T Coronae Borealis
Recurrent nova in the constellation Corona Borealis
From Wikipedia, the free encyclopedia
T Coronae Borealis is a binary star and a recurrent nova about 3,000 light-years (920 parsecs) away in the constellation Corona Borealis.[12] T Coronae Borealis is its variable-star designation and the name most frequently used in the astronomical literature, but it also has the official proper name Blaze Star. The system was first observed in outburst in 1866 by John Birmingham,[13] but had been observed earlier in quiescence as a 10th magnitude star.[14] It may have been observed in 1217 and in 1787 as well.[15][16] In February 1946, the flare-up was discovered independently by three observers: the Soviet amateur astronomer A. S. Kamenchuk, the 15-year-old schoolboy Michael Woodman from Wales, and the British variable star observer N. F. H. Knight.[17] This led to the theory that the star flares every 80 years[18] with the next nova expected to occur before 2027.
| Observation data Epoch J2000 Equinox J2000 | |
|---|---|
| Constellation | Corona Borealis |
| Right ascension | 15h 59m 30.1622s[1] |
| Declination | +25° 55′ 12.613″[1] |
| Apparent magnitude (V) | 2.0–10.8[2] |
| Characteristics | |
| Evolutionary stage | Red giant + white dwarf[3] |
| Spectral type | M3III+p[4] |
| Variable type | recurrent nova[2] |
| Astrometry | |
| Radial velocity (Rv) | −27.75±0.04[5] km/s |
| Proper motion (μ) | RA: −4.461 mas/yr[1] Dec.: 12.016 mas/yr[1] |
| Parallax (π) | 1.0920±0.0275 mas[1] |
| Distance | 2,990 ± 80 ly (920 ± 20 pc) |
| Absolute magnitude (MV) | +0.16 (min.)[6] |
| Orbit[5] | |
| Period (P) | 227.5528±0.0002 days |
| Semi-major axis (a) | 0.960 AU |
| Eccentricity (e) | 0.009±0.003[7] |
| Inclination (i) | 61.5° |
| Periastron epoch (T) | 2459978.37±0.08 |
| Semi-amplitude (K1) (primary) | 23.90±0.05 km/s |
| Details | |
| Red giant | |
| Mass | 0.93[5] M☉ |
| Radius | 63.5±0.3[8] – 71.1[5] R☉ |
| Luminosity | 583±4[8] L☉ |
| Surface gravity (log g) | 0.672+0.009 −0.007[8] cgs |
| Temperature | 3,561±3[8] K |
| Metallicity [Fe/H] | +0.20+0.05 −0.03[8] dex |
| Rotational velocity (v sin i) | 4.75±0.26[5] km/s |
| White dwarf | |
| Mass | 1.35[5] M☉ |
| Radius | 0.0045[9] R☉ |
| Luminosity | ~100[10] L☉ |
| Other designations | |
| Blaze Star, T CrB, AAVSO 1555+26, BD+26°2765, HD 143454, HIP 78322, HR 5958, SAO 84129, 2MASS J15593015+2555126[11] | |
| Database references | |
| SIMBAD | data |
Nomenclature
T Coronae Borealis (abbreviated T CrB or unofficially T Cor Bor)[19] is the star's variable star designation and is its most commonly used name. It also has the Bright Star Catalogue designation HR 5958 and the Henry Draper Catalogue designation HD 143454.[11]
The proper name Blaze Star[20] has been used since its outburst in 1866, and was officially approved by the IAU Working Group on Star Names on 22 September 2025.[21]
Description

T CrB normally has a magnitude of about 10, which is near the limit of typical binoculars. Two well-documented outbursts have been observed, reaching magnitude 2.0 on May 12, 1866 and magnitude 3.0 on February 9, 1946,[22] though a more recent paper shows the 1866 outburst with a possible peak range of magnitude 2.5±0.5.[23] When at peak magnitude of 2.5, this recurrent nova is dimmer than about 100 brightest stars in the night sky,[24] but easily visible to the naked eye.

T CrB is a binary system containing a large cool component and a smaller hot component. The cool component is a red giant that transfers material to the hot component.[3] The hot component, which initially was the most massive and brightest of the two stars, is now a white dwarf surrounded by an accretion disc, all hidden inside a dense cloud of material from the red giant. When the system is quiescent, the red giant dominates the visible light output and the system appears as an M3 giant. The hot component contributes some emission and dominates the ultraviolet output. During outbursts, the transfer of material to the hot component increases greatly, the hot component expands, and the overall luminosity of the system increases by orders of magnitude.[10][25][26][27]

The two components of the system orbit each other every 227.5528 d. The orbit is almost circular and is inclined at an angle of 61.5°. The separation between the components is 0.960 AU.[5]
2016–present activity
On April 20, 2016, Sky & Telescope reported a sustained brightening since February 2015 from magnitude 10.5 to about 9.2. A similar event was reported in 1938, 8 years before the 1946 outburst.[28] By June 2018, the star had dimmed slightly but still remained at an unusually high level of activity. By mid-2023, it had faded by 0.35 magnitude or about 28%;[a] its lowest brightness seen since 2016.[29] A similar dimming occurred in the year before the 1946 outburst,[30] leading some to predict an eruption before September 2024.[31] It has repeatedly been predicted to be imminent, but several predictions have lapsed as of May 2026 and no such nova has yet been observed.[30]
Outburst predictions
Predictions of the next nova (in order of when the prediction was made):
- 2026–2027 (made in 1946 either by N. F. H. Knight or W. M. Lindley)[32]
- Mid‐February 2024 to end‐September 2026 (made in March 2023)[33]
- Beginning January 2024 to mid-August 2024 (made in June 2023)[34] (lapsed)
- January 2024 (made in August 2023)[35] (lapsed)
- End of October 2024 (made in June 2024)[36] (lapsed)
- Around March 27, 2025 (lapsed); November 10, 2025 (lapsed); June 25, 2026; or February 8, 2027 (made in October 2024)[37]
Notes
- 1-100-0.35/5 = 0.2756