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Alioth
View on Wikipedia| Observation data Epoch J2000 Equinox J2000 | |
|---|---|
| Constellation | Ursa Major |
| Right ascension | 12h 54m 01.74959s[1] |
| Declination | +55° 57′ 35.3627″[1] |
| Apparent magnitude (V) | 1.77[2] |
| Characteristics | |
| Spectral type | A1III-IVp kB9 |
| U−B color index | +0.02[2] |
| B−V color index | −0.02[2] |
| Variable type | α2 CVn |
| Astrometry | |
| Radial velocity (Rv) | −9.3[3] km/s |
| Proper motion (μ) | RA: +111.91 mas/yr[1] Dec.: −8.24 mas/yr[1] |
| Parallax (π) | 39.51±0.20 mas[1] |
| Distance | 82.6 ± 0.4 ly (25.3 ± 0.1 pc) |
| Absolute magnitude (MV) | −0.2[4] |
| Details | |
| Mass | 2.91[5] M☉ |
| Radius | 4.29+0.19 −0.21[6] R☉ |
| Luminosity | 104.4±9.3[6] L☉ |
| Surface gravity (log g) | 3.59[6] cgs |
| Temperature | 8,908±24[6] K |
| Metallicity [Fe/H] | +0.00[4] dex |
| Rotation | 5.088631(18)[7] days |
| Rotational velocity (v sin i) | 33[8] km/s |
| Age | 300[9] Myr |
| Other designations | |
| Alioth, Allioth, Aliath, ε UMa, 77 Ursae Majoris, BD+56°1627, FK5 483, GC 17518, HD 112185, HIP 62956, HR 4905, SAO 28553, PPM 33769 | |
| Database references | |
| SIMBAD | data |
Alioth /ˈæliɒθ/ ⓘ, also called Epsilon Ursae Majoris, is a star in the northern constellation of Ursa Major. The designation is Latinised from ε Ursae Majoris and abbreviated Epsilon UMa or ε UMa.[10][11] Despite being designated "ε" (epsilon), it is the brightest star in the constellation and at magnitude 1.77 is the thirty-third brightest star in the sky.
It is the star in the tail of the bear closest to its body, and thus the star in the handle of the Big Dipper (or Plough) closest to the bowl. It is also a member of the large and diffuse Ursa Major moving group. Historically, the star was frequently used in celestial navigation in the maritime trade, because it is listed as one of the 57 navigational stars.[1]
Physical characteristics
[edit]

According to Hipparcos, Epsilon Ursae Majoris is 81 light-years (25 parsecs) from the Sun. Its spectral type is A1p; the "p" stands for peculiar, as its spectrum is characteristic of an α2 Canum Venaticorum variable. Epsilon Ursae Majoris, as a representative of this type, may harbor two interacting processes: first, the star's strong magnetic field separating different elements in its hydrogen 'fuel'; second, a rotation axis at an angle to the magnetic axis may be spinning different bands of magnetically sorted elements into the line of sight between Epsilon Ursae Majoris and the Earth. The intervening elements react differently at different frequencies of light as they whip in and out of view, causing Epsilon Ursae Majoris to have very strange spectral lines that fluctuate over a period of 5.1 days. The kB9 suffix to the spectral type indicates that the calcium K line is present and representative of a B9 spectral type even though the rest of the spectrum indicates A1.
Epsilon Ursae Majoris's rotational and magnetic poles are at almost 90 degrees to one another. Darker (denser) regions of chromium form a band at right angles to the equator.
It has long been suspected that Epsilon Ursae Majoris is a spectroscopic binary, possibly with more than one companion.[13] A 2008 study suggested Alioth's 5.1-day variation may be due to a substellar object of about 14.7 Jupiter masses in an eccentric orbit (e=0.5) with an average separation of 0.055 astronomical units.[14] It is now thought that the 5.1-day period is the rotation period of the star,[7] and no companions have been detected using the most modern equipment.[15] Observations of Alioth with the Navy Precision Optical Interferometer also did not detected a companion.[6]
Epsilon Ursae Majoris has a relatively weak magnetic field for a variable of this type, 15 times weaker than α Canum Venaticorum, but it is still 100 times stronger than that of the Earth.[16]
Name and etymology
[edit]ε Ursae Majoris (Latinised to Epsilon Ursae Majoris) is the star's Bayer designation.
