Probabilistic locked mode predictor in the presence of a resistive wall and finite island saturation in tokamaks

• Published in: Physics of plasmas Vol. 31; no. 3
• Main Authors: Akçay, C., Finn, John M., Brennan, Dylan P., Olofsson, K. E. J., Cole, A. J.
• Format: Journal Article
• Published: 01.03.2024
• ISSN: 1070-664X; 1089-7674
• DOI: 10.1063/5.0177827

We present a framework for estimating the probability of locking to an error field in a rotating tokamak plasma. This leverages machine learning methods trained on data from a mode-locking model, including an error field, resistive magnetohydrodynamics modeling of the plasma, a resistive wall, and an external vacuum region, leading to a fifth-order ordinary differential equation (ODE) system. It is an extension of the model without a resistive wall introduced by Akçay et al. [Phys. Plasmas 28, 082106 (2021)]. Tearing mode saturation by a finite island width is also modeled. We vary three pairs of control parameters in our studies: the momentum source plus either the error field, the tearing stability index, or the island saturation term. The order parameters are the time-asymptotic values of the five ODE variables. Normalization of them reduces the system to 2D and facilitates the classification into locked (L) or unlocked (U) states, as illustrated by Akçay et al., [Phys. Plasmas 28, 082106 (2021)]. This classification splits the control space into three regions: L ̂, with only L states; U ̂, with only U states; and a hysteresis (hysteretic) region H ̂, with both L and U states. In regions L ̂ and U ̂, the cubic equation of torque balance yields one real root. Region H ̂ has three roots, allowing bifurcations between the L and U states. The classification of the ODE solutions into L/U is used to estimate the locking probability, conditional on the pair of the control parameters, using a neural network. We also explore estimating the locking probability for a sparse dataset, using a transfer learning method based on a dense model dataset.