A two-dimensional isothermal collisional drift-wave turbulence model including magnetic fluctuations is studied numerically. The model has as limits the electrostatic collisional drift-wave and two-dimensional magnetohydrodynamic systems. The electromagnetic and electrostatic regimes for thermal gradient-driven (drift-wave) turbulence are decided by the parameter β̂=(4πnT/B2)(L2s/L2n), where Ls and Ln are the parallel and background profile scale lengths, respectively. Significant electromagnetic effects were found only for β̂∼10 for most parameters, and were most pronounced in the strongly adiabatic regime for drift waves. The principal effect of the magnetic fluctuations is magnetic induction in the parallel force balance for electrons, which is linear. This diminishes the adiabaticity of the system by reducing the immediacy of the dissipative coupling between the density and electrostatic potential fluctuations. The transport was still found to be dominantly electrostatic even for β̂=10, although its level decreased with β̂ due to reduced coherency in the coupling between E×B velocity and density fluctuations.
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Camargo et al. (1996) studied this question.
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