Impurity penetration through the edge transport barrier

被引:16
作者
Belo, P
Parail, V
Corrigan, G
Heading, D
Houlberg, W
Monier-Garbet, P
Ongena, J
机构
[1] EURATOM, IST Fus Assoc, Ctr Fusao Nucl, P-1049001 Lisbon, Portugal
[2] UKAEA Euratom Fus Assoc, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England
[3] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
[4] CEN Cadarache, EURATOM Assoc, F-13108 St Paul Les Durance, France
[5] EURATOM, Plasma Phys Lab, Lab Plasmafys, Ecole Royale Mil B, B-1000 Brussels, Belgium
关键词
D O I
10.1088/0741-3335/46/8/010
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The ELMs in H-mode plasmas manifest themselves as short bursts of increased edge transport, which expel energy and particles, including impurities from the plasma edge to the SOL and further towards target plates and limiters (Zohm H 1996 Plasma Phys. Control. Fusion 38 1213, Loarte A et al 2003 Plasma Phys. Control. Fusion 45 1549). ELMs are considered beneficial events with respect to impurities since they can prevent impurities from accumulating in the plasma core. JET has recently performed an experiment in which a controlled influx of noble gas impurities was successfully used in order to reduce the amplitude and frequency of type-l ELMs. An interesting correlation between the level of the main gas puffing and the radial redistribution of impurities has been found in this experiment: it was shown that impurities are contained near the separatrix in discharges with a relatively strong level of main gas puffing. Reduction of the puffing below a certain level leads to impurity accumulation in the core followed by thermal collapse. This paper describes the results of predictive modelling of impurity seeding experiments on JET using a coupling of the 1.5D core transport code JETTO (for the main ions) and ID transport code SANCO (for impurities). Two sets of boundary conditions for the density and temperatures, which correspond to two different deuterium gas puffing rates, were used in the modelling. An explanation for the experimentally observed phenomenon is presented.
引用
收藏
页码:1299 / 1311
页数:13
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