TY - JOUR
T1 - Coupled simulation of kinetic pedestal growth and MHD ELM crash
AU - Park, G.
AU - Cummings, J.
AU - Chang, C. S.
AU - Podhorszki, N.
AU - Klasky, S.
AU - Ku, S.
AU - Pankin, A.
AU - Samtaney, R.
AU - Shoshani, A.
AU - Snyder, P.
AU - Strauss, H.
AU - Sugiyama, L.
PY - 2007/7/1
Y1 - 2007/7/1
N2 - Edge pedestal height and the accompanying ELM crash are critical elements of ITER physics yet to be understood and predicted through high performance computing. An entirely self-consistent first principles simulation is being pursued as a long term research goal, and the plan is planned for completion in time for ITER operation. However, a proof-of-principle work has already been established using a computational tool that employs the best first principles physics available at the present time. A kinetic edge equilibrium code XGC0, which can simulate the neoclassically dominant pedestal growth from neutral ionization (using a phenomenological residual turbulence diffusion motion superposed upon the neoclassical particle motion) is coupled to an extended MHD code M3D, which can perform the nonlinear ELM crash. The stability boundary of the pedestal is checked by an ideal MHD linear peeling-ballooning code, which has been validated against many experimental data sets for the large scale (type I) ELMs onset boundary. The coupling workflow and scientific results to be enabled by it are described.
AB - Edge pedestal height and the accompanying ELM crash are critical elements of ITER physics yet to be understood and predicted through high performance computing. An entirely self-consistent first principles simulation is being pursued as a long term research goal, and the plan is planned for completion in time for ITER operation. However, a proof-of-principle work has already been established using a computational tool that employs the best first principles physics available at the present time. A kinetic edge equilibrium code XGC0, which can simulate the neoclassically dominant pedestal growth from neutral ionization (using a phenomenological residual turbulence diffusion motion superposed upon the neoclassical particle motion) is coupled to an extended MHD code M3D, which can perform the nonlinear ELM crash. The stability boundary of the pedestal is checked by an ideal MHD linear peeling-ballooning code, which has been validated against many experimental data sets for the large scale (type I) ELMs onset boundary. The coupling workflow and scientific results to be enabled by it are described.
UR - https://www.scopus.com/pages/publications/36049027694
UR - https://www.scopus.com/inward/citedby.url?scp=36049027694&partnerID=8YFLogxK
U2 - 10.1088/1742-6596/78/1/012087
DO - 10.1088/1742-6596/78/1/012087
M3 - Article
AN - SCOPUS:36049027694
SN - 1742-6588
VL - 78
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 1
M1 - 012087
ER -