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28 November 2023 to 1 December 2023
IAEA Headquarters
Europe/Vienna timezone
Workshop programme now available

EFIT-AI neural network surrogates for magnetic, MSE, and kinetic equilibrium reconstruction

30 Nov 2023, 13:10
1h 30m
Conference Room 1 (CR1), C Building, 2nd floor (IAEA Headquarters)

Conference Room 1 (CR1), C Building, 2nd floor

IAEA Headquarters

Poster AI Posters Session

Speaker

Dr Cihan Akcay (General Atomics)

Description

Artificial neural network (NN) surrogate models have been developed and trained on magnetic, magnetic + motional stark effect (MSE), and kinetic DIIII-D equilibria to accelerate tokamak equilibrium reconstructions for offline, between-shot, and real-time applications. Adaptation of the ML/AI algorithms has been facilitated through the recently developed device-independent portable equilibrium solver and a large EFIT database of DIII-D magnetic, MSE and kinetic equilibria[1]. The main model comprises a fully connected NN coupled to a convolutional NN that together enforce the toroidal force-balance constraint by concurrently learning the poloidal flux and toroidal current density on the EFIT spatial grid. In addition, the NN surrogates also predict pressure, current, P', FF', and safety factor (q) profiles, and important plasma parameters such as the internal inductance, normalized beta, and magnetic axis location. Models are optimized for both architecture and hyperparameters, as well as inference speed, which has been clocked at real-time EFIT-like speeds.

The NN surrogates for the magnetic EFITs show generalizability to previously-unseen negative-triangularity shapes, by incorporating the spatial correlation among various magnetic sensors in DIII-D into the NN input vector. The magnetic + MSE surrogates show improved predictions of the q profiles, and certain plasma parameters like the internal inductance. Finally, the kinetic surrogates show additional improvements in accurately reproducing EFIT-predicted internal current and pressure profiles. These results suggest the possibility of using a surrogate model as a real-time tool for plasma control and other applications.

[1]. L. Lao et al., PPCF, 64, 074001 (2022)

This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Acquisition and Assistance under Award Number(s) DE-SC0021203 and DE-FC02-04ER54698.

This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.

Speaker's Affiliation General Atomics
Member State or IGO/NGO United States

Primary authors

Dr Cihan Akcay (General Atomics) Dr Sandeep Madireddy (Argonne National Laboratory) Dr Xuan Sun (Oakridge and Associates Unversity) Dr Torrin Bechtel (General Atomics) Joseph McClenaghan (General Atomics) Dr Anirban Samaddar (Argonne National Laboratory) Scott Kruger (Tech-X Corporation) Lang Lao (General Atomics) Yueqiang Liu (General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA)

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