Hostname: page-component-669899f699-ggqkh Total loading time: 0 Render date: 2025-05-04T23:16:24.193Z Has data issue: false hasContentIssue false
Accepted manuscript

Enhanced Collisional Losses from a Magnetic Mirror Using the Lenard-Bernstein Collision Operator

Published online by Cambridge University Press:  30 April 2025

Maxwell H. Rosen*
Affiliation:
Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08540, USA
W. Sengupta
Affiliation:
Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08540, USA
I. Ochs
Affiliation:
Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08540, USA
F. I. Parra
Affiliation:
Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08540, USA Princeton Plasma Physics Laboratory, Princeton, NJ 08540, USA
G. W. Hammett
Affiliation:
Princeton Plasma Physics Laboratory, Princeton, NJ 08540, USA
*
Email address for correspondence: [email protected]
Rights & Permissions [Opens in a new window]

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

Collisions are crucial in governing particle and energy transport in plasmas confined in a magnetic mirror trap. Modern gyrokinetic codes model transport in magnetic mirrors, but some utilize approximate model collision operators. This study focuses on a Pastukhov-style method of images calculation of particle and energy confinement times using a Lenard-Bernstein model collision operator. Prior work on parallel particle and energy balances used a different Fokker-Planck plasma collision operator. The method must be extended in non-trivial ways to study the Lenard-Bernstein operator. To assess the effectiveness of our approach, we compare our results with a modern finite element solver. Our findings reveal that the particle confinement time scales like a exp(a2) using the Lenard-Bernstein operator, in contrast to the more accurate scaling that the Coulomb collision operator would yield a2 exp(a2), where a2 is approximately proportional to the ambipolar potential. We propose that codes solving for collisional losses in magnetic mirrors utilizing the Lenard-Bernstein or Dougherty collision operator scale their collision frequency of any electrostatically confined species. This study illuminates the collision operator’s intricate role in the Pastukhov-style method of images calculation of collisional confinement.

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press