Under the
Sirian Sun.
The search for planets on
Sirius star system which lies at 2.64 parsecs (8.3 ly) from Earth has
proven so far to be unfruitful. Over a period of over 1.5 centuries
since the discovery of Sirius B in 1862, a white dwarf companion,
many astronomers had hoped that the star would reveal its third
companion, a brown dwarf , which has been projected to exist by
gravitational perturbations as according to Devant et al(1).
Alvan Clark's discovery in
1862 of Sirius B was a watershed in the use of gravitational
computations to infer presence of a companion. Now we have satellites
to peer even more but still this star system has kept itself veiled
from the discovery of its children.
I would posit that there
are several reasons for the inability so far to detect planets on
Sirius. These are:
- Brightness of Sirius A causes too much 'noise' in the electronics.
- The use of filters affects the system as well and any light from the planets are also filtered.
- Focus is on a putative third star instead of possible planetary system.
- Looking for transits across the star which is not detectable due to 1. and also the the line of sight may not correspond to the star's protoplanetary disc formed millions of years ago and aligned not to the Earth's point of view.
- There is the possibility that the planets are in a polar orbit i.e. 90 degrees to our point of view, see ellipse fig.1.
- the white dwarf with its immense gravity would have in its lifetime destroyed any planets that would have formed in the system
- gravitational stability of the system indicates that planets are possible at certain locations see Devant(1), and figure 2.
- The use of gravitational microlensing is recommended.
- The launch in December 2013 of the Gaia spacecraft offers a good opportunity to look for the Einstein ring effect on Sirius.
- Gaia will study 1 billion stars and take readings on every star every six seconds. This will enable a large number of planets to be detected as the Einstein time will have been in effect for many stars.
Gaia spacecraft launched into solar orbit period of 180
days. For more information go to http://sci.esa.int/gaia/
In their paper, Thalmann
et al(2) has stipulated that precision astrometry suffers from many
insidious faults which result in errors. These include changes in
differential atmospheric refraction from ground based systems,
changes in pixel scale and orientation and other ambient conditions.
Thalmann has also confirmed the absence of dust around Sirius B and
this possibly indictates a planet sterile environment as far as the orbit of
Sirius B is concerned.
Sirius and
the “missing” planets.
The
sketch of the ellipse (courtesy wikipedia) above indicates to an
observer out in space that the star system of Sirius, has possibly a
planet that swings past 2 stars. The small black square represents
the planet(s) and the 2 blue rectangles Sirius A and B. The Y plane
rectangle is Sirius B and the X plane one is Sirius A.
Assuming
the Earth lies somewhere along or near the Y plane then it is very obvious that the planet
cannot be seen as a transit feature as it is very close to the extremly
luminous Sirius A.
Sirius
B
Companion | α CMa B |
Period (P) | 50.090 ± 0.055 yr |
Semi-major axis (a) | 7.50 ± 0.04" |
Eccentricity (e) | 0.5923 ± 0.0019 |
Inclination (i) | 136.53 ± 0.43° |
Longitude of the node (Ω) | 44.57 ± 0.44° |
Periastron epoch (T) | 1894.130 ± 0.015 |
Argument
of periastron (ω) (secondary) |
147.27 ± 0.54° |
Courtesy wikipedia.
I
would posit that the probability of life occurring near this white
dwarf is quite unlikely as in reaching that stage of stellar
evolution it has essentially destroyed any planets it had in the
past. It has tremendous gravity and is only slightly larger than the
Earth. If it has any planets they are likely to be captured from free-floating planets.
Further,
Sirius B is an X-ray source unlike Sirius A which resembles more like
our sun but is twice as large and more luminous.
