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Pseudo-Spectrum of the Resistive Magneto-hydrodynamics Operator: Resolving the Resistive Alfven Paradox

Published 25 Mar 2018 in physics.plasm-ph, cs.NA, math-ph, math.MP, math.NA, math.SP, and physics.flu-dyn | (1803.09303v1)

Abstract: The `Alfv\'en Paradox' is that as resistivity decreases, the discrete eigenmodes do not converge to the generalized eigenmodes of the ideal Alfv\'en continuum. To resolve the paradox, the ϵ\epsilon-pseudospectrum of the RMHD operator is considered. It is proven that for any ϵ\epsilon, the ϵ\epsilon- pseudospectrum contains the Alfv\'en continuum for sufficiently small resistivity. Formal ϵpseudoeigenmodes\epsilon-pseudoeigenmodes are constructed using the formal Wentzel-Kramers-Brillouin-Jeffreys solutions, and it is shown that the entire stable half-annulus of complex frequencies with ρω<sup>2=v</sup>B(x)<sup>2\rho{|\omega|<sup>2}=|\bf{v}</sup> \cdot \bf{B}(x)|<sup>2 is resonant to order ϵ\epsilon, i.e.~belongs to the ϵpseudospectrum\epsilon-pseudospectrum. The resistive eigenmodes are exponentially ill-conditioned as a basis and the condition number is proportional to exp(RM<sup>1</sup>2)\exp(R_M<sup>{1\over</sup> 2}), where RMR_M is the magnetic Reynolds number.

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