Observations of binary systems allow us to determine the internal structure constant, k2, which is related to the variation of density within the star and is an important parameter of stellar evolution models. It is best studied in binary systems with eccentric orbits that show apsidal motion. The period of rotation of the periastron in eccentric eclipsing binaries does not allow us to derive the individual internal stellar constant of the component stars.
System | Spectral | e | P | U | e3 | P3 | Source |
type | [days] | [years] | [years] | ||||
HS Her | B4+A4 | 0.021 | 1.637 | 72.4 | 0.7 | 74.1 | Wolf (2001) |
U Oph | B5+B5 | 0.003 | 1.677 | 21.2 | 0.22 | 38.7 | Kämper (1986) |
DR Vul | B0+B0.5 | 0.095 | 2.251 | 36.3 | 0.73 | 62.8 | Wolf et al. (1999) |
YY Sgr | B6+B5 | 0.159 | 2.628 | 290.4 | 0.44 | 44.3 | Wolf (2000) |
RU Mon | B7+B7 | 0.396 | 3.585 | 347 | 0.46 | 73.3 | Wolf et al. (1999) |
TV Cet | F2+F5 | 0.055 | 9.103 | 30000 | 0.25 | 28.5 | this paper |
The observational average value of
is given by the relation
![]() |
(3) |
Taking into account the value of the eccentricity and the masses
of the components, one has to subtract from
a relativistic correction
(Levi-Civita 1937;
Giménez 1985)
![]() |
(4) |
![]() |
(5) |
The values of
and resulting mean internal
structure constants
are given in Table 3.
Theoretical values
according to available theoretical models
for the internal stellar structure along the main sequence, computed by
Claret & Giménez (1992) for a variety of masses and chemical compositions,
are also given.
Copyright ESO 2001