TY - JOUR
T1 - Wind collision and accretion simulations of the massive binary system HD 166734
AU - Kashi, Amit
N1 - Publisher Copyright:
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PY - 2020
Y1 - 2020
N2 - I have run hydrodynamic simulations that follow the colliding wind structure of the massive binary system HD 166734 along its binary orbit. I show that close to periastron passage the secondary wind is suppressed and the secondary accretes mass from the primary wind. The system consists of two blue supergiants with masses of M1 ≈ 39.5 M⊙ and M2 ≈ 30.5 M⊙, on an orbit of P 34.538 d with an eccentricity of e ≈ 0.618. This close O-O binary with high eccentricity is observed through its orbit in X-rays, where it shows an unusually long minimum close to periastron passage. I use advanced simulations with wind acceleration and a prescription treatment of accretion and I simulate the entire orbit at high resolution, which captures the instabilities in the winds. I find that the colliding wind structure is unstable even at apastron. As the stars approach periastron passage, the secondary wind is quenched by the primary wind and the accretion on to the secondary begins. The accretion phase lasts for 12 d, and the amount of accreted mass obtained per cycle is Macc 1.3 × 10-8M⊙. The accretion phase can account for the observed decline in X-ray emission from the system.
AB - I have run hydrodynamic simulations that follow the colliding wind structure of the massive binary system HD 166734 along its binary orbit. I show that close to periastron passage the secondary wind is suppressed and the secondary accretes mass from the primary wind. The system consists of two blue supergiants with masses of M1 ≈ 39.5 M⊙ and M2 ≈ 30.5 M⊙, on an orbit of P 34.538 d with an eccentricity of e ≈ 0.618. This close O-O binary with high eccentricity is observed through its orbit in X-rays, where it shows an unusually long minimum close to periastron passage. I use advanced simulations with wind acceleration and a prescription treatment of accretion and I simulate the entire orbit at high resolution, which captures the instabilities in the winds. I find that the colliding wind structure is unstable even at apastron. As the stars approach periastron passage, the secondary wind is quenched by the primary wind and the accretion on to the secondary begins. The accretion phase lasts for 12 d, and the amount of accreted mass obtained per cycle is Macc 1.3 × 10-8M⊙. The accretion phase can account for the observed decline in X-ray emission from the system.
KW - Accretion, accretion discs
KW - Binaries: General
KW - Stars: Individual: HD 166734
KW - Stars: winds, outflows
UR - http://www.scopus.com/inward/record.url?scp=85101390537&partnerID=8YFLogxK
U2 - 10.1093/MNRAS/STAA203
DO - 10.1093/MNRAS/STAA203
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AN - SCOPUS:85101390537
SN - 0035-8711
VL - 492
SP - 5261-5270Y
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -