Bulletin of the American Physical Society
65th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 30–November 3 2023; Denver, Colorado
Session BP11: Poster Session I:
Fundamental: Magnetic Reconnection; Dusty plasmas & Nanoparticle synthesis
ICF measurement and analysis
Space plasma physics
MFE: Disruptions avoidance and mitigation; Whole device modeling and reactor technologies
9:30 AM - 12:30 PM
Monday, October 30, 2023
Room: Plaza ABC
Abstract: BP11.00099 : Probabilistic locked mode predictor in the presence of a resistive wall and finite island saturation*
Presenter:
John M Finn
(Tibbar Plasma Technologies)
Authors:
John M Finn
(Tibbar Plasma Technologies)
Dylan Brennan
(Two Hathaway Research)
Cihan Akcay
(General Atomics)
Andrew Cole
(No affiliation)
We present a framework for estimating the locking probability for a rotating tokamak plasma with an error field. This approach uses machine learning methods trained on the results of a reduced mode-locking model, which includes a resistive MHD model of the plasma, a resistive wall (RW), an external vacuum region, and an error field, leading to a 5th order ODE system. It is an extension of the third order model without a RW introduced in Ref. 1. A saturation model for the tearing perturbation by finite island width is also included. We choose two control parameters, the applied torque and an error field. The order parameters are the five time-asymptotic values of the dependent variables. We show that a normalization of these order parameters allows the classification of states as locked (L) or unlocked (U) in terms of only two order parameters and improves a clustering algorithm for the classification. This classification splits the control parameter space into 3 distinct regions: only L states, only U states, and a hysteresis H region, with both L and U states. This classification is then used to estimate the locking probability, conditional on the control parameters, using a neural network. This conditional probability is between 0 and 1 in the H region. We also explore using different pairs of control parameters and explore finding an estimate of the locking probability for a sparse data set, using a transfer learning method based on a dense model data set.
*This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, Theory Program under Awards DE-FG02-95ER54309, DE-SC0019016, and DE-SC0022031. This material is also based upon work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Award 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.
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