2025MNRAS.540..973C


Query : 2025MNRAS.540..973C

2025MNRAS.540..973C - Mon. Not. R. Astron. Soc., 540, 973-983 (2025/June-2)

Wind internal shocks in a binary system.

CASTELLANOS-RAMIREZ A., CANTO J., LIZANO S., RAGA A.C., GONZALEZ R.F. and ZAPATA L.A.

Abstract (from CDS):

The wind ejection velocity of a star in orbital motion in a binary system undergoes a variation along its orbit with respect to the centre of mass. Due to this time-dependent ejection velocity, the wind collides with itself, generating two-shock wave structures called working surfaces, which propagate outwards in the flow. In this work, we present both an analytic model and one-dimensional numerical simulations to describe the formation and dynamical evolution of the working surfaces, assuming an elliptic orbit for the star. In addition, the luminosity emitted by these structures, as they move away from the source, is computed. Our semi-analytic model of internal shock dynamics and numerical simulations show that two working surfaces are formed for directions near the periastron (in the range of ${\pm} 60^{\circ }$), which propagate with different velocities, where the faster one is produced later. These two working surfaces collide with each other, producing a single working surface. We found a good agreement between our analytic model and our numerical simulations.

Abstract Copyright: © 2025 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): shock waves - binaries: general - stars: winds, outflows

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* R Scl C* 01 26 58.0939182720 -32 32 35.439234828 17.26 9.59 5.72 3.69 2.30 C-N5+ 354 0
2 HH 34 HH 05 35 31.30 -06 28 43.0     16     ~ 493 2
3 HH 1 HH 05 36 20.8 -06 45 13           ~ 415 1
4 V* GX Mon OH* 06 52 47.0423680104 +08 25 19.097958468   15.40 15.46 10.56   M9 126 0
5 RAFGL 3068 C* 23 19 12.60744 +17 11 33.1332           C 288 1
6 NAME HH 270-110 HH ~ ~           ~ 8 0

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