On the structural law of exoplanetary systems.pptx
1. ON THE STRUCTURAL LAW OF
EXOPLANETARY SYSTEMS
Patricia Lara, Arcadio Poveda & Christine Allen
Instituto de Astronomía, UNAM
ICNAAM 2012
Kos, Greece
19-25 September 2012
5. Titius-Bode Relation (TBR)
Original TBR
where n = 0, 3, 6,12 ..
Classic TBR
(modern formulation)
where n = -∞ , 0, 1, 2, …
10
4
n
a n
a 2
3
.
0
4
.
0
Exponential TBR
where n = 1, 2, 3, …
n
n k
P
P
0
Dermott´s law
where n = 0, 1, 2, …
bn
n
n e
a
C
a
a 0
0
6. TBR in the Solar System
Sistema Solar
a = 0.1912e0.5594n
R
2
= 0.992
0
5
10
15
20
25
30
35
0 1 2 3 4 5 6 7 8 9 10
n
a
(AU)
Poveda &Lara, 2008
Solar System
8. 55 Cancri
Distance
12.34 (± 0.4) pc
Spectral Type
K0IV-V
Mass
0.905 (± 0.015) M
Age
10.2 (± 2.5) Gyr
Radius
0.943 (± 0.01) R
Metallicity [Fe/H]
0.31 (± 0.04)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7
55 Cnc e b c f d
Orbital period (days) 0.7365449
± 5e-06
14.651262
± 0.0008
44.3446
± 0.007
260.7
± 1.1
5218
± 230
Eccentricity 0.057 0.0159 0.053
a (AU) [measured] 0.0156 0.1148 0.2403 0.781 - 5.76 -
a (AU) [predicted] 0.0239 0.074 0.2292 0.7103 2.2011 6.8214 21.14
exoplanet.eu
9. υ Andromeda
Distance
13.47 (± 0.13) pc
Spectral Type
F8 V
Mass
1.27 (± 0.06) M
Age
3.8 (± 1) Gyr
Radius
1.631 (± 0.014) R
Metallicity [Fe/H]
0.09 (± 0.06)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6
Ups And b c d e
Orbital period (days) 4.6171
± 4.7e-05
237.7
± 0.2
1302.61 3848.86
± 0.74
Eccentricity 0.013 0.24 0.274 0.00536
a (AU) [measured] 0.059 - 0.861 2.55 5.2456 -
a (AU) [predicted] 0.069 0.218 0.683 2.145 6.732 21.13
10. μ Ara
Distance
15.3 pc
Spectral Type
G3 IV-V
Mass
1.08 (± 0.05) M
Age
6.41 Gyr
Radius
1.245 (± 0.255) R
Metallicity [Fe/H]
0.28 (± 0.04)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6
mu Ara c d b e
Orbital period (days)
9.6386
± 0.0015
310.55
± 0.83
643.25
± 0.9
4205.8
± 758.9
Eccentricity 0.172 0.0666 0.128 0.0985
a (AU) [measured] 0.09094 - 0.921 1.5 5.235 -
a (AU) [predicted] 0.098 0.263 0.704 1.885 5.046 13.507
11. Gliese 876
Distance
4.7 (± 0.01) pc
Spectral Type
M4 V
Mass
0.334 (± 0.03) M
Age
2.5 (+2.5
-2.4) Gyr
Radius
0.36 R
Metallicity [Fe/H]
0.05 (± 0.2)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7
Gliese 876 d c b e
Orbital period (days) 1.93778
± 2.0e-05
30.0881
± 0.0082
61.1166
± 0.0086
124.26
± 0.7
Eccentricity 0.207 0.25591 0.0324 0.055
a (AU) [measured] 0.020807 - - 0.12959 0.208317 0.3343
a (AU) [predicted] 0.022 0.038 0.067 0.117 0.205 0.36 0.63
12. KOI-730
Apparent Magnitude V
15
Mass
1.07 M
Effective Temperature
5590 K
Radius
1.1 R
n = 1 n = 2 n = 3 n = 4 n = 5
KOI-730 e c b d
Orbital period
(days)
7.3831
± 4.0e-04
9.8499
± 3.0e-04
14.7903
± 0.0002
19.7216
± 0.0004
a (AU) [measured] 0.076 0.092 0.12 0.145 -
a (AU) [predicted] 0.075 0.094 0.117 0.146 0.182
13. HR 8799
Distance
39.4 (± 0.1) pc
Spectral Type
A5V
Mass
1.56 M
Age
0.06 (+0.1
-0.03) Gyr
Radius
1.5 (± 0.3) R
Metallicity [Fe/H]
-0.47
n = 1 n = 2 n = 3 n = 4 n = 5
HR 8799 e d c b
Orbital period (days) 18000 41 054 82 145 164 250
a (AU) [measured] 14.5 27 42.9 68 -
a (AU) [predicted] 15.214 25.333 42.183 70.239 116.957
14. Gliese 581
Distance
6.21 (± 0.1) pc
Spectral Type
M2.5 V
Mass
0.31 (± 0.02) M
Age
8 (+3