The traditional name Alioth comes from the Arabic alyat al-hamal ("the sheep's fat tail"). In 2016, the International Astronomical Union organized a Working Group on Star Names (WGSN)[17] to catalog and standardize proper names for stars. The WGSN's first bulletin of July 2016[18] included a table of the first two batches of names approved by the WGSN; which included Alioth for this star.
This star was known to the Hindus as Añgiras, one of the Seven Rishis.[19]
In Chinese, 北斗 (Běi Dǒu), meaning Northern Dipper, refers to an asterism equivalent to the Big Dipper. Consequently, the Chinese name for Epsilon Ursae Majoris itself is 北斗五 (Běi Dǒu wu, English: the Fifth Star of Northern Dipper) and 玉衡 (Yù Héng, English: Star of Jade Sighting-Tube).[20]
Namesakes
[edit]The United States Navy's Crater class cargo ship USS Allioth (AK-109) was named after the star.
See also
[edit]References
[edit]- ^ a b c d van Leeuwen, F. (November 2007). "Validation of the new Hipparcos reduction". Astronomy and Astrophysics. 474 (2): 653–664. arXiv:0708.1752. Bibcode:2007A&A...474..653V. doi:10.1051/0004-6361:20078357. S2CID 18759600.
- ^ a b c Johnson, H. L.; et al. (1966). "UBVRIJKL photometry of the bright stars". Communications of the Lunar and Planetary Laboratory. 4 (99): 99. Bibcode:1966CoLPL...4...99J.
- ^ Evans, D. S. (June 20–24, 1966). Batten, Alan Henry; Heard, John Frederick (eds.). "The Revision of the General Catalogue of Radial Velocities". Determination of Radial Velocities and their Applications, Proceedings from IAU Symposium no. 30. 30. University of Toronto: International Astronomical Union: 57. Bibcode:1967IAUS...30...57E.
- ^ a b Tektunali, H. G. (June 1981). "The spectrum of the CR star Epsilon Ursae Majoris". Astrophysics and Space Science. 77 (1): 41–58. Bibcode:1981Ap&SS..77...41T. doi:10.1007/BF00648756. S2CID 122817347.
- ^ Shaya, Ed J.; Olling, Rob P. (January 2011). "Very Wide Binaries and Other Comoving Stellar Companions: A Bayesian Analysis of the Hipparcos Catalogue". The Astrophysical Journal Supplement. 192 (1): 2. arXiv:1007.0425. Bibcode:2011ApJS..192....2S. doi:10.1088/0067-0049/192/1/2. S2CID 119226823.
- ^ a b c d e Baines, Ellyn K.; Clark, James H., III; Schmitt, Henrique R.; Stone, Jordan M.; von Braun, Kaspar (2023-12-01). "33 New Stellar Angular Diameters from the NPOI, and Nearly 180 NPOI Diameters as an Ensemble". The Astronomical Journal. 166 (6): 268. arXiv:2505.23514. Bibcode:2023AJ....166..268B. doi:10.3847/1538-3881/ad08be. ISSN 0004-6256.
{{cite journal}}: CS1 maint: multiple names: authors list (link) - ^ a b Shulyak, D.; Krtička, J.; Mikulášek, Z.; Kochukhov, O.; Lüftinger, T. (2010-12-01). "Modelling the light variability of the Ap star ε Ursae Majoris". Astronomy & Astrophysics. 524: A66. arXiv:1009.1297. doi:10.1051/0004-6361/201015094. ISSN 0004-6361.
- ^ Royer, F.; et al. (October 2002). "Rotational velocities of A-type stars in the northern hemisphere. II. Measurement of v sin i". Astronomy and Astrophysics. 393 (3): 897–911. arXiv:astro-ph/0205255. Bibcode:2002A&A...393..897R. doi:10.1051/0004-6361:20020943. S2CID 14070763.
- ^ Nakajima, Tadashi; Morino, Jun-Ichi (2012). "Potential Members of Stellar Kinematic Groups within 30 pc of the Sun". The Astronomical Journal. 143 (1): 2. Bibcode:2012AJ....143....2N. doi:10.1088/0004-6256/143/1/2.
