The collisional drift wave instability in steep density gradient regimes
arXiv:1812.02430 · doi:10.1088/1741-4326/aaf6cc
Abstract
The collisional drift wave instability in a straight magnetic field configuration is studied within a full-F gyro-fluid model, which relaxes the Oberbeck-Boussinesq (OB) approximation. Accordingly, we focus our study on steep background density gradients. In this regime we report on corrections by factors of order one to the eigenvalue analysis of former OB approximated approaches as well as on spatially localised eigenfunctions, that contrast strongly with their OB approximated equivalent. Remarkably, non-modal phenomena arise for large density inhomogeneities and for all collisionalities. As a result, we find initial decay and non-modal growth of the free energy and radially localised and sheared growth patterns. The latter non-modal effect sustains even in the nonlinear regime in the form of radially localised turbulence or zonal flow amplitudes.
arXiv commentaccepted at Nuclear Fusion
References in corpus (11)
- Bifurcation in electrostatic resistive drift wave turbulence
- A New Paradigm for Turbulent Transport Across a Steep Gradient in Toroidal Plasmas
- Universal instability for wavelengths below the ion Larmor scale
- Unconventional Ballooning Structures for Toroidal Drift Waves
- Generalized universal instability: Transient linear amplification and subcritical turbulence
- Non-Oberbeck-Boussinesq zonal flow generation
- The universal instability in general geometry
- Theory of the Drift-Wave Instability at Arbitrary Collisionality
- Nonlinear Resistivity for Magnetohydrodynamical Models
- Gyrofluid vortex interaction
- Lattice Boltzmann model for collisionless electrostatic drift wave turbulence obeying Charney-Hasegawa-Mima dynamics