Structure of a Protobinary System: An Asymmetric Circumbinary Disk and Spiral Arms

被引:23
|
作者
Matsumoto, Tomoaki [1 ,2 ,3 ]
Saigo, Kazuya [4 ]
Takakuwa, Shigehisa [5 ,6 ]
机构
[1] Hosei Univ, Fac Sustainabil Studies, Chiyoda Ku, Tokyo 1028160, Japan
[2] Princeton Univ, Dept Astrophys Sci, 4 Ivy Lane, Princeton, NJ 08544 USA
[3] RIKEN Ctr Computat Sci R CCS, Chuo Ku, 7-1-26 Minatojima Minami Machi, Kobe, Hyogo 6500047, Japan
[4] Natl Astron Observ Japan, Chile Observ, Osawa 2-21-1, Mitaka, Tokyo 1818588, Japan
[5] Kagoshima Univ, Grad Sch Sci & Engn, Dept Phys & Astron, 1-21-35 Korimoto, Kagoshima 8900065, Japan
[6] Acad Sinica, Inst Astron & Astrophys, 1,Sect 4,Roosevelt Rd, Taipei 10617, Taiwan
来源
ASTROPHYSICAL JOURNAL | 2019年 / 871卷 / 01期
基金
日本学术振兴会;
关键词
binaries: general; hydrodynamics; protoplanetary disks; stars: formation; stars: protostars; ROSSBY-WAVE INSTABILITY; PLANET FORMATION; ACCRETION RATES; EVOLUTION; MASS; CIRCUMSTELLAR; YOUNG; FRAGMENTATION; SIMULATIONS; BINARIES;
D O I
10.3847/1538-4357/aaf6ab
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We investigate the gas structures around young binary stars using three-dimensional numerical simulations. Each model exhibits circumstellar disks, spiral arms, and a circumbinary disk with an inner gap or cavity. The circumbinary disk has an asymmetric pattern rotating at an angular velocity of approximately one-fourth of the binary orbit of the moderate-temperature models. Because of this asymmetry, the circumbinary disk has a density bump and a vortex, both of which continue to exist until the end of our calculation. The density bump and vortex are attributed to enhanced angular momentum, which is promoted by the gravitational torque of the stars. In a hot model (c >= 2.0), the asymmetry rotates considerably more slowly than in the moderate-temperature models. The cold models (c <= 0.02) exhibit eccentric circumbinary disks, the precession of which is approximated by a secular motion of the ballistic particles. The asymmetry in the circumbinary disk does not depend on the mass ratio, but it becomes less clear as the specific angular momentum of the infalling envelope increases. The relative accretion rate onto the stars is sensitive to the angular momentum of the infalling envelope. For envelopes with constant angular momentum, the secondary tends to have a higher accretion rate than the primary, except in very low angular momentum cases. For envelopes with a constant angular velocity, the primary has a higher accretion rate than the secondary because gas with low specific angular momentum falls along the polar directions.
引用
收藏
页数:17
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