A dissipative extension to ideal hydrodynamics

ABSTRACT We present a formulation of special relativistic dissipative hydrodynamics (SRDHD) derived from the well-established Müller–Israel–Stewart (MIS) formalism using an expansion in deviations from ideal behaviour. By re-summing the non-ideal terms, our approach extends the Euler equations of motion for an ideal fluid through a series of additional source terms that capture the effects of bulk viscosity, shear viscosity, and heat flux. For efficiency these additional terms are built from purely spatial derivatives of the primitive fluid variables. The series expansion is parametrized by the dissipation strength and time-scale coefficients, and is therefore rapidly convergent near the ideal limit. We show, using numerical simulations, that our model reproduces the dissipative fluid behaviour of other formulations. As our formulation is designed to avoid the numerical stiffness issues that arise in the traditional MIS formalism for fast relaxation time-scales, it is roughly an order of magnitude faster than standard methods near the ideal limit.

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Publication Details

Journal
Monthly Notices of the Royal Astronomical Society
Published
2024-10-07
DOI
https://doi.org/10.1093/mnras/stae2284
Citations
3
Primary Topic
Advanced Thermodynamics and Statistical Mechanics
Type
article
Field-Weighted Citation Impact
0.84

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article

A dissipative extension to ideal hydrodynamics

Ian Hawke, M. J. Hatton
3 citations
Monthly Notices of the Royal Astronomical Society
Advanced Thermodynamics and Statistical Mechanics
0.84
article

A dissipative extension to ideal hydrodynamics

Ian Hawke, M. J. Hatton
article en
3 citations

Abstract

ABSTRACT We present a formulation of special relativistic dissipative hydrodynamics (SRDHD) derived from the well-established Müller–Israel–Stewart (MIS) formalism using an expansion in deviations from ideal behaviour. By re-summing the non-ideal terms, our approach extends the Euler equations of motion for an ideal fluid through a series of additional source terms that capture the effects of bulk viscosity, shear viscosity, and heat flux. For efficiency these additional terms are built from purely spatial derivatives of the primitive fluid variables. The series expansion is parametrized by the dissipation strength and time-scale coefficients, and is therefore rapidly convergent near the ideal limit. We show, using numerical simulations, that our model reproduces the dissipative fluid behaviour of other formulations. As our formulation is designed to avoid the numerical stiffness issues that arise in the traditional MIS formalism for fast relaxation time-scales, it is roughly an order of magnitude faster than standard methods near the ideal limit.

Monthly Notices of the Royal Astronomical SocietyVol. 535(1)
University of Southampton (GB)
Science and Technology Facilities Council
Openalex Percentile: Top 28%
Advanced Thermodynamics and Statistical Mechanics
0.84
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