α CMa A
|
|
---|---|
Mass | 2.02M☉ |
Radius | 1.711R☉ |
Luminosity | 25.4L☉ |
Surface gravity (logg) | 4.33cgs |
Temperature | 9,940K |
Metallicity [Fe/H] | 0.50dex |
Rotation | 16 km/s |
Age | 2–3 × 108years |
α CMa B
|
|
Mass | 0.978M☉ |
Radius | 0.0084 ± 3%R☉ |
Luminosity | 0.026L☉ |
Surface gravity (logg) | 8.57cgs |
Temperature | 25200K |
Sirius
B is an X-ray source.
Gravitational
microlensing and Sirius
With a white dwarf in tow the complexities of this
system are many. The historical viewpoint that sometime in the very
distant past, Sirius B went into a red giant phase and then collapsed
into a white dwarf would indicate that the possibility of Sirius A
being a captured star exists. Sirius A may have been captured along
with its putative planets and some of these then settled into stable orbits
that would not cause escape from or collisions with Sirius B.
Alternatively, accretion of stellar matter from the
Sirius B or A stars may have resulted in the unique protoplanetary
disc being formed at such alignments as to make it compatible with
the combined gravitational impulses from both stars see Fig.2.
Hence this unique alignment is one that is unexpected.
But in space, expect the unexpected.
The best possible option therefore to see the planets on
Sirius is the use of gravitational microlensing which would at the
appropriate angle provide theoretically up to 1000 times
magnification of the planets brightness.(3)
Planets in the lensing zone can be detected from 1 to 4
AU from the main star(3).
I predict that there are planets within this region based on the 90% probability given by Devant(1) for a massive brown dwarf to exist. And, drawing from Kepler's laws the period would be about 5 years around the primary.
I predict that there are planets within this region based on the 90% probability given by Devant(1) for a massive brown dwarf to exist. And, drawing from Kepler's laws the period would be about 5 years around the primary.
The expected brown dwarf is replaced by a system of
planets as well as asteroid belts as in the case of the star Vega
which so far seems to have 2 of these belts.
Mathematics
of Microlensing.
As the maths is theoretically founded on some
assumptions and to make it easier to understand, I have posted the
equation below :
The angle theta represents the size of the Einstein ring
and since the sensitivity of the Gaia instruments are reading to
values of microarcseconds, then the microlensing events are
recordable.
Planets
in a lensing zone normally around 1 to 4 AU from the primary are
detectable.(3)
For
the Sirius system, accretion of ejected material from the primary may
have severely
affected
planet formation in the proper plane because the white dwarf's
gravity would have aligned the protoplanets so much off the normal
ecliptic as to be not in the line of sight as seen from Earth.
With
time, the planets form at angles that are severely off the ecliptic.
Numerical
stability algorithms show that material is stable in Binary stars to
about 3 AU from the primary as long as the inclination of the
protoplanetary disc is around 60°(4).
But
this has not accounted for gravitational pertubations from white
dwarf companions as in the case of Sirius.
Please
do read my references for further details.
References:
- Is Sirius a triple star? D.Benest and JL Duvent. Astron.Astrophys. 299, 621-628(1995).
- Piercing the glare: A direct imaging search for planets in the Sirius system.C Thalman et al. Astrophysical Journal Letters, 732:L34, May 10, 2011.
- Detecting Earth-mass planets with gravitational microlensing. DP Bennett and Sun Hong Rhee. Astrophysical Journal 472:660-664, 1996 Dec 1st.
- Discovery of a Jupiter/Saturn analog using gravitational microlensing. Gaudi et al.
Science 319, 927 (2008).
For
mathematics of gravitational microlensing please read :
Strong
gravitational lensing: relativity in action.
Joachim
Wambsganss,1 and B
Paczynski 2
1Astronomisches
Rechen-Institut, Zentrum f¨ur Astronomie der Universit¨at
Heidelberg,
M¨onchhofstr.
12-14, 69120 Heidelberg, Germany email: jkw@uni-hd.de
2Visitor,
Dept. of Astrophysical Sciences, Princeton University,Princeton, NJ
08540, USA.
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