HD 15082
Observation data Epoch J2000 Equinox J2000 | |
---|---|
Constellation | Andromeda |
Right ascension | 02h 26m 51.05823s[1] |
Declination | +37° 33′ 01.7330″[1] |
Apparent magnitude (V) | 8.3[2] |
Characteristics | |
Spectral type | kA5 hA8 mF4[3] |
Variable type | δ Sct[2] |
Astrometry | |
Proper motion (μ) | RA: –1.26[1] mas/yr Dec.: –9.22[1] mas/yr |
Parallax (π) | 8.65 ± 0.80[1] mas |
Distance | 380 ± 30 ly (120 ± 10 pc) |
Details | |
Mass | 1.55 ± 0.04[3] M☉ |
Surface gravity (log g) | 4.3 ± 0.2[2] cgs |
Temperature | 7,400 ± 200[2] K |
Metallicity [Fe/H] | 0.1 ± 0.2[3] dex |
Rotational velocity (v sin i) | 86[2] km/s |
Age | 100[4] Myr |
Other designations | |
HD 15082 (also known as WASP-33) is a star located roughly 378 light years away[3] in the northern constellation of Andromeda.[5] The star is a Delta Scuti variable and a planetary transit variable. It is the first Delta Scuti variable known to host a planet.[6] A hot Jupiter type extrasolar planet orbits this star with an orbital period of 1.22 days.
In common with many rapidly rotating stars of spectral type A, the stellar classification of HD 15082 is more challenging to discern. The hydrogen lines and effective temperature of the star are similar to spectral type A8, however the calcium II K line resembles that of an A5 star, and the metallic lines are more similar to an F4 star. The spectral type is thus written kA5 hA8 mF4.[3] This suggests that HD 15082 is an Am star.[3]
The exoplanet, HD 15082b (also known as WASP-33b) orbits so close to its star that its surface temperature is about 3,200 °C (5,790 °F).[7]
Planet
Companion (in order from star) |
Mass | Semimajor axis (AU) |
Orbital period (days) |
Eccentricity | Inclination | Radius |
---|---|---|---|---|---|---|
b | < 4.59 MJ | 0.02558 (± 0.00023) | 1.21986967 (± 4.5e-07) | 0 | 87.67° | 1.438 RJ |
In 2010, the SuperWASP project announced the discovery of an extrasolar planet, designated HD 15082 b, orbiting the star. The discovery was made by detecting the transit of the planet as it passes in front of its star, an event which occurs every 1.22 days. As the planet crosses the star's disc, it causes the rotational broadening signature in the star's spectrum to change, enabling the determination of the sky-projected angle between the star's equator and the orbital plane of the planet to be determined. (This differs from the Rossiter–McLaughlin effect which is observed for radial velocity measurements). For HD 15082 b, this angle is about 250 degrees, indicating that it is in a retrograde orbit. Limits from radial velocity measurements imply it has less than 4.1 times the mass of Jupiter.[3]
June 2015 NASA reported the exoplanet has a stratosphere, and the atmosphere contains titanium oxide which creates the stratosphere. Titanium oxide is one of only a few compounds that is a strong absorber of visible and ultraviolet radiation, which heats the atmosphere, and able to exist in a gas-state in a hot atmosphere.[8][9]
Non-Keplerian features of motion for HD 15082 b
In view of the high rotational speed of its parent star, the orbital motion of HD 15082 b may be affected in a measurable way by the huge oblateness of the star and effects of general relativity.
First, the distorted shape of the star makes its gravitational field deviate from the usual Newtonian inverse-square law. The same is true for the Sun, and part of the precession of the orbit of Mercury is due to this effect. However, it is estimated to be greater for HD 15082b.[10]
Other effects will also be greater for HD 15082b. In particular, precession due to general relativistic frame-dragging should be greater for HD 15082b than for Mercury, where it is so far too small to have been observed. It has been argued that the oblateness of HD 15082 could be measured at a percent accuracy from a 10-year analysis of the time variations of the planet's transits.[10] Effects due to the planet's oblateness are smaller by at least one order of magnitude, and they depend on the unknown angle between the planet’s equator and the orbital plane, perhaps making them undetectable. The effects of frame-dragging are slightly too small to be measured by such an experiment.
Notes
- ↑ Parameters from the photometric + radial velocity solution in table 3 of Cameron et al. (2010). Different analysis methods result in slightly different parameters, see Cameron et al. (2010) for details.
References
- 1 2 3 4 5 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
- 1 2 3 4 5 Herrero, E.; et al. (February 2011), "WASP-33: the first δ Scuti exoplanet host star", Astronomy and Astrophysics, 526: L10, arXiv:1010.1173, Bibcode:2011A&A...526L..10H, doi:10.1051/0004-6361/201015875
- 1 2 3 4 5 6 7 8 Collier Cameron, A.; et al. (2010). "Line-profile tomography of exoplanet transits - II. A gas-giant planet transiting a rapidly rotating A5 star". Monthly Notices of the Royal Astronomical Society. 407: 507. arXiv:1004.4551. Bibcode:2010MNRAS.407..507C. doi:10.1111/j.1365-2966.2010.16922.x.
- ↑ Moya, A.; et al. (November 2011), "High spatial resolution imaging of the star with a transiting planet WASP-33", Astronomy & Astrophysics, 535: A110, arXiv:1110.3160, Bibcode:2011A&A...535A.110M, doi:10.1051/0004-6361/201116889
- ↑ "WASP-33 b". ETD - Exoplanet Transit Database. Retrieved 2010-04-28.
- ↑ "Discovery Of A Pulsating Star That Hosts A Giant Planet", Science Daily, January 19, 2011
- ↑ "Hottest planet is hotter than some stars". Retrieved 2015-06-12.
- 1 2 "NASA's Hubble Telescope Detects 'Sunscreen' Layer on Distant Planet". Retrieved 2015-06-11.
- ↑ Haynes, Korey; Mandell, Avi M.; Madhusudhan, Nikku; Deming, Drake; Knutson, Heather (2015-05-06). "Spectroscopic Evidence for a Temperature Inversion in the Dayside Atmosphere of the Hot Jupiter WASP-33b". arXiv:1505.01490.
- 1 2 Iorio, Lorenzo (2010-07-25), Classical and relativistic node precessional effects in WASP-33b and perspectives for detecting them, arXiv:1006.2707, Bibcode:2011Ap&SS.331..485I, doi:10.1007/s10509-010-0468-x