Neoclassical transport in strong gradient regions
POSTER
Abstract
We present a new model to describe neoclassical transport in strong gradient regions in tokamaks such as internal transport barriers and the pedestal. Previous work on neoclassical transport across transport barriers assumed large density and potential gradients but a small temperature gradient or neglected the gradient of the mean parallel flow. Using a large aspect ratio and low collisionality expansion, we relax these restrictive assumptions and keep gradient scale lengths that are of the size of the poloidal gyroradius. The poloidally varying part of the electric potential is retained because it is sufficiently large that it can detrap particles or trap them on the high-field side. We derive equations describing the neoclassical transport of particles, parallel momentum and energy by ions in the banana regime. We show that the resulting transport is dominated by the trapped. Even so, passing particles cannot be neglected because they determine the poloidally varying piece of the electric potential which modifies the transport coefficients. We find that a non-zero neoclassical particle flux requires parallel momentum input which could be provided through interaction with turbulence or impurities. Solutions to our transport equations are highly sensitive to the choice of sources and boundary conditions and do not always exist.
Publication: S. Trinczek, F. I. Parra, et al., J. Plasma Phys. 89, 905890304, (2023)
Presenters
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Silvia Trinczek
Princeton Plasma Physics Laboratory
Authors
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Silvia Trinczek
Princeton Plasma Physics Laboratory
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Felix I Parra
Princeton Plasma Physics Laboratory
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Peter J Catto
Massachusetts Institute of Technology
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Iván Calvo
Laboratorio Nacional de Fusión, CIEMAT, Spain, CIEMAT
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Matt Landreman
University of Maryland