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
2Main 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
3TTG-overview
4ITER 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.
6ITER 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.
7Current 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.
8Fluid - 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.
9Fluid 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
10Particle 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.
11Databases, 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
12Transient 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
13Frameworks 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. -
14Frameworks, 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 -
15Simulation 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) -
-
16Drift 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
17Intrinsic 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)
18Model 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).
19Trace 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).
20COllisional 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
21Stiffness with rotation
Weiland Grey norot, Green Wexb1.1104,
Purple Wexb 2.1 104, Dimits shift included
in calc. but no effect
22Summary
- 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.
23Summary 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)