Multi-fluid and kinetic models of partially ionized magnetic reconnection
Abstract
Magnetic reconnection in partially ionized plasmas is a ubiquitous and important phenomenon in both laboratory and astrophysical systems. Here, simulations of partially ionized magnetic reconnection with well-matched initial conditions are performed using both multi-fluid and fully-kinetic approaches. Despite similar initial conditions, the time-dependent evolution differs between the two models. In multi-fluid models, the reconnection rate locally obeys either a decoupled Sweet–Parker scaling, where neutrals are unimportant, or a fully coupled Sweet–Parker scaling, where neutrals and ions are strongly coupled, depending on the resistivity. In contrast, kinetic models show a faster reconnection rate that is proportional to the fully-coupled, bulk Alfvén speed, $$v^*_A$$. In this work, these differences are interpreted as the result of operating in different collisional regimes. Multi-fluid simulations are found to maintain $$ν_{ni}L/v^*_A$$ ≳1, where $$ν_{ni}$$ is the neutral–ion collision frequency and L is the time-dependent current sheet half-length. This strongly couples neutrals to the reconnection outflow, while kinetic simulations evolve to allow $$ν_{ni}L/v^*_A$$ <1, decoupling neutrals from the reconnection outflow. Differences in the way reconnection is triggered may explain these discrepancies.
- Authors:
-
- Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
- Harvard and Smithsonian, Cambridge, MA (United States)
- Publication Date:
- Research Org.:
- Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States); Argonne National Laboratory (ANL), Argonne, IL (United States). Argonne Leadership Computing Facility (ALCF)
- Sponsoring Org.:
- National Aeronautics and Space Administration (NASA); National Science Foundation (NSF); USDOE Office of Science (SC)
- OSTI Identifier:
- 1804609
- Alternate Identifier(s):
- OSTI ID: 1776994
- Grant/Contract Number:
- AC02-09CH11466; H-TIDES NNH15AB29I; S014981-F; 1931388; 80NSSC18K1124; 80NSSC20K0174; NNM07AB07C; AC02-06CH11357; AC0209CH11466.
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Physics of Plasmas
- Additional Journal Information:
- Journal Volume: 28; Journal Issue: 4; Journal ID: ISSN 1070-664X
- Publisher:
- American Institute of Physics (AIP)
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; Atomic and molecular collisions; Thermodynamic states and processes; Computational fluid dynamics; Energy equations; Charge exchange reactions; Particle-in-cell method; Plasma properties and parameters; Magnetic reconnection; Collisional processes; Partially ionized plasma
Citation Formats
Jara-Almonte, J., Murphy, N. A., and Ji, H. Multi-fluid and kinetic models of partially ionized magnetic reconnection. United States: N. p., 2021.
Web. doi:10.1063/5.0039860.
Jara-Almonte, J., Murphy, N. A., & Ji, H. Multi-fluid and kinetic models of partially ionized magnetic reconnection. United States. https://doi.org/10.1063/5.0039860
Jara-Almonte, J., Murphy, N. A., and Ji, H. Tue .
"Multi-fluid and kinetic models of partially ionized magnetic reconnection". United States. https://doi.org/10.1063/5.0039860. https://www.osti.gov/servlets/purl/1804609.
@article{osti_1804609,
title = {Multi-fluid and kinetic models of partially ionized magnetic reconnection},
author = {Jara-Almonte, J. and Murphy, N. A. and Ji, H.},
abstractNote = {Magnetic reconnection in partially ionized plasmas is a ubiquitous and important phenomenon in both laboratory and astrophysical systems. Here, simulations of partially ionized magnetic reconnection with well-matched initial conditions are performed using both multi-fluid and fully-kinetic approaches. Despite similar initial conditions, the time-dependent evolution differs between the two models. In multi-fluid models, the reconnection rate locally obeys either a decoupled Sweet–Parker scaling, where neutrals are unimportant, or a fully coupled Sweet–Parker scaling, where neutrals and ions are strongly coupled, depending on the resistivity. In contrast, kinetic models show a faster reconnection rate that is proportional to the fully-coupled, bulk Alfvén speed, $v^*_A$. In this work, these differences are interpreted as the result of operating in different collisional regimes. Multi-fluid simulations are found to maintain $ν_{ni}L/v^*_A$ ≳1, where $ν_{ni}$ is the neutral–ion collision frequency and L is the time-dependent current sheet half-length. This strongly couples neutrals to the reconnection outflow, while kinetic simulations evolve to allow $ν_{ni}L/v^*_A$ <1, decoupling neutrals from the reconnection outflow. Differences in the way reconnection is triggered may explain these discrepancies.},
doi = {10.1063/5.0039860},
journal = {Physics of Plasmas},
number = 4,
volume = 28,
place = {United States},
year = {Tue Apr 13 00:00:00 EDT 2021},
month = {Tue Apr 13 00:00:00 EDT 2021}
}
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