Generalized fluid theory including non-Maxwellian kinetic effects
Olivier Izacard

TL;DR
This paper develops a generalized fluid theory that incorporates non-Maxwellian kinetic effects, enabling more accurate and computationally efficient modeling of plasma turbulence and transport phenomena.
Contribution
It introduces a minimal set of fluid equations with analytic non-Maxwellian distribution functions, bridging the gap between kinetic and fluid models in plasma physics.
Findings
Derived fluid closures from Landau Fokker-Planck operator for arbitrary collisionality
Implemented a minimal INMDF fluid model to simulate particle and heat diffusion
Identified the origin of diffusion as a competition between INMDF growth and thermalization
Abstract
The results obtained by the plasma physics community for the validation and the prediction of turbulence and transport in magnetized plasma come mainly from the use of very CPU-consuming particle-in-cell or (gyro)kinetic codes which naturally include non-Maxwellian kinetic effects. To date, fluid codes are not considered to be relevant for the description of these kinetic effects. Here, after revisiting the limitations of the current fluid theory developed in the 19th century, we generalize the fluid theory including kinetic effects such as non-Maxwellian super-thermal tails with as few fluid equations as possible. The collisionless and collisional fluid closures from the nonlinear Landau Fokker-Planck collision operator are shown for an arbitrary collisionality. Indeed, the first fluid models associated with two examples of collisionless fluid closures are obtained by assuming an…
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