{ "id": "1804.05210", "version": "v1", "published": "2018-04-14T12:18:06.000Z", "updated": "2018-04-14T12:18:06.000Z", "title": "Non-resistive dissipative magnetohydrodynamics from the Boltzmann equation in the 14-moment approximation", "authors": [ "Gabriel S. Denicol", "Xu-Guang Huang", "Etele Molnár", "Gustavo M. Monteiro", "Harri Niemi", "Jorge Noronha", "Dirk H. Rischke", "Qun Wang" ], "comment": "17 pages, 2 figures", "categories": [ "nucl-th", "hep-ph", "physics.flu-dyn" ], "abstract": "We derive the equations of motion of relativistic, non-resistive, second-order dissipative magnetohydrodynamics from the Boltzmann equation using the method of moments. We assume the fluid to be composed of a single type of point-like particles with vanishing dipole moment or spin, so that the fluid has vanishing magnetization and polarization. We also assume the fluid to be non-resistive, which allows to express the electric field in terms of the magnetic field. We derive equations of motion for the irreducible moments of the deviation of the single-particle distribution function from local thermodynamical equilibrium. We analyze the Navier-Stokes limit of these equations, reproducing previous results for the structure of the first-order transport coefficients. Finally, we truncate the system of equations for the irreducible moments using the 14-moment approximation, deriving the equations of motion of relativistic, non-resistive, second-order dissipative magnetohydrodynamics. We also give expressions for new transport coefficients appearing due to the coupling of the magnetic field to the dissipative quantities.", "revisions": [ { "version": "v1", "updated": "2018-04-14T12:18:06.000Z" } ], "analyses": { "keywords": [ "boltzmann equation", "non-resistive dissipative magnetohydrodynamics", "approximation", "second-order dissipative magnetohydrodynamics", "magnetic field" ], "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable" } } }