1968
DOI: 10.1086/110614
|View full text |Cite
|
Sign up to set email alerts
|

Dynamical evolution of triple stars.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

5
170
0
2

Year Published

2003
2003
2018
2018

Publication Types

Select...
5
4

Relationship

0
9

Authors

Journals

citations
Cited by 228 publications
(177 citation statements)
references
References 0 publications
5
170
0
2
Order By: Relevance
“…Harrington 1968Harrington , 1969Soderhjelm 1975;Breiter & Vokrouhlický 2015). Here n 1 and n 2 are the mean motion values of the orbits 1 and 2, both related to the semi-major axes a 1 and a 2 through the third Kepler law: n 2 1 a 3 1 = GM 1 and n 2 2 a 3 2 = GM 2 (G is the gravitational constant).…”
Section: Secular Effectsmentioning
confidence: 99%
“…Harrington 1968Harrington , 1969Soderhjelm 1975;Breiter & Vokrouhlický 2015). Here n 1 and n 2 are the mean motion values of the orbits 1 and 2, both related to the semi-major axes a 1 and a 2 through the third Kepler law: n 2 1 a 3 1 = GM 1 and n 2 2 a 3 2 = GM 2 (G is the gravitational constant).…”
Section: Secular Effectsmentioning
confidence: 99%
“…By the use of the theory of Harrington (1968Harrington ( , 1969, based on the von Zeipel averaging method of the canonical equations, Söderhjelm (1975Söderhjelm ( , 1982 derived analytical formulae for the long period perturbations in the standard Delaunay variables. Although these formulae are exact up to second order in the (a/a ) ratio, their practical use is limited, at least in their original forms.…”
Section: An Analytical Formula Of the Long Period Perturbation Of An mentioning
confidence: 99%
“…There the first two of our groups called together as "short period" perturbations, while the "apse-node terms" are called as "long period" ones. In the stellar three-body problem this latter classification was used by Harrington 1968Harrington , 1969.) These effects can be most easily detected in those triple systems, where the close binary happens to be an eclipsing one.…”
Section: Introductionmentioning
confidence: 99%
“…The Kozai resonance (recently and frequently referred to as Kozai cycle[s]) was first described by Kozai (1962) when investigating secular perturbations of asteroids. The first (theoretical) investigation of this phenomenon with respect to multiple stellar systems can be found in the studies by Harrington (1968Harrington ( , 1969, Mazeh & Saham (1979), and Söderhjelm (1982). A higher, third-order theory of Kozai cycles was given by Ford et al (2000), while the first application of KCTF to explain the present configuration of a close, hierarchical triple system (the emblematic Algol, itself) was presented by Kiseleva et al (1998).…”
Section: Introductionmentioning
confidence: 99%