Abstract
M3D-C1, a code for solving the linear and non-linear extended-MHD equations in toroidal geometry, is used to model pellet ELM triggering in DIII-D ITER-like plasmas. Understanding of the physical mechanisms of ELM triggering and improved modeling are required for confident extrapolation to ITER and beyond. M3D-C1 results run in linear 2D mode show that the localized perturbation is due to the pellet destabilizing peeling-ballooning modes. Calculations of linear peeling-ballooning stability as a function of pellet size suggest that a 2D pellet density ring underestimates the effects of the pellet.
| Original language | English (US) |
|---|---|
| State | Published - 2019 |
| Event | 46th European Physical Society Conference on Plasma Physics, EPS 2019 - Milan, Italy Duration: Jul 8 2019 → Jul 12 2019 |
Conference
| Conference | 46th European Physical Society Conference on Plasma Physics, EPS 2019 |
|---|---|
| Country/Territory | Italy |
| City | Milan |
| Period | 7/8/19 → 7/12/19 |
All Science Journal Classification (ASJC) codes
- Atomic and Molecular Physics, and Optics