2003
DOI: 10.1051/0004-6361:20021641
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An efficient shock-capturing central-type scheme for multidimensional relativistic flows

Abstract: Abstract.A third order shock-capturing numerical scheme for three-dimensional special relativistic magnetohydrodynamics (3-D RMHD) is presented and validated against several numerical tests. The simple and efficient central scheme described in Paper I (Del Zanna & Bucciantini 2002) for relativistic hydrodynamics is here extended to the magnetic case by following the strategies prescribed for classical MHD by Londrillo & Del Zanna (2000). The scheme completely avoids spectral decomposition into characteristic w… Show more

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Cited by 247 publications
(367 citation statements)
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References 35 publications
(49 reference statements)
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“…All calculations were performed using the Godunov code ) based on the essentially non-oscillatory (ENO) spatial reconstruction, Harten-Lax-van-Leer (HLL) approximate Riemann-solver, Runge-Kutta (RK) time integration (Del Zanna et al 2003) to solve isothermal MHD equations, and constrained transport method (Evans & Hawley 1988) to keep a zero magnetic field divergence. The computational domain covers 30 kpc × 30 kpc × 7.5 kpc of space with 512×512×128 cells of a 3D cartesian grid, which yields about 60 pc of spatial resolution in each direction.…”
Section: Methodsmentioning
confidence: 99%
“…All calculations were performed using the Godunov code ) based on the essentially non-oscillatory (ENO) spatial reconstruction, Harten-Lax-van-Leer (HLL) approximate Riemann-solver, Runge-Kutta (RK) time integration (Del Zanna et al 2003) to solve isothermal MHD equations, and constrained transport method (Evans & Hawley 1988) to keep a zero magnetic field divergence. The computational domain covers 30 kpc × 30 kpc × 7.5 kpc of space with 512×512×128 cells of a 3D cartesian grid, which yields about 60 pc of spatial resolution in each direction.…”
Section: Methodsmentioning
confidence: 99%
“…In this case, roughly speaking, there are two options for numerically handling the transport terms [38]. One is to use the Godunov-type, approximate Riemann solver [39,40], and the other is to use the high-resolution central (HRC) scheme [41,20]. We adopt a HRC scheme proposed by Kurganov and Tadmor [42] and very recently used in special relativistic simulations by LucasSarrano et al [43].…”
Section: Numerical Scheme For Solving Grmhd Equationsmentioning
confidence: 99%
“…The parameters for the initial conditions adopted here are the same as those in [41]. On the other hand, we varied the grid spacing to see the convergence in contrast to the previous works.…”
Section: B Multi Dimensional Testsmentioning
confidence: 99%
“…31 and 32. A related version of the code has been designed for special relativistic 33 and general relativistic ideal MHD equations. 34 With respect to previous versions, in the code an explicit plasma resistivity has been introduced and space resolution has been improved by using high-order compact ͑or implicit͒ difference schemes 30 to approximate flux derivatives.…”
Section: The Numerical Schemementioning
confidence: 99%