Recent progress in the quantitative validation of JOREK simulations of ELMs in JET

Future devices like JT-60SA, ITER and DEMO require quantitative predictions of pedestal density and temperature levels, as well as inter-ELM and ELM divertor heat fluxes, in order to improve global confinement capabilities while preventing divertor erosion/melting in the planning of future experimen...

Descripción completa

Detalles Bibliográficos
Autores: Pamela, S.J.P., Huijsmans, G.T.A., Eich, T., Saarelma, Samuli, Lupelli, I., Maggi, C.F., Giroud, C., Chapman, I.T., Smith, S.F., Frassinetti, L., Becoulet, M., Hoelzl, M., Orain, F., Futatani, S., JET Contributors
Tipo de recurso: artículo
Fecha de publicación:2017
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/104779
Acceso en línea:https://hdl.handle.net/2117/104779
https://dx.doi.org/10.1088/1741-4326/aa6e2a
Access Level:acceso abierto
Palabra clave:Plasma dynamics
JET-ILW
ELM
Pedestal
MHD
Peeling ballooning modes
JOREK
Simulations
Tècniques de plasma
Àrees temàtiques de la UPC::Enginyeria biomèdica
Descripción
Sumario:Future devices like JT-60SA, ITER and DEMO require quantitative predictions of pedestal density and temperature levels, as well as inter-ELM and ELM divertor heat fluxes, in order to improve global confinement capabilities while preventing divertor erosion/melting in the planning of future experiments. Such predictions can be obtained from dedicated pedestal models like EPED, and from non-linear MHD codes like JOREK, for which systematic validation against current experiments is necessary. In this paper, we show progress in the quantitative validation of the JOREK code using JET simulations. Results analyse the impact of diamagnetic terms on the dynamics and size of the ELMs, and evidence is provided that the onset of type-I ELMs is not governed by linear MHD stability alone, but that a nonlinear threshold could be responsible for large MHD events at the plasma edge.