Nonlinear Damping and Field-aligned Flows of Propagating Shear Alfv\'en Waves with Braginskii Viscosity

TL;DR

This paper develops a nonlinear theory for shear Alfvén wave damping in plasma, revealing that nonlinear viscous effects are significantly stronger than linear predictions but often still negligible in solar corona conditions.

Contribution

It introduces a nonlinear analysis of Braginskii MHD effects on Alfvén wave damping, highlighting the dominance of nonlinear viscous dissipation over linear predictions in realistic plasma amplitudes.

Findings

Nonlinear damping is about a billion times stronger than linear theory predicts.

Damping length depends on viscosity with an optimal value beyond which damping decreases.

Nonlinear effects are significant but often negligible in typical coronal conditions.

Abstract

Braginskii MHD provides a more accurate description of many plasma environments than classical MHD since it actively treats the stress tensor using a closure derived from physical principles. Stress tensor effects nonetheless remain relatively unexplored for solar MHD phenomena, especially in nonlinear regimes. This paper analytically examines nonlinear damping and longitudinal flows of propagating shear Alfv\'en waves. Most previous studies of MHD waves in Braginskii MHD considered the strict linear limit of vanishing wave perturbations. We show that those former linear results only apply to Alfv\'en wave amplitudes in the corona that are so small as to be of little interest, typically a wave energy less than $10^{-11}$ times the energy of the background magnetic field. For observed wave amplitudes, the Braginskii viscous dissipation of coronal Alfv\'en waves is nonlinear and a factor around $10^9$ stronger than predicted by the linear theory. Furthermore, the dominant damping occurs through the parallel viscosity coefficient $\eta_0$, rather than the perpendicular viscosity coefficient $\eta_2$ in the linearized solution. This paper develops the nonlinear theory, showing that the wave energy density decays with an envelope $(1+z/L_d)^{-1}$. The damping length $L_d$ exhibits an optimal damping solution, beyond which greater viscosity leads to lower dissipation as the viscous forces self-organise the longitudinal flow to suppress damping. Although the nonlinear damping greatly exceeds the linear damping, it remains negligible for many coronal applications.