G. Barnes et al., Angular momentum transport in magnetized stellar radiative zones. III. Thesolar light-element abundances, ASTROPHYS J, 511(1), 1999, pp. 466-480
We calculate the depletion of the trace elements lithium and beryllium with
in a solar-mass star during the course of its evolution from the zero-age m
ain sequence to the age of the present-day Sun. In the radiative layers ben
eath the convection zone, we assume that these elements are transported by
the turbulent fluid motions that result from instability of the shear how a
ssociated with internal differential rotation. This turbulent mixing is mod
eled as a diffusion process, using a diffusion coefficient that is taken to
be proportional to the gradient of the angular velocity distribution insid
e the star. We study the evolution of the light-element abundances produced
by rotational mixing for models in which internal angular momentum redistr
ibution takes place either by hydrodynamic or by hydromagnetic means. Since
models based on these alternative mechanisms for angular-momentum transpor
t predict similar surface rotation rates late in the evolution, we explore
the extent to which light-element abundances make it possible to distinguis
h between them. In the case of an internally magnetized star, our computati
ons indicate that both the details of the surface abundance evolution and t
he magnitude of the depletion at solar age can depend sensitively on the as
sumed strength and configuration of the poloidal magnetic field inside the
star. For a configuration with no direct magnetic coupling between the radi
ative and convective portions of the stellar interior, the depletion of lit
hium calibrated to the solar lithium depletion at the solar age is similar
at all ages to the lithium depletion of a model in which angular-momentum t
ransport occurs solely by hydrodynamical processes. However, the two models
can be distinguished on the basis of their respective beryllium depletions
, with the depletion of the magnetic model being significantly smaller than
that of the nonmagnetic model.