Stability of hierarchical triples - I. Dependence on inner eccentricity and inclination

dc.contributor.authorA Mylläri
dc.contributor.authorM Valtonen
dc.contributor.authorA Pasechnik
dc.contributor.authorS Mikkola
dc.contributor.organizationfi=Suomen ESO-keskus|en=Finnish Centre for Astronomy with ESO|
dc.contributor.organizationfi=Tuorlan observatorio|en=Tuorla Observatory|
dc.contributor.organizationfi=fysiikan ja tähtitieteen laitos|en=Department of Physics and Astronomy|
dc.contributor.organization-code1.2.246.10.2458963.20.90670098848
dc.contributor.organization-code2606700
dc.converis.publication-id30821000
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/30821000
dc.date.accessioned2022-10-28T13:14:14Z
dc.date.available2022-10-28T13:14:14Z
dc.description.abstractIn simulations it is often important to decide if a given hierarchical triple star system is stable over an extended period of time. We introduce a stability criterion, modified from earlier work, where we use the closest approach ratio Q of the third star to the inner binary centre of mass in their initial osculating orbits. We study by numerical integration the orbits of over 1000 000 triple systems of the fixed masses and outer eccentricities eout, but varying inner eccentricities ein and inclinations i. 12 primary combinations of masses have been tried, representing the range encountered in stellar systems. The definition of the instability is either the escape of one of the bodies, or the exchange of the members between the inner and outer systems. An analytical approximation is derived using the energy change in a single close encounter between the inner and outer systems, assuming that the orbital phases in subsequent encounters occur randomly. The theory provides a fairly good description of the typical Q(st), the smallest Q value that allows the system to be stable over N = 10 000 revolutions of the initial outer orbit. The final stability limit formula is Q(st) = 10(1/3)A[(f g)(2)/(1 - e(out))](1/6), where the coefficient A similar to 1 should be used in N-body experiments, and A = 2.4 when the absolute long-term stability is required. The functions f (e(in), cos i) and g(m(1), m(2), m(3)) are derived in the paper. At the limit of e(in) = i = m(3) = 0, f g = 1.
dc.format.pagerange830
dc.format.pagerange841
dc.identifier.eissn1365-2966
dc.identifier.jour-issn0035-8711
dc.identifier.olddbid180703
dc.identifier.oldhandle10024/163797
dc.identifier.urihttps://www.utupub.fi/handle/11111/33559
dc.identifier.urnURN:NBN:fi-fe2021042719033
dc.language.isoen
dc.okm.affiliatedauthorValtonen, Mauri
dc.okm.affiliatedauthorPasechnik, Alexey
dc.okm.affiliatedauthorMikkola, Seppo
dc.okm.affiliatedauthorDataimport, Suomen ESO-keskus
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherOXFORD UNIV PRESS
dc.publisher.countryUnited Kingdomen_GB
dc.publisher.countryBritanniafi_FI
dc.publisher.country-codeGB
dc.relation.doi10.1093/mnras/sty237
dc.relation.ispartofjournalMonthly Notices of the Royal Astronomical Society
dc.relation.issue1
dc.relation.volume476
dc.source.identifierhttps://www.utupub.fi/handle/10024/163797
dc.titleStability of hierarchical triples - I. Dependence on inner eccentricity and inclination
dc.year.issued2018

Tiedostot

Näytetään 1 - 1 / 1
Ladataan...
Name:
sty237.pdf
Size:
4.5 MB
Format:
Adobe Portable Document Format
Description:
Publisher's version