High Z neoclassical transport: Application and limitation of analytical formulae for modelling JET experimental parameters
Creators
- 1. CEA, IRFM, F-13108 Saint-Paul-lez-Durance (France)
- 2. CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, U (United Kingdom)
- 3. Max-Planck-Institut fur Plasmaphysik, Garching (Germany)
- 4. General Atomics, P.O. Box 85608, San Diego, California 92186-5608 (United States)
- 5. Aix-Marseille Universite, CNRS, PIIM UMR 7345, 13397 Marseille Cedex 20 (France)
- 6. FOM Institute DIFFER: Dutch Institute for Fundamental Energy Research, P.O. Box 6336, 5600 HH Eindhoven (Netherlands)
Description
Heavy impurities, such as tungsten (W), can exhibit strongly poloidally asymmetric density profiles in rotating or radio frequency heated plasmas. In the metallic environment of JET, the poloidal asymmetry of tungsten enhances its neoclassical transport up to an order of magnitude, so that neoclassical convection dominates over turbulent transport in the core. Accounting for asymmetries in neoclassical transport is hence necessary in the integrated modeling framework. The neoclassical drift kinetic code, NEO [E. Belli and J. Candy, Plasma Phys. Controlled Fusion P50, 095010 (2008)], includes the impact of poloidal asymmetries on W transport. However, the computational cost required to run NEO slows down significantly integrated modeling. A previous analytical formulation to describe heavy impurity neoclassical transport in the presence of poloidal asymmetries in specific collisional regimes [C. Angioni and P. Helander, Plasma Phys. Controlled Fusion 56, 124001 (2014)] is compared in this work to numerical results from NEO. Within the domain of validity of the formula, the factor for reducing the temperature screening due to poloidal asymmetries had to be empirically adjusted. After adjustment, the modified formula can reproduce NEO results outside of its definition domain, with some limitations: When main ions are in the banana regime, the formula reproduces NEO results whatever the collisionality regime of impurities, provided that the poloidal asymmetry is not too large. However, for very strong poloidal asymmetries, agreement requires impurities in the Pfirsch-Schluter regime. Within the JETTO integrated transport code, the analytical formula combined with the poloidally symmetric neoclassical code NCLASS [W. A. Houlberg et al., Phys. Plasmas 4, 3230 (1997)] predicts the same tungsten profile as NEO in certain cases, while saving a factor of one thousand in computer time, which can be useful in scoping studies. The parametric dependencies of the temperature screening reduction due to poloidal asymmetries would need to be better characterised for this faster model to be extended to a more general applicability. (authors)
Availability note (English)
Available from doi: http://dx.doi.org/10.1063/1.5019275Additional details
Identifiers
- DOI
- 10.1063/1.5019275;
Publishing Information
- Journal Title
- Physics of Plasmas
- Journal Volume
- 25
- Journal Issue
- no.1
- Journal Page Range
- p. 1-14
- ISSN
- 1070-664X
INIS
- Country of Publication
- United States
- Country of Input or Organization
- France
- INIS RN
- 54072915
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY; S42: ENGINEERING;
- Descriptors DEI
- ASYMMETRY; BANANA REGIME; COMPUTERIZED SIMULATION; CONTROLLED THERMONUCLEAR FUSION; CONVECTION; KINETICS; NEOCLASSICAL TRANSPORT THEORY; PFIRSCH-SCHLUETER REGIME; PLASMA; RADIOWAVE RADIATION; SYMMETRY; TUNGSTEN
- Descriptors DEC
- CHARGED-PARTICLE TRANSPORT THEORY; ELECTROMAGNETIC RADIATION; ELEMENTS; ENERGY TRANSFER; HEAT TRANSFER; MASS TRANSFER; METALS; NUCLEAR REACTIONS; NUCLEOSYNTHESIS; RADIATIONS; REFRACTORY METALS; SIMULATION; SYNTHESIS; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTIONS; TRANSITION ELEMENTS; TRANSPORT THEORY; TRAPPING
Optional Information
- Collaborations
- JET Contributors