Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session TI2: Pedestal, LH Transition, Non-Inductive Startup
9:30 AM–12:30 PM,
Thursday, November 8, 2018
OCC
Room: Oregon Ballroom 203
Chair: Jerry Hughes, Massachusetts Institute of Technology
Abstract ID: BAPS.2018.DPP.TI2.2
Abstract: TI2.00002 : Self-consistent pedestal prediction for JET
10:00 AM–10:30 AM
Presenter:
Samuli Saarelma
(CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, UK)
Author:
Samuli Saarelma
(CCFE, Culham Science Centre, Abingdon, Oxon OX14 3DB, UK)
In H-mode plasmas the energy confinement is strongly linked to pressure pedestal height (pped). At the same time, the core pressure has a stabilising effect on the peeling-ballooning modes (PBM) that limit pped. Therefore, in a truly predictive model the core and pedestal have to be resolved self-consistently.
The most widely used model for pedestal predictions, EPED requires advance knowledge of the density pedestal (nped) and the global beta which are not available when predicting future experiments. We have further developed the EPED model to incorporate
self-consistent modelling of core transport and nped along with pped.
For the prediction of nped, we have used a model based on neutral penetration. While this model lacks the important contribution of inter-ELM pedestal transport, it is able to predict nped in a large JET-ILW database with an average of 22% error. For the self-consistent core and pedestal prediction we use heating power as input and couple pedestal prediction with BohmgyroBohm transport model. For experimental JET plasmas found at the PBM stability limit this method accurately predicts both the pedestal and core as long as fast particle pressure is included in the prediction. When the experimental pedestals are not limited by PBMs, the pedestal height is overpredicted.
We also investigated the effect of the mass of the main ion isotope (mi) on the pedestal prediction. The isotope affects directly the diamagnetic stabilisation of the PBMs. This alone does not explain the higher pedestals of deuterium plasmas compared to hydrogen. However, the experimental density pedestal increases with mi (both nsep and nped increase from H to D). With these changes
imposed to the density pedestal pped is well predicted suggesting that the main isotope effect in JET-ILW H-mode is through the modification of nped that in turn affects pped prediction.
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To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.TI2.2
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