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IPP Annual Report 2007 - Max-Planck-Institut für Plasmaphysik ...

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use of generator power consumption applying lower PF coil<br />

voltages reducing inductive loads and new shape and scenario<br />

evolution accounting better for PF coil interactions. Plasma<br />

currents up to 1 MA at limited triangular plasma shapes,<br />

heating powers up to 7.5 MW and flattop times of more than<br />

5 s were achieved.<br />

In spring <strong>2007</strong> the transition of the AUG vessel to fully<br />

tungsten coated plasma facing surfaces (PFCs) was completed<br />

with the 200 μm W-cladding of the lower outer divertor target<br />

tiles. Careful cleaning of all other tiles was performed to remove<br />

old carbon and boron layers. Accordingly the main emphasis<br />

of the <strong>2007</strong> experimental campaign was on the operation in<br />

an all-metal machine. The proposals were prioritized into W<br />

compatibility of ITER scenarios, extension of the working<br />

space with a metal wall and other ITER related physics<br />

investigations. Plasma operation was accomplished from<br />

April to July and September to October. We conducted 54 long<br />

shifts at high availability with a total of 1150 pulses (technical<br />

tests, diagnostic calibrations and plasma discharges).<br />

1.2 ITER relevant results in <strong>2007</strong><br />

In April <strong>2007</strong> the restart of AUG was done without prior<br />

boronization as the first divertor tokamak operating with a<br />

full tungsten wall. The reduced generator capacity caused<br />

limitations of transformer flux swing, plasma current, plasma<br />

shaping and heating power. In spite of these tough boundary<br />

conditions, a “milestone” pulse was already achieved six<br />

weeks after the first plasma attempt with a full performance<br />

H-mode discharge at β N =2, confinement factor H 98 =1 and a<br />

density of 70 % of the Greenwald density as in previous H-mode<br />

discharges with boronization. No boronizations were performed<br />

throughout the whole campaign. The W concentration<br />

remained at an acceptable level by using central ECRF<br />

at higher heating powers enhancing the turbulent impurity<br />

transport. Obviously the divertor W source has only minor<br />

influence on the plasma W content, which is mainly determined<br />

by the local influx from the low field side limiters<br />

and the central column. The carbon content of a few per<br />

mille did not decrease further, but the net C deposition in the<br />

inner divertor was strongly reduced. This is important for<br />

the tritium co-deposition problem in ITER, as is the whole<br />

W programme for DEMO where the erosion of low-Z material<br />

and the destruction of graphite under neutron bombardment<br />

will be unacceptable (section 2).<br />

The use of ICRF heating is restricted with tungsten walls<br />

by W sputtering caused by accelerated light impurities in<br />

the ICRF antenna near-fields. Therefore the beneficial effect<br />

of ICRH for suppression of W accumulation is offset under<br />

un-boronized conditions. Simulations show an important<br />

influence of the antenna geometry and the resulting box<br />

currents on these electric fields, which will be checked in<br />

2008 after the installation of covering metal corner plates<br />

on one of the antennas.<br />

ASDEX Upgrade<br />

4<br />

During the last years on ASDEX Upgrade the physics base<br />

for ITER operation was significantly extended in both the<br />

foreseen standard H-mode scenario as well as the stationary<br />

improved H-mode (ITER Hybrid) scenario. The progress was<br />

slowed down in <strong>2007</strong> in favour of the tungsten experiments.<br />

Concerning anomalous transport, zonal flows, geodesic acoustic<br />

modes and turbulence k-spectra were investigated by<br />

Doppler reflectometry (section 6.1-6.2). New insights were<br />

gained on the interaction of energetic particles (produced by<br />

ICRH) with TAEs and other modes driven by the fast ions<br />

based on new diagnostics (fast ion loss detectors, SXR, fast<br />

ECE, hopping millimetre-wave reflectometer (from IST),<br />

CO 2 laser) and theoretical tools (section 6.3-6.6). The structures<br />

of ELM produced filaments, pellet ELM triggering,<br />

wall heat loads from ELMs and disruptions, fuel retention in<br />

W surrounding, and disruption mitigation by a fast gas puff<br />

valve close to the plasma have been looked at (section 7).<br />

1.3 Technical Enhancements and Programme in 2008<br />

The restart of AUG is planned for February 2008, again<br />

without boronization and with the main emphasis on reactor<br />

relevant scenarios in an all-metal machine. Assessment of<br />

plasma performance, divertor properties, C retention, erosion,<br />

hydrogen and noble gas balance and operation without intrinsic<br />

C radiation are the main themes. Improved H-modes<br />

at low ITER-like collisionality (may need the revival of<br />

boronizations) and at high densities will be possible with the<br />

increased power from EZ3 extending our operational window.<br />

At the start of the new campaign the EZ3 generator current<br />

will be enhanced providing an increase from 144 MVA to<br />

175 MVA. With the EZ4 flywheel back in operation in<br />

October 2008 and with the experience gained last year the<br />

AUG operation will be boosted into shaped plasma operation<br />

with up to 1.6 MA and more than 20 MW heating power<br />

at pulse lengths lasting for 10 s. This is supported by reliable<br />

tokamak operation including NTM stabilization, ELM and<br />

disruption mitigation. For the 2008 AUG campaign 171 experimental<br />

proposals have been submitted by 84 scientists,<br />

with more than 50 % from outside <strong>IPP</strong> and including 44 ITPA<br />

joint experiments. A prioritized programme was approved by<br />

the AUG PC and will be conducted by new TF leaders including<br />

one from the UKAEA.<br />

In order to achieve AUG´s programmatic goals and to maintain<br />

a leading position parallel to the ITER construction, it is<br />

necessary to continuously upgrade the AUG diagnostic and<br />

technical systems (section 4). The successful H-mode operation<br />

with an all-tungsten wall has set a milestone. The preparations<br />

of the next major hardware extensions are well<br />

underway with support from other EU Associations. Fast ion<br />

loss detectors for the poloidal distribution of fast ions, CTS<br />

(from RisØ) and beam fluctuation measurements (from HAS)<br />

are the next new diagnostics. The tube geometry of the<br />

blower gun extending the pellet ELM-triggering capability

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