2020ApJ...896..123S


Query : 2020ApJ...896..123S

2020ApJ...896..123S - Astrophys. J., 896, 123-123 (2020/June-3)

Alfven-wave-driven magnetic rotator winds from low-mass stars. I. Rotation dependences of magnetic braking and mass-loss rate.

SHODA M., SUZUKI T.K., MATT S.P., CRANMER S.R., VIDOTTO A.A., STRUGAREK A., SEE V., REVILLE V., FINLEY A.J. and BRUN A.S.

Abstract (from CDS):

Observations of stellar rotation show that low-mass stars lose angular momentum during the main sequence. We simulate the winds of sunlike stars with a range of rotation rates, covering the fast and slow magneto-rotator regimes, including the transition between the two. We generalize an Alfven-wave-driven solar wind model that builds on previous works by including the magneto-centrifugal force explicitly. In this model, the surface-averaged open magnetic flux is assumed to scale as B*f*open∝Ro–1.2, where f*open and Ro are the surface open-flux filling factor and Rossby number, respectively. We find that, (1) the angular-momentum loss rate (torque) of the wind is described as τw~2.59×1030 erg (Ω*/Ω☉)2.82, yielding a spin-down law Ω*∝t–0.55. (2) The mass-loss rate saturates at {dot}Mw∼3.4×10–14M☉ yr–1, due to the strong reflection and dissipation of Alfven waves in the chromosphere. This indicates that the chromosphere has a strong impact in connecting the stellar surface and stellar wind. Meanwhile, the wind ram pressure scales as Pw∝Ω*0.57, which is able to explain the lower envelope of the observed stellar winds by Wood et al. (3) The location of the Alfven radius is shown to scale in a way that is consistent with one-dimensional analytic theory. Additionally, the precise scaling of the Alfven radius matches previous works, which used thermally driven winds. Our results suggest that the Alfven-wave-driven magnetic rotator wind plays a dominant role in the stellar spin-down during the main sequence.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Stellar evolution - Stellar rotation - Stellar winds - Solar wind - Solar evolution - Stellar mass loss - Magnetohydrodynamical simulations

Simbad objects: 11

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Number of rows : 11
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 * eps Eri BY* 03 32 55.8444911587 -09 27 29.739493865 5.19 4.61 3.73 3.00 2.54 K2V 2073 1
2 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
3 * 61 Vir PM* 13 18 24.3139864471 -18 18 40.297748582 5.710 5.440 4.740     G6.5V 742 1
4 NAME Proxima Centauri PM* 14 29 42.9461331854 -62 40 46.164680672 14.21 12.95 11.13 9.45 7.41 M5.5Ve 1483 0
5 * alf Cen ** 14 39 36.50 -60 50 02.3   0.4 -0.1     G2V+K1V 1031 0
6 * ksi Boo BY* 14 51 23.37993 +19 06 01.6994 5.618 5.370 4.593 3.91 3.48 G7Ve+K5Ve 503 0
7 * 36 Oph ** 17 15 20.9839376 -26 36 10.157115           K2V+K1V 145 0
8 * 70 Oph SB* 18 05 27.28518 +02 30 00.3558 5.40 4.89 4.03 3.38 2.92 K0-V 679 0
9 * 61 Cyg A BY* 21 06 53.9395895022 +38 44 57.902349973 7.50 6.39 5.21 4.19 3.54 K5V 1099 0
10 * eps Ind PM* 22 03 21.6536261624 -56 47 09.522795714   5.75 4.69     K5V 616 0
11 V* EV Lac PM* 22 46 49.7312610268 +44 20 02.374381562   11.85 10.26 9.89   M4.0Ve 993 2

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