Stellar evolution of massive stars with a radiative alpha-omega dynamo

Models of rotationally-driven dynamos in stellar radiative zones have suggested that magnetohydrodynamic transport of angular momentum and chemical composition can dominate over the otherwise purely hydrodynamic processes. A proper consideration of the interaction between rotation and magnetic fields is therefore essential. Previous studies have focused on a magnetic model where the magnetic field strength is derived as a function of the stellar structure and angular momentum distribution. We have adapted our one-dimensional stellar rotation code, RoSE, to model the poloidal and toroidal magnetic field strengths with a pair of time-dependent advection-diffusion equations coupled to the equations for the evolution of the angular momentum distribution and stellar structure. This produces a much more complete, though still reasonably simple, model for the magnetic field evolution. Our model reproduces well observed surface nitrogen enrichment of massive stars in the Large Magellanic Cloud. In particular it reproduces a population of slowly-rotating nitrogen-enriched stars that cannot be explained by rotational mixing alone alongside the traditional rotationlly-enriched stars. The model further predicts a strong mass-dependency for the dynamo-driven field. Above a threshold mass, the strength of the magnetic dynamo decreases abruptly and so we predict that more massive stars are much less likely to support a dynamo-driven field than less massive stars.

[1]  D. Sasselov,et al.  HR 5907: Discovery of the most rapidly rotating magnetic early B-type star by the MiMeS Collaboration , 2011, 1109.3157.

[2]  C. Tout,et al.  Towards a unified model of stellar rotation , 2011, 1109.0993.

[3]  Y. Ponty,et al.  Astrophysical Dynamics: From Stars to Galaxies , 2011 .

[4]  Renzo Ramelli,et al.  Solar Polarization 5: In Honor of Jan Stenflo , 2009 .

[5]  Cambridge,et al.  Modelling the binary progenitor of Supernova 1993J , 2009, 0904.0282.

[6]  T. Forveille,et al.  The surprising magnetic topology of τ Sco: fossil remnant or dynamo output? , 2006, astro-ph/0606156.

[7]  Tim J. Harries,et al.  The magnetic field and wind confinement of θ1 Orionis C , 2002 .

[8]  S. Owocki,et al.  Dynamical Simulations of Magnetically Channeled Line-driven Stellar Winds. I. Isothermal, Nonrotating, Radially Driven Flow , 2002, astro-ph/0201195.

[9]  G. Wade,et al.  The magnetic field and wind confinement of beta Cephei: new clues for interpreting the Be phenomenon? , 2001 .

[10]  Gautier Mathys,et al.  Magnetic Fields Across the Hertzsprung-Russell Diagram , 2001 .

[11]  A. Brandenburg The Inverse Cascade and Nonlinear Alpha-Effect in Simulations of Isotropic Helical Hydromagnetic Turbulence , 2000, astro-ph/0006186.

[12]  S. Woosley,et al.  Presupernova Evolution of Rotating Massive Stars. I. Numerical Method and Evolution of the Internal Stellar Structure , 1999, astro-ph/9904132.

[13]  C. Tout,et al.  CAN A DISC DYNAMO GENERATE LARGE-SCALE MAGNETIC FIELDS ? , 1996 .

[14]  C. Tout,et al.  Approximate input physics for stellar modelling , 1995, astro-ph/9504025.

[15]  J. Landstreet,et al.  The magnetic field geometry of HD 215441 , 1978 .

[16]  Peter P. Eggleton,et al.  The Evolution of low mass stars , 1971 .

[17]  E. Parker The dynamical state of the interstellar gas and field. II. , 1966 .

[18]  E. Parker Dynamics of the Interplanetary Gas and Magnetic Fields , 1958 .

[19]  H. W. Babcock Zeeman Effect in Stellar Spectra. , 1947 .

[20]  T. G. Cowling,et al.  On the Sun's general magnetic field , 1945 .