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Updated: May 29, 2026

Magnetically Induced Rotating Rayleigh-Taylor Instability
Published on: March 3, 2017
Alfvén waves and ideal two-dimensional Galerkin truncated magnetohydrodynamics
Giorgio Krstulovic1, Marc-Etienne Brachet, Annick Pouquet
1Laboratoire de Physique Statistique de l'École Normale Supérieure, associé au CNRS et aux Universités Paris VI et VII, Paris, France.
Numerical simulations reveal that 2D Euler and ideal magnetohydrodynamics (MHD) flows exhibit distinct energy spectra and lack pseudodissipation. Imposing a magnetic field slows down scale equilibration in MHD turbulence.
Area of Science:
- Fluid Dynamics
- Plasma Physics
- Computational Physics
Background:
- Understanding turbulence in fluid and magnetohydrodynamic systems is crucial.
- Two-dimensional (2D) systems offer simplified models for complex turbulent phenomena.
- Statistical equilibria and conserved quantities are well-defined in truncated 2D models.
Purpose of the Study:
- To numerically investigate the dynamics of 2D Euler and ideal magnetohydrodynamics (MHD) flows.
- To analyze energy spectra, scale interactions, and dissipation ranges.
- To examine the effect of a uniform magnetic field on MHD turbulence.
Main Methods:
- Numerical simulations of 2D Euler and ideal MHD flows.
- Utilizing systems with a finite number of modes up to 4096^2.
- Employing the Orszag-Tang vortex initial condition with a neutral X point.
Main Results:
- Observed energy spectra E(k)~k^(-3/2) in MHD, indicating eddy-wave interactions.
- No pseudodissipative range was visible in either Euler or ideal 2D MHD.
- A uniform magnetic field slowed down scale equilibration and prevented saturation in MHD.
Conclusions:
- The absence of pseudodissipation in 2D Euler may relate to vanishing turbulent viscosity.
- In 2D MHD, insufficient numerical resolution might explain the lack of a pseudodissipative range.
- Magnetic fields significantly alter the dynamics of 2D turbulence, affecting scale formation and equilibration.
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