1. Origin of the Different Architectures
of the Jovian and Saturnian Satellite Systems
Takanori Sasaki, Shigeru Ida (Tokyo Tech)
Glen R. Stewart (U. Colorado)

2. Jovian System v.s. Saturnian System
rocky rocky icy icy, undiff.
Io Europa Ganymede Callisto
mutual mean motion resonances (MMR)
icy
only one big body
Titan

3. Overview of this study
Circum-Planetary Disk Satellite Formation
Canup & Ward, 2002, 2006 Ida & Lin, 2004, 2008, in prep.
Satellites formed in c.-p. disk Analytical solution for
Actively-supplied accretion disk accretion timescale
Supplied from circum-stellar disk type I migration timescale
→ Analytical solution for T, Σ trapping condition in MMR

4. Overview of this study
Circum-Planetary Disk Satellite Formation
Canup & Ward, 2002, 2006 Ida & Lin, 2004, 2008, in prep.
Satellites formed in c.-p. disk Analytical solution for
Actively-supplied accretion disk accretion timescale
Supplied from circum-stellar disk type I migration timescale
→ Analytical solution for T, Σ trapping condition in MMR
Adding New Ideas Disk boundary conditions
Difference of Jovian/Saturnian systems is naturally reproduced?

5. The Ideas
Jupiter
inner cavity opened up gap in c.-s. disk
→ infall to c.-p. disk stop abruptly
Saturn
no cavity did not open up gap in c.-s. disk
→ c.-p. disk decay with c.-s. disk
Difference of “inner cavity” is from Königl (1991) and Stevenson (1974)
Difference of gap conditions is from Ida & Lin (2004)

6. Jovian System
inner cavity outer proto-satellite
@corotation radius grow faster & migrate earlier
Because the infall mass flux per unit area is constant,
the total mass flux to satellite feeding zones is larger in outer regions.

7. Jovian System
Type I migration is
halted near the inner edge
The outer most satellite migrates and sweeps up
the inner small satellites.

8. Jovian System
MMR
Proto-satellites grow & migrate repeatedly
They are trapped in MMR with the innermost satellite

9. Jovian System
Total mass of the trapped satellites > Disk mass
→ the halting mechanism is not effective
→ Innermost satellite is released to the host planet

10. Jovian System
after the gap opening → c.-p. disk deplete quickly

11. Saturnian System
No inner cavity outer proto-satellite
grow faster & migrate earlier

12. Saturnian System
fall to Saturn
Large proto-satellites migrate from the outer regions
and fall to the host planet with inner smaller satellites

13. Saturnian System
c.-p. disk depleted slowly
with the decay of c.-s. disk

14. Monte Carlo Simulation (n=100)
Parameters:
Disk viscosity (α model) α = 10−3 − 10−2
Disk decay timescale τin = 3 × 10 − 5 × 10
6 6 yr
Number of “satellite seeds” N = 10 − 20

15. Results: Distribution of the number of large satellites
Jovian Saturnian
40 80
Total count of the case
60
20 40
20
0 0
0 1 2 3 4 5 6 7 0 1 2 3 4
number of produced satellites

16. Results: Distribution of the number of large satellites
Jovian Saturnian
40 80
Total count of the case
60
20 40
20
0 0
0 1 2 3 4 5 6 7 0 1 2 3 4
number of produced satellites
inner two bodies: rocky icy satellite
& outer two bodies: icy & large enough (~MTitan)

17. Results: Properties of produced satellite systems
Jovian Saturnian
1e-3
Galilean Satellites
Titan
1e-4
Ms/Mp
1e-5 rocky component
icy component
1e-6
0 10 20 30 0 10 20 30
a/Rp

18. Results: Properties of produced satellite systems
Jovian Saturnian
1e-3
Galilean Satellites
Titan
1e-4
Ms/Mp
1e-5 rocky component
icy component
1e-6
0 10 20 30 0 10 20 30
a/Rp
inner three bodies the largest satellite
are trapped in MMR has ~90% of total satellite mass

19. Summary
• Jovian Satellite System v.s. Saturnian Satellite System
Difference of size, number, location, and compositions
