name=gosset/>
The stars do not eclipse each other, but they are deformed by the gravity and show small brightness variations during the orbit. These brightness variations are regular and consistent over long periods, so the orbital period is known accurately. The inclination can be estimated from the mass function and the colliding winds. The eccentricity is small and the most accurate model of spectral line profile variations during the orbit gives an eccentricity of 0.2. The semi-major axis of the orbit is {{solar radius|35.4}}, with the WO star moving in an ellipse of semi-major axis {{solar radius|30}} and the more massive O companion in an ellipse of semi-major axis {{solar radius|5.4}}. The separation of the stars varies from {{solar radius|28}} to {{solar radius|42}}.[12]
Although the hot secondary star produces what would typically be considered a fast stellar wind, it is entirely overpowered by the wind from the primary star. The shock front where the winds collide is approximately a cone around the O star with a half angle of 50°. The apex of the shock cone is estimated to lie at {{solar radius|25}} from the WO stars and {{solar radius|10}} from the O star. {{solar radius|10}} is comparable to the radius of a typical non-supergiant O5 star so that its own wind is forced back against the surface of the star.[12]
Variability
WR 30a shows regular and continuous brightness variations of 0.02 magnitudes with a stable period of 4.6 days. These are ascribed to the orbital motion and to the deformed shapes of the two stars. In addition, the system shows occasional very rapid brightness of up to 0.2 magnitudes. These brightness changes have only been seen at visual wavelengths and last for only a few hours. At blue wavelengths the variations are either not seen, or sometimes a small opposite brightness change. They are not predictable but there is a possible period around three days. The cause of these brightness changes is completely unknown.[35]
Features
The primary star, of spectral classification WO4, is one of the very few known oxygen-sequence Wolf-Rayet stars, just four in the Milky Way galaxy and five in external galaxies. Modelling the atmosphere gives a luminosity around {{solar luminosity|195,000|link=y}}. It is a very small dense star, with a radius less than the sun's but with a mass nearly 10 solar masses. Very strong stellar winds, with a terminal velocity of 4,500 kilometers per second are causing WR 93b to lose over {{solar mass|10−5}}/year.[5] For comparison, the Sun loses (2-3) x 10−14 solar masses per year due to its solar wind, several hundred million times less than WR 30a.
The secondary star has an O5 spectral class. It is not a supergiant, but could be a main sequence or giant star. Some helium lines and nitrogen emission is detected in the spectrum, indicating the mixing of fusion products to the surface and a strong stellar wind.[12]
The secondary star is visually over 10 times brighter than the primary and over five times more massive, although the primary dominates the appearance of the spectrum. Researchers are careful to avoid ambiguity about the star defined as the primary and typically refer to the components as "WR" and "O".[5][18]
WR 30a is a very strong x-ray source. This is expected for a colliding-wind binary, but the source of the x-rays has not been conclusively determined. They may have a thermal or non-thermal origin.[9]
Evolutionary status
WO Wolf-Rayet stars are the last evolutionary stage of the most massive stars before exploding as supernovae, possibly with a gamma-ray burst.[41] It is very likely that WR 30a is on its last stages of nuclear fusion, near or beyond the end of helium burning.[42] Single-star evolutionary models of the WO component of WR 30a suggest it started life as a rapidly rotating {{solar mass|120}} star which has now lost over 90% of its mass.[35]
See also
- WR 102
- WR 142
- WR 93b
- List of supernova candidates
References
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