2021
DOI: 10.1016/j.physleta.2021.127522
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Analysis of the Kolmogorov model with an asymptotic-preserving method

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“…In this context, the Alfvén theorem of magnetic flux conservation in an ideal MHD plasma is the mirror correspondent of the Helmholtz-Kelvin theorem of vorticity conservation in ideal hydrodynamics (Batchelor 1950;Elsasser 1950b;Truesdell 1950;Axford 1984;Greene 1993). We incidentally note that some formal similarities can be also recognised in the eigenmode analysis of resistive tearing modes and of ideal instabilities in presence of viscosity in a Kolmogorov hydrodynamic flow (Fedele, Negulescu & Ottaviani 2021). In terms of the RMHD equations above, the Lagrangian invariance of magnetic lines is expressed by the ideal limit (d e = ρ s = S −1 = 0) of (2.1), although a finite ρ s alone allows preservation of the ideal MHD topological conservation, provided a redefinition of the stream function of the velocity field U according to ϕ → ϕ − ρ 2 s ∇ 2 ϕ ).…”
Section: Magnetic Reconnection In Tearing Modes and Formation Of Magn...mentioning
confidence: 78%
“…In this context, the Alfvén theorem of magnetic flux conservation in an ideal MHD plasma is the mirror correspondent of the Helmholtz-Kelvin theorem of vorticity conservation in ideal hydrodynamics (Batchelor 1950;Elsasser 1950b;Truesdell 1950;Axford 1984;Greene 1993). We incidentally note that some formal similarities can be also recognised in the eigenmode analysis of resistive tearing modes and of ideal instabilities in presence of viscosity in a Kolmogorov hydrodynamic flow (Fedele, Negulescu & Ottaviani 2021). In terms of the RMHD equations above, the Lagrangian invariance of magnetic lines is expressed by the ideal limit (d e = ρ s = S −1 = 0) of (2.1), although a finite ρ s alone allows preservation of the ideal MHD topological conservation, provided a redefinition of the stream function of the velocity field U according to ϕ → ϕ − ρ 2 s ∇ 2 ϕ ).…”
Section: Magnetic Reconnection In Tearing Modes and Formation Of Magn...mentioning
confidence: 78%