Table 1
Kinematic data for Mira.
b(°) | −58 | ϖ (mas) | 10.9 ± 1.2a |
μα, LSR (mas yr-1) | −20.93a | μδ, LSR (mas yr-1) | −222.39a |
RVLSR (km s-1) | 47.2f | Vspace, LSR (km s-1) | 107.9 |
Vspace, LSR PA (°) | 185.4 | Vspace, LSRi (°) | 25.9 |
Vwind (km s-1) | 4c | Voutflow (km s-1) | 160 ± 10d |
Bipolar flow PA (°) | 168−180d | Bipolar flow i (°) | –69d |
Orbital pole PA (°) | 228e | Orbital pole i (°) | ± 22e |
P (yr) | ≈ 500e | a (AU) | ≈ 100ae |
M1 + M2 (M⊙) | 4.4e | Ṁ (M⊙ yr-1) | 10-7b |
Notes. Negative inclinations are towards the observer. The various vectors are displayed in a 3D view in Fig. 4. The adopted solar motion to convert heliocentric velocities in LSR velocities is (U,V,W)⊙ = (11.10,12.24,7.25) km s-1 (Schönrich et al. 2010). The matrix to convert equatorial velocities into galactic velocities is taken from Johnson & Soderblom (1987).
References.
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