-1) Gyr
Radius
0.3 (± 0.01) R
Metallicity [Fe/H]
-0.135
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7
Gliese 581 e b c d
Orbital period (days)
3.14945
± 1.7e-04
5.36865
± 9e-05
12.9182
± 0.0022
66.64
± 0.14
Eccentricity 0.32 0.031 0.07
a (AU) [measured] 0.028 0.041 0.073 - - 0.22 -
a (AU) [predicted] 0.029 0.043 0.066 0.099 0.15 0.227 0.344
15. Kepler-20
Distance
290 (± 30) pc
Spectral Type
G8
Mass
0.912 (± 0.035) M
Age
8.8 (+4.7
-2.7) Gyr
Radius
0.944 (+0.06
-0.095)R
Metallicity [Fe/H]
0.02 (± 0.04)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7 n = 8
Kepler-20 b e c f d
Orbital period (days) 3.6961219
6.098493
± 6.5 e-05
10.85092
± 1.3 e-05
19.57706
± 0.00052
77.61185
Eccentricity < 0.32 - < 0.4 0.09 < 0.6
a (AU) [measured] 0.04537 0.0507 0.093 0.11 - - 0.3453 -
a (AU) [predicted] 0.042 0.059 0.083 0.118 0.168 0.238 0.337 0.477
16. Kepler-33
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7
Kepler-33 b c d e f
Orbital period (days)
5.66793
± 0.00012
13.17562
± 1.4 e-04
21.77596
± 1.1 e-04
31.7844
± 0.00039
41.02902
± 0.0004
a (AU) [measured] 0.0677 - 0.1189 0.1662 0.2138 0.2535 -
a (AU) [predicted] 0.07 0.091 0.12 0.157 0.206 0.27 0.354
Apparent Magnitude V
14
Mass
1.291 (+0.063
-0.121) M
Effective Temperature
5904 K
Radius
1.82 (+0.14
-0.18) R
17. HD 10180
Distance
39.4 (± 1) pc
Spectral Type
G1V
Mass
1.06 (± 0.05) M
Age
4.3 (± 0.5) Gyr
Metallicity [Fe/H]
0.08 (± 0.01)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7
HD 10180 c d e f g h
Orbital period (days) 5.75979
± 0.0001
16.3579
± 0.038
49.745
± 0.022
122.76
± 0.17
601.2
± 8.1
2222
± 91
Eccentricity 0 0.088 0.026 0.135 0.19 0.08
a (AU) [measured] 0.0641 0.1286 0.2699 0.4929 1.422 3.4 -
a (AU) [predicted] 0.058 0.128 0.282 0.621 1.369 3.019 6.655
18. Kepler-11
Spectral Type
G
Mass
0.95 (± 0.1) M
Age
8 (± 2) Gyr
Radius
1.1 (± 0.1) R
Metallicity [Fe/H]
0 (± 0.1)
n = 1 n = 2 n = 3 n = 4 n = 5 n = 6 n = 7 n = 8
Kepler-11 b c d e f g
Orbital period (days)
10.30375
± 0.00016
13.02502
± 8 e-05
22.68719
± 0.00021
31.9959
± 0.00028
46.68876
± 0.00074
118.37774
± 0.00112
Eccentricity 0 0 0 0 0 0
a (AU) [measured] 0.091 0.106 0.159 0.194 0.25 - 0.462 -
a (AU) [predicted] 0.087 0.114 0.15 0.198 0.26 0.342 0.449 0.591
19. In summary…
Exoplanetary systems with 4 observed planets
(with vacancies and extrapolations)
υ And 1 vacancy
n = 2 a = 0.218 AU
n = 6 a = 21.13 AU
KOI-730 0 vacancies
n= 5 a = 0.182 AU
Gliese 581 2 vacancies
n = 4 a = 0.099 AU
n =5 a=0.15 AU**
n= 7 a = 0.63 AU
Gliese 876 2 vacancies
n = 2 a = 0.038 AU
n = 3 a = 0.067 AU
n = 7 a = 0.63 AU
μ Ara 1 vacancy
n = 2 a = 0.263 AU
n = 6 a = 13.507 AU
HR 8799 0 vacancies
n = 5 a = 116.957 AU
20. Exoplanetary systems with
5 planets
55 Cancri 1 vacancy
n = 5 a= 2.20 AU
n = 7 a = 21.14 AU
Kepler-20 2 vacancies
n = 5 a = 0.168 AU
n = 6 a = 0.238 AU
n = 8 a = 0.477 AU
Kepler-33 1 vacancy
n = 2 a = 0.091 AU
n = 7 a = 0.354 AU
Exoplanetary systems with
6 planets
HD 10180 0 vacancies
n = 7 a = 6.655 AU
Kepler-11 1 vacancy
n = 6 a = 0.342 AU
n = 8 a = 0.591 AU
21. Conclusions
The results shown here demonstrate that all 11 exoplanetary
systems currently known to harbor four or more planets obey aTB-
like structural relation .
The two parameters entering the exponential formulation used
here characterize two different aspects of the systems. a0 is
essentially a measure of the overall compactness of the planetary
system. b, on the other hand, characterizes the separation (in units
of a0) between successive planets in the system.
We find no relation between the value of b and the intrinsic
characteristics (angular momentum, ratio between the stellar and
planetary mass, etc.) of the systems considered here.
This seems to suggest that the origin of theTB relation is not
related to the formation mechanisms of the systems, but rather to
their subsequent dynamical evolution.
23. For once pay attention to the widths of the planets from each other
and notice that they are distant from each other almost in a
proportion as their bodily heights increase. Given the distance from
the Sun to Saturn as 100 units, then Mercury is distant 4 such units
from the Sun,Venus 4+3=7 of the same; the Earth 4+6=10; Mars
4+12=16. But see, from Mars to Jupiter there comes forth a
departure from this so exact progression.
From Mars follows a place of 4+24=28 such units, where at the
present neither a chief nor a neighboring planet is to be seen. And
shall the Builder have left this place empty? Never! Let us
confidently wager that, without doubt, this place belongs to the as
yet still undiscovered satellites of Mars; let us add that perhaps
Jupiter also has several around itself that until now have not been
seen with any glass. Above this, to us unrevelead, position ariases
Jupiter’s domain of 4+48=52; and Saturn’s at 4+96=100 units.What
a praiseworthy relation!
First I would like thank yo the organizing comitte for invite me to this event
I´m here to present my work that I being doing with my advisors Dr. Arcadio Poveda and Mrs Christine Allen
The title of this talk is On the structural law fo exoplanetary systems
Well What is it about?
The major semi-axes of the Solar System obey a simple geometric progression know the Titius-Bode Law.
The Titius-Bode Law is not really a law in the physical sense but rather a numerical relation. SO because of that we will call it
Titius-Bode relation or TBR.
Here is the mathematical relation for the Solar system where “a” gives the distance in astronomical units for the corresponding orbital number.
The TBR was born and prevale until our days because of two astronomers: Johann Daniel Titius and Johann Elert Bode
Titius was the first to declare it and Bode using his fame and prestige promote it every time that he has oportunity.
The discovery of the fith planet in 55 cancri (THAT AT THE TIME WAS THE EXOPLANETARY SYSTEM WITH MOST PLANETS OBSERVED)
Who motivated us to try TBR to this exoplanetary system.
Here we will show that the others 10 systems to harbor four or more planets also obey a structural law.
If we put in a mathematical form what Titius state orally, the ecuation will be like this…
We can see that Titius scaleated the distance from the Sun to the Earth to 10 units so the orbital number follow this progression where for Mercury is 0, 3 for Venus, 6 to the Earth.
Through the years the Original TBR suffer modifications for the Solar System in the orbital number, here we can observed that for Mercury correspond –infinity, 0 for Venus, 1 for the Earth and so on.
In 1968, Dermott et al shown that the major satellite of Jupiter, Saturn and Uranus obey a similar progression of…
For Keplerian orbits Dermorr’s law will obey a similar law like this….. And the two parameters to stablish in this exponential relation is Ao and B.
For the porpuose that TBR could be a structural law for planetary systems, it has to be a generalized relation.
So we applied to the solar system.
Here I show the fit to the Solar system where in the horizontal axis is the orbital number and in the vertical axis is the distances in astronomic units, and looks very well and this fit along with 55 cancri was published in paper of Poveda and Lara, for 55 Cancri we will see later his fit
Also we apply TBR to the major satellite of Jupiter, Saturn and Uranus.
And every fit looks good and here we have to pay attention to the Gallilean Satellite. Io, Europe and Ganimedes are in resonance know as the Laplacian resonance (1:2:4) and this system is an exemplar example of the TBR.
This the fit for 55 Cancri, and here we observed the orbital parameters and the observed distances.
In the paper of Poveda and Lara, 55 Cancri e has a major semi-axes of 0.038 but in 2010 Dawson et al argued that the major semi-axis of 55 Cancri is 0.0156.
Because of that I show the fit with the corrected distance.
This fit show a vacancy in the orbital 5, and we predict a planet as yet to be found at 2.2 AU. Also we extrapolate to the orbital 7 and with less ceartanty we predict a planet in the orbital 7 with a major semi-axis of 21.14
Now we start to analize the exoplanetary systems with 4 planets.
We see the the exoplanetary system of Upsilon Andromeda. Also we the observed and predicted distances by TBR.
TBR fir show a vacancy in the orbital 2 with a major semi-axis of