Estimates of global recycling coefficients for LTX-β discharges

A. Maan, D. P. Boyle, R. Majeski, G. J. Wilkie, M. Francisquez, S. Banerjee, R. Kaita, R. Maingi, B. P. LeBlanc, S. Abe, E. Jung, E. Perez, W. Capecchi, E. T. Ostrowski, D. B. Elliott, C. Hansen, S. Kubota, V. Soukhanovskii, L. Zakharov

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4 Scopus citations

Abstract

We report the first observation of global recycling coefficient R near 0.5 in the Lithium Tokamak eXperiment-β (LTX-β), significantly below the minimum R previously reported in other devices. In a series of experiments with varied Li wall conditioning, estimates of the recycling coefficient have been made using a Lyman-α array and DEGAS2 modeling. A progressive reduction in Lyman-α emission with increased lithium and an increase in edge electron temperature are observed. It is also observed that with increasing Li coating thickness, the effective particle confinement time τ p * is reduced and approaches TRANSP calculated energy confinement time (τE), with τ p * near τ E , TRANSP for the lowest recycling coefficients. Edge temperatures approaching core plasma temperatures, first reported in LTX, can now be directly connected to estimates of the recycling coefficient and qualitatively agree with previous UEDGE simulations. The particle flux to the limiting surfaces appears to be significantly reduced in comparison with fluid scrape-off layer (SOL) models, indicating that a large fraction of the SOL ions are mirror trapped. SOL collisionality drops more than an order of magnitude below the banana regime boundary, indicating the importance of kinetic effects. Full-f 1x2v gyrokinetic simulations of SOL field lines with the GKEYLL code indicate that the fraction of ions trapped along field lines increases as collisionality drops, as a result of increased lithium evaporation.

Original languageEnglish
Article number022505
JournalPhysics of Plasmas
Volume31
Issue number2
DOIs
StatePublished - Feb 1 2024

Funding

The authors acknowledge support from the entire past and present LTX-β team, especially J. Armeli, D. Corl, T. Kozub, E. Merino, F. Rabanales, P. Sloboda, and G. Zimmer. This material is based on the work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, under Award Nos. DE-AC02-09CH11466, DE-AC05-00OR22725, DE-AC52-07NA27344, DE-SC0023481, DE-SC0019006, DE-SC0019239, and DE-SC0019308. 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. The authors acknowledge support from the entire past and present LTX-β team, especially J. Armeli, D. Corl, T. Kozub, E. Merino, F. Rabanales, P. Sloboda, and G. Zimmer. This material is based on the work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, under Award Nos. DE-AC02-09CH11466, DE-AC05-00OR22725, DE-AC52-07NA27344, DE-SC0023481, DE-SC0019006, DE-SC0019239, and DE-SC0019308. 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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