2021
DOI: 10.1093/mnras/stab1006
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An adaptive mesh, GPU-accelerated, and error minimized special relativistic hydrodynamics code

Abstract: We present a new special relativistic hydrodynamics (SRHD) code capable of handling coexisting ultra-relativistically hot and non-relativistically cold gases. We achieve this by designing a new algorithm for conversion between primitive and conserved variables in the SRHD solver, which incorporates a realistic ideal-gas equation of state covering both the relativistic and non-relativistic regimes. The code can handle problems involving a Lorentz factor as high as 106 and optimally avoid the catastrophic cancel… Show more

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Cited by 3 publications
(13 citation statements)
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“…where is the specific thermal energy. Note that although the GAMER code [16] that we use for our simulation runs carries out calculations in units where c = 1, we include the factors of c here for completeness. This set of equations is closed by an equation of state (EOS) h(ρ, p); the EOS that we employ in this work is the Taub-Mathews (TM) EOS [17][18][19], which is an approximation to the Synge model, the exact EOS for an ideal, non-degenerate gas composed of a single particle species [20].…”
Section: Physicsmentioning
confidence: 99%
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“…where is the specific thermal energy. Note that although the GAMER code [16] that we use for our simulation runs carries out calculations in units where c = 1, we include the factors of c here for completeness. This set of equations is closed by an equation of state (EOS) h(ρ, p); the EOS that we employ in this work is the Taub-Mathews (TM) EOS [17][18][19], which is an approximation to the Synge model, the exact EOS for an ideal, non-degenerate gas composed of a single particle species [20].…”
Section: Physicsmentioning
confidence: 99%
“…The use of the TM EOS enables the relativistic and non-relativistic gas phases to be combined in a single, realistic simulation, which cannot be achieved with a standard polytropic EOS with a single value for the ratio of specific heats Γ. For the TM EOS, Γ → 5/3 for a non-relativistic fluid and Γ → 4/3 for a relativistic fluid, and the transition between the phases occurs near k B T ∼ mc 2 (see Figure 1 of [16]).…”
Section: Physicsmentioning
confidence: 99%
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