- ^ Kunitzsch, Paul; Smart, Tim (2006). A Dictionary of Modern star Names: A Short Guide to 254 Star Names and Their Derivations (2nd rev. ed.). Cambridge, Massachusetts: Sky Pub. ISBN 978-1-931559-44-7.
- ^ "IAU Catalog of Star Names". Retrieved 28 July 2016.
- ^ "MAST: Barbara A. Mikulski Archive for Space Telescopes". Space Telescope Science Institute. Retrieved 8 December 2021.
- ^ Morgan, B. L.; Beddoes, D. R.; Scaddan, R. J.; Dainty, J. C. (1978). "Observations of binary stars by speckle interferometry – I". Monthly Notices of the Royal Astronomical Society. 183 (4): 701–710. Bibcode:1978MNRAS.183..701M. doi:10.1093/mnras/183.4.701.
- ^ Sokolov, N. A. (March 2008). "Radial velocity study of the chemically peculiar star ɛ Ursae Majoris". Monthly Notices of the Royal Astronomical Society: Letters. 385 (1): L1 – L4. arXiv:0904.3562. Bibcode:2008MNRAS.385L...1S. doi:10.1111/j.1745-3933.2008.00419.x. S2CID 17104356.
- ^ Shulyak, D.; Paladini, C.; Causi, G. Li; Perraut, K.; Kochukhov, O. (2014). "Interferometry of chemically peculiar stars: Theoretical predictions versus modern observing facilities". Monthly Notices of the Royal Astronomical Society. 443 (2): 1629. arXiv:1406.6093. Bibcode:2014MNRAS.443.1629S. doi:10.1093/mnras/stu1259. S2CID 96452769.
- ^ Kochukhov, O.; Shultz, M.; Neiner, C. (2019). "Magnetic field topologies of the bright, weak-field Ap stars θ Aurigae and ∊ Ursae Majoris". Astronomy and Astrophysics. 621: A47. arXiv:1811.04928. Bibcode:2019A&A...621A..47K. doi:10.1051/0004-6361/201834279. S2CID 119070948.
- ^ "IAU Working Group on Star Names (WGSN)". Retrieved 22 May 2016.
- ^ "Bulletin of the IAU Working Group on Star Names, No. 1" (PDF). Archived (PDF) from the original on 2022-10-09. Retrieved 28 July 2016.
- ^ Allen, R. H. (1963). Star Names: Their Lore and Meaning (Reprint ed.). New York: Dover Publications Inc. p. 438. ISBN 0-486-21079-0. Retrieved 2012-09-04.
{{cite book}}: ISBN / Date incompatibility (help) - ^ (in Chinese) AEEA (Activities of Exhibition and Education in Astronomy) 天文教育資訊網 2006 年 6 月 15 日 Archived 2014-11-02 at the Wayback Machine
- ^
This article incorporates text from a publication now in the public domain: Chambers, Ephraim, ed. (1728). "Allioth". Cyclopædia, or an Universal Dictionary of Arts and Sciences (1st ed.). James and John Knapton, et al.
Alioth
View on GrokipediaStellar characteristics
Physical properties
Alioth is a massive A-type star with a mass of 2.91 M⊙, significantly greater than the Sun's, which places it among the more evolved members of its spectral class.[3] Its radius measures 4.29 R⊙, making it substantially larger than the Sun and contributing to its high luminosity of 104.4 ± 9.3 L⊙.[5] The effective temperature of the star's photosphere is 9,200 ± 200 K, indicative of its hot, white appearance, while the surface gravity is log g = 3.6 (cgs), reflecting its expanded envelope consistent with post-main-sequence evolution.[3]| Property | Value | Unit |
|---|---|---|
| Mass | 2.91 | M⊙ |
| Radius | 4.29 | R⊙ |
| Luminosity | 104.4 ± 9.3 | L⊙ |
| Effective temperature | 9,200 ± 200 | K |
| Surface gravity | log g = 3.6 | (cgs) |
Spectral classification and variability
Alioth is classified as an A0p Cr star, a chemically peculiar A-type star of luminosity class III-IV exhibiting spectral features indicative of an α² Canum Venaticorum (α² CVn) variable.[7] This classification reflects its evolved luminosity class (III-IV) and peculiarities in line strengths, including enhanced chromium and europium lines, with the "p" denoting chemical anomalies driven by atomic diffusion in its stably stratified atmosphere. The star's spectrum shows a white-blue hue, consistent with its B-V color index of -0.02. As the brightest member of Ursa Major, Alioth has an apparent visual magnitude of 1.77, making it a prominent naked-eye object, while its absolute magnitude is approximately -0.2.[8] It displays photometric variability typical of α² CVn stars, with small-amplitude brightness changes of about 0.02 magnitudes in the V band, resulting in a double-wave light curve modulated by rotation.