 A near-infrared (y band)light curve for DN Orionis. The main plot shows the variation over a full orbital period, and the inset plot shows the time near maximum eclipse. Adapted from Etzel and Olson (1995)[1] | |
| Observation data Epoch J2000 Equinox J2000 | |
|---|---|
| Constellation | Orion |
| Right ascension | 06h 00m 28.34516s[2] |
| Declination | 10° 13′ 04.9963″[2] |
| Apparent magnitude (V) | 9.18[3] |
| Characteristics | |
| Spectral type | A0 + G5III[4] |
| B−Vcolor index | 0.240±0.026[3] |
| Astrometry | |
| Proper motion (μ) | RA: −1.771mas/yr[2] Dec.: −7.243mas/yr[2] |
| Parallax (π) | 1.9058±0.0452 mas[2] |
| Distance | 1,710 ± 40 ly (520 ± 10 pc) |
| Absolute magnitude (MV) | 0.19 + 0.86[1] |
| Orbit[5] | |
| Period (P) | 12.9663 d |
| Eccentricity (e) | 0.00 |
| Periastronepoch (T) | 2,428,494.55±10.0 JD |
| Semi-amplitude (K1) (primary) | 8.2 km/s |
| Semi-amplitude (K2) (secondary) | 120.4 km/s |
| Details | |
| Primary | |
| Mass | 2.80±0.05[1] M☉ |
| Radius | 2.36±0.07[1] R☉ |
| Luminosity | 50[1] L☉ |
| Surface gravity (log g) | 4.14 cgs |
| Secondary | |
| Mass | 0.34±0.10[1] M☉ |
| Radius | 6.66±0.15[1] R☉ |
| Luminosity | 25[1] L☉ |
| Surface gravity (log g) | 2.31 cgs |
| Other designations | |
| DN Ori,BD+10° 967,HD 40632,HIP 28456,SAO 95108[6] | |
| Database references | |
| SIMBAD | data |
DN Orionis is anAlgol variable[7] located in the constellation ofOrion. The primary star is a spectral type A0 star and the secondary is an evolvedgiant star of type G5III.[4] The pair form a classical Algol-type system in which each star eclipses the other once per orbit, dropping the visual magnitude from 9.14 down to 9.62 at primary minimum and 9.25 at secondary minimum.[7] Theirorbital period is close to 13 days long.[5]
This is a slightlydetached system in which the secondary is almost in contact with itsRoche limit, while the primary has anaccretion disk that is creatingemission lines in itsspectrum.[4] The pair have an unusually low mass ratio and the secondary appears to be of very low mass and overluminous.[5] Mass is flowing from the extended atmosphere of the cooler secondary to the hotter primary.[1] An evolutionary history of this system suggests that the current secondary was once the primary component, but has since transferred most of its mass to the partner star as itevolved off themain sequence.[4]
