Astron. Astrophys. 363, 555-567 (2000)
Appendix: the angular momentum conservation model of wind accretion for barium stars: equations
For the binary system, the two components (an intrinsic AGB star
with mass , the present white dwarf,
and a main sequence star with mass ,
the present barium star) rotating around the mass core C, so the total
angular momentum is conservative in the mass core reference frame. If
the two components exchange material through wind accretion, the
angular momentum conservation of total system is showed by:
![[EQUATION]](img81.gif)
where µ is reduced mass, and r is the distance
from to
.
and are the distances from
,
to the mass core C respectively.
(=2 ) is angular velocity, where
is the orbital period (Huang 1956).
v is an additional effective velocity defined through the
angular momentum variation in the direction of orbital motion of
component 2. The first term on the right side of the equal-sign is the
angular momentum lost by the escaping material and the second term is
the additional angular momentum lost by the escaping material.
For the binary system, according to Huang (1956), the changes of
orbital elements, the orbital semi-major axis A and
eccentricity e, are
![[EQUATION]](img84.gif)
![[EQUATION]](img85.gif)
where
![[EQUATION]](img86.gif)
According to the angular momentum conservation model, the
term can be obtained from the
following equation:
![[EQUATION]](img88.gif)
thus
![[EQUATION]](img89.gif)
then, we can obtain
![[EQUATION]](img90.gif)
Thus
![[EQUATION]](img91.gif)
The term is:
![[EQUATION]](img93.gif)
Combining Eqs. (9), (10), (15) and (16), we can obtain the
changes of orbital semi-major axis A and eccentricity
e:
![[EQUATION]](img94.gif)
![[EQUATION]](img95.gif)
© European Southern Observatory (ESO) 2000
Online publication: December 11, 2000
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