[9] These variations arise from surface abundance inhomogeneities that alter opacity across different wavelengths, with larger amplitudes in the ultraviolet (up to 0.12 mag) decreasing toward the infrared.[9] The star's chemical peculiarities include overabundances of elements such as chromium (mean log ε(Cr) ≈ -5.7), iron (log ε(Fe) ≈ -4.65), strontium, manganese (log ε(Mn) ≈ -5.6), and europium, contrasted by depletions in titanium (log ε(Ti) ≈ -7.6).[7] Silicon abundances also vary across the surface, contributing to the peculiar spectral profile. These anomalies stem from radiative diffusion processes, which segregate elements based on their ionization and migration velocities in the absence of significant convection. Observations reveal periodic variations in spectral lines of these elements, tied to the star's rotation, with enhancements concentrated at magnetic poles and depletions at the equator for heavy metals like Cr, Fe, and Sr.Magnetic field and rotation
Alioth exhibits a relatively weak magnetic field compared to other chemically peculiar Ap stars, with a polar field strength of approximately 400 G. This is roughly 600–1600 times the average surface magnetic field of Earth (0.25–0.65 G) but about 10 times weaker than the field in prototypical Ap stars such as α Canum Venaticorum, which has longitudinal field extrema exceeding 4000 G.[10][11] The field is predominantly dipolar in geometry, as inferred from its sinusoidal variation over the rotation cycle.[10] The longitudinal component of the magnetic field, measured via the Zeeman effect in circularly polarized spectra, varies smoothly from +128 G to -64 G across the 5.0887-day rotation period.[10] Earlier measurements suggested larger variations up to +1100 G and -300 G, but high-precision observations confirm the weaker values, resolving prior discrepancies.[12] The obliquity of the magnetic axis relative to the rotation axis is estimated at 46°–90°, with detailed modeling of surface distributions favoring values around 62°–64°.[10][12] This rapid rotation, with an equatorial velocity of v sin i ≈ 25 km s⁻¹, induces stellar oblateness and Doppler shifts in spectral lines, broadening them and contributing to the observed line profile variations.[12] The misaligned magnetic and rotation axes cause the field to modulate the distribution of chemical elements on the surface, forming spots enriched in metals like Cr, Fe, and Mn at the magnetic poles.[12] As these spots rotate into and out of view, they produce periodic changes in brightness (up to 0.02 mag) and spectral features, consistent with the oblique rotator model. No stellar companions have been confirmed to influence the rotation or variability, with radial velocity changes attributed solely to the rotational modulation of surface inhomogeneities.Kinematics and group membership
Distance and proper motion
Alioth occupies the position in the sky at equatorial coordinates RA 12h 54m 01.8s, Dec +55° 57′ 35″ (J2000.0).[13] The most precise measurement of its distance comes from the Gaia DR3 parallax of 39.51 ± 0.16 mas, yielding a distance of 82.6 ± 0.3 light-years (25.3 ± 0.1 pc).[13] This places Alioth within the local volume of the galaxy, allowing for detailed kinematic analysis. Alioth exhibits proper motion components of +111.91 ± 0.16 mas/yr in right ascension and -8.24 ± 0.14 mas/yr in declination, as measured by Gaia DR3.[13] These values indicate the star's transverse motion across the celestial sphere relative to the solar system. The corresponding tangential velocity is 14.3 km/s.[13] Combined with its radial velocity of -12.3 km/s, the full three-dimensional space motion of Alioth is characterized by velocity components U = 14 km/s (toward the galactic center), V = 2 km/s (in the direction of galactic rotation), and W = -9 km/s (toward the north galactic pole).| Velocity Component | Value (km/s) |
|---|---|
| Radial velocity | -12.3 |
| Tangential velocity | 14.3 |
| U (galactocentric) | 14 |
| V (galactic rotation) | 2 |
| W (north galactic pole) | -9 |