Abstract:Using a numerical simulation, we study the effects of ambipolar diffusion and ohmic diffusion on the magnetic field evolution in the interior of an isolated neutron star. We are interested in the behavior of the magnetic field on a long time scale, over which all Alfvén and sound waves have been damped. We model the stellar interior as an electrically neutral plasma composed of neutrons, protons and electrons, which can interact with each other through collisions and electromagnetic forces. Weak interactions c… Show more
“…It may be more efficient to incorporate the developed formalism in the framework of an existing code instead of developing a new code from scratch. Possible existing codes are described in Mignone et al (2010), Igumenshchev, Narayan & Abramowicz (2003) and Hoyos, Reisenegger & Valdivia (2007). Applications of this study may be useful to both linear and nonlinear stability analysis of known barotropic MHD configurations (Bernstein et al 1958;Almaguer et al 1988;Katz et al 1993;Yahalom, Katz & Inagaki 1994;Vladimirov, Moffatt & Ilin 1996, 1997, 1999Yahalom 2011).…”
“…It may be more efficient to incorporate the developed formalism in the framework of an existing code instead of developing a new code from scratch. Possible existing codes are described in Mignone et al (2010), Igumenshchev, Narayan & Abramowicz (2003) and Hoyos, Reisenegger & Valdivia (2007). Applications of this study may be useful to both linear and nonlinear stability analysis of known barotropic MHD configurations (Bernstein et al 1958;Almaguer et al 1988;Katz et al 1993;Yahalom, Katz & Inagaki 1994;Vladimirov, Moffatt & Ilin 1996, 1997, 1999Yahalom 2011).…”
“…Possible existing codes are described in Igumenshchev, Narayan & Abramowicz (2003), Miyoshi & Kusano (2005), Faber et al. (2006), Hoyos, Reisenegger & Valdivia (2007), Mignone et al. (2010).…”
Section: Resultsmentioning
confidence: 99%
“…It may be more efficient to incorporate the developed formalism in the frame work of an existing code instead of developing a new code from scratch. Possible existing codes are described in Igumenshchev, Narayan & Abramowicz (2003), Miyoshi & Kusano (2005), Faber et al (2006), Hoyos, Reisenegger & Valdivia (2007), Mignone et al (2010). I anticipate applications of this study both to linear and nonlinear stability analyses of known barotropic magnetohydrodynamic configurations (Bernstein et al 1958;Almaguer et al 1988;Vladimirov et al 1996Vladimirov et al , 1997Vladimirov et al , 1999.…”
Section: Resultsmentioning
confidence: 99%
“…It may be more efficient to incorporate the developed formalism in the frame work of an existing code instead of developing a new code from scratch. Possible existing codes are described in [15,16,17,18,19]. I anticipate applications of this study both to linear and non-linear stability analysis of known barotropic magnetohydrodynamic configurations [20,21,22].…”
Variational principles for magnetohydrodynamics were introduced by previous authors both in Lagrangian and Eulerian form. In this paper we introduce simpler Eulerian variational principles from which all the relevant equations of non-barotropic magnetohydrodynamics can be derived. The variational principle is given in terms of five independent functions for non-stationary barotropic flows. This is less then the eight variables which appear in the standard equations of barotropic magnetohydrodynamics which are the magnetic field B the velocity field v, the entropy s and the density ρ.
“…We shall now show that a velocity field given by equation ( 19), such that the equations for α, β, χ, η, ν, σ, s satisfy the corresponding equations (16,21,25,27) must satisfy Euler's equations. Let us calculate the material derivative of ⃗ v:…”
The current paper is devoted to the introduction of simpler Eulerian variational principles from which all the relevant equations of non-barotropic stationary magnetohydrodynamics can be derived for magnetic fields which lie on surfaces. A variational principle is given in terms of three independent variables for stationary non-barotropic magnetohydrodynamic flows. This is a smaller number of variables than the eight variables which appear in the standard equations of non-barotropic magnetohydrodynamics which are the magnetic field, the velocity field, the specific entropy and the density. We further investigate the case in which the flow along magnetic lines is not ideal.
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