Observation data Epoch J2000.0 Equinox J2000.0 | |
---|---|
Constellation | Aries[1] |
Right ascension | 03h 09m 28.5434s[2] |
Declination | +30° 40′ 24.863″[2] |
Apparent magnitude (V) | 11.57 ± 0.15[3] |
Characteristics | |
Spectral type | K3V[4] |
Apparent magnitude (B) | 12.58 ± 0.30[3] |
Apparent magnitude (V) | 11.57 ± 0.15[3] |
Apparent magnitude (J) | 10.015 ± 0.020[5] |
Apparent magnitude (H) | 9.560 ± 0.019[5] |
Apparent magnitude (K) | 9.421 ± 0.017[5] |
Variable type | planetary transit[6] |
Astrometry | |
Radial velocity (Rv) | 5.21±0.28[2] km/s |
Proper motion (μ) | RA: 3.334(68) mas/yr[2] Dec.: −44.433(53) mas/yr[2] |
Parallax (π) | 7.6997±0.0579 mas[2] |
Distance | 424 ± 3 ly (129.9 ± 1.0 pc) |
Details[7] | |
WASP-11 A | |
Mass | 0.77±0.02[8] M☉ |
Radius | 0.74±0.01[8] R☉ |
Luminosity | 0.28±0.002[8] L☉ |
Surface gravity (log g) | 4.58±0.02[8] cgs |
Temperature | 4,884±16[8] K |
Metallicity [Fe/H] | 0.25±0.07[9] dex |
Rotational velocity (v sin i) | 1.9±0.9[9] km/s |
Age | 8.7±3.5[8] Gyr |
WASP-11 B | |
Mass | 0.34 M☉ |
Temperature | 3,494±37[10] K |
Other designations | |
HAT-P-10, TOI-4516, TIC 85593751, WASP-11, TYC 2340-1714-1, GSC 02340-01714, 2MASS J03092855+3040249[3] | |
Database references | |
SIMBAD | data |
Exoplanet Archive | data |
WASP-11, also designated HAT-P-10, is a binary star system. The primary star is a main-sequence orange dwarf star. The secondary is an M dwarf with a projected separation of 42 AU.[10] The system is located about 424 light-years away[2] in the constellation Aries.
A hot Jupiter with half Jupiter's mass, WASP-11b (or HAT-P-10b), was detected around the primary star independently by the Hungarian Automated Telescope Network and the Wide Angle Search for Planets teams, both of which used the transit method.[4][6]
Companion (in order from star) |
Mass | Semimajor axis (AU) |
Orbital period (days) |
Eccentricity | Inclination | Radius |
---|---|---|---|---|---|---|
b | 0.532+0.020 −0.021 MJ |
0.04376+0.00071 −0.00067 |
3.7224793±0.0000007 | <0.03 | 89.03±0.34° | 0.990±0.022 RJ |