Quasi-two-dimensional dynamics of plasmas and fluids

Publisher Website
Google Scholar
Abstract
In the lowest order of approximation quasi-two-dimensional dynamics of planetary atmospheres and of plasmas in a magnetic field can be described by a common convective vortex equation, the Charney and Hasegawa–Mima (CHM) equation. In contrast to the two-dimensional Navier–Stokes equation, the CHM equation admits ‘‘shielded vortex solutions’’ in a homogeneous limit and linear waves (‘‘Rossby waves’’ in the planetary atmosphere and ‘‘drift waves’’ in plasmas) in the presence of inhomogeneity. Because of these properties, the nonlinear dynamics described by the CHM equation provide rich solutions which involve turbulent, coherent and wave behaviors. Bringing in nonideal effects such as resistivity makes the plasma equation significantly different from the atmospheric equation with such new effects as instability of the drift wave driven by the resistivity and density gradient. The model equation deviates from the CHM equation and becomes coupled with Maxwell equations. This article reviews the linear and nonlinear dynamics of the quasi-two-dimensional aspect of plasmas and planetary atmosphere starting from the introduction of the ideal model equation (CHM equation) and extending into the most recent progress in plasma turbulence.