharges described in paper by W. M. Solomon,
K. H. Burrell, J. S. deGrassie, R. Budny, R. J.
Groebner, J. E. Kinsey, G. J. Kramer, T. C. Luce,
M. A. Makowski, D. Mikkelsen, et al., Plasma
Physics and Controlled Fusion 49(12B), B313 (2007)
18
Model comparisons
  • Comparisons between nonlinear gyrokinetic
    simulations (GYRO), TGLF and Weiland model for
    ITER-like plasma (ref scenario 3).
  • Fluid results obtained for k??0.2.
  • Comparison between Weiland model and nonlinear
    GENE simulations for JET discharges planned for
    2009 (330 kCPU hours allocated in HPC-FF).
  • J. Candy, H. Nordman, T. Fülöp et al, Proc of
    IAEA Fusion Energy Conf TH/P8-28, Geneva (2008).

19
Trace versus self-consistent treatment
  • Weiland model treats impurities
  • self-consistently. The often used trace impurity
    approximation is not adequate in TE dominated
    regimes.
  • Carbon peaking factor R/LnC in (a) ITG dominated
    regime and (b) TE dominated regime versus
    normalised temperature gradient for standard
    parameters.
  • T. Fülöp, H. Nordman, PoP 16, 032306 (2009).

20
COllisional Model of Electrostatic Turbulence
  • Semi-analytical gyrokinetic model of long
    wavelength electrostatic microinstabilities.
  • Shear dependent model ballooning potential
  • The electron-ion collisions are modeled by a
    Lorentz operator
  • Simple analytic expressions for the quasilinear
    particle and heat fluxes
  • See poster of I. Pusztai

21
Stiffness with rotation
Weiland Grey norot, Green Wexb1.1104,
Purple Wexb 2.1 104, Dimits shift included
in calc. but no effect
22
Summary
  • Increased emphasis on ITER relevance and
    collaborations in the new EU programme
  • A new framework for collaboration in basic
    transport problems , TTG, is supposed to connect
    Accompanying programmes in the Associations and
    is expected to produce new physics results that
    can be transferred to more applied activities .
  • Both the TF-T meeting at JET and the ITPA meeting
    in Naka have shown that a large number of basic
    physics problem remain and that we need to apply
    a combination of experimental, numerical and
    analytical techniques in order to make progress.
  • At the ITPA meeting in Naka plans were made for
    combined activities of the new European TTG, The
    TTTF activities in Europé and the US and ITPA.

23
Summary cont.
  • New areas of interest
  • Current rampup and rampdown experiments
  • Transport in Hybride discharges. This may require
    more detailed geometry effects since
    electromagnetic effects appear to be important
  • Transient transport for comparison of kinetic and
    fluid models
  • Transient momentum transport (torq modulation)
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