The input physics is identical to that of Meynet et al. (1994, paper
V). This includes in particular the adoption of ``high'' mass loss
rates, i.e.
M_ M
/yr for WNL stars and twice
the mass loss rates of de Jager et al. (1988) for stars with
_. Otherwise we follow the prescription of paper
I. For consistence with the earlier grids the initial composition is
calculated as in paper I: X=0.7584, Y=0.2412, Z=0.0004.
The HRD with the calculated tracks is shown in Fig. A1 Hatched areas indicate regions of slow nuclear
burning phases. The H, He, and C burning lifetimes are given in Table
. Due to numerical instabilities the 85 M_ M
model
could not be fully evolved to the end of He burning. The remaining
He-burning lifetime as well as the duration of C-burning were
estimated by interpolation between the two adjacent tracks.
For similar reasons of the 20 M_ M
model had also
to be estimated.
The mass limit for the formation of WR stars, , at
Z=0.0004 from the present tracks is
85 M_ M
, as
already derived in de Mello et al. (1998). Other properties of the
Z=0.0004 models can readily be derived from the detailed data included
in the present database.