1996
DOI: 10.1006/jcph.1996.0121
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Shock-Capturing Approach and Nonevolutionary Solutions in Magnetohydrodynamics

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Cited by 89 publications
(73 citation statements)
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“…This is the combination of an intermediate shock and a rarefaction wave, a feature sometimes encountered in coplanar problems due to the non-strict hyperbolicity of MHD. Given its nature, it cannot be found by exact Riemann solvers, and the physical acceptability itself as a solution of the ideal MHD equations is still debated (Barmin et al 1996;Myong & Roe 1998;Torrilhon 2004). On the other hand, this feature is invariably found by means of any numerical scheme, where some sort of dissipation, either physical or numerical, is always present.…”
Section: Shock Tube With Gauge Effectsmentioning
confidence: 99%
“…This is the combination of an intermediate shock and a rarefaction wave, a feature sometimes encountered in coplanar problems due to the non-strict hyperbolicity of MHD. Given its nature, it cannot be found by exact Riemann solvers, and the physical acceptability itself as a solution of the ideal MHD equations is still debated (Barmin et al 1996;Myong & Roe 1998;Torrilhon 2004). On the other hand, this feature is invariably found by means of any numerical scheme, where some sort of dissipation, either physical or numerical, is always present.…”
Section: Shock Tube With Gauge Effectsmentioning
confidence: 99%
“…In the ideal MHD model, the finitevolume method is used, and the numerical flux is evaluated by the total variation diminishing (TVD) Lax-Friedrich scheme. 13) In order to achieve third-order accuracy in space and second-order accuracy in time, monotone upstreamcentered schemes conservation laws (MUSCL) interpolation and second-order Rung-Kutta time integration are used. In addition, with a view to realize the TVD condition, a minimal model (MINMOD) limiter is used.…”
Section: Simulation Codementioning
confidence: 99%
“…They also demonstrated numerically that the intermediate shock does not emerge if coplanarity of the solution is broken by inserting a thin layer within which the magnetic field rotates continuously. Barmin et al (1996), on the other hand, found numerically that the compound wave breaks into a rotational discontinuity and a slow shock if the exact coplanarity is perturbed. Although Falle & Komissarov (2001) agreed with Wu (1990) that the temporary survival of 1 → 3, 2 → 4 and 1 → 4 shocks in their interactions with Alfvén waves is due to the non-unique shock structures, it was claimed that they should be regarded as transients.…”
Section: Introductionmentioning
confidence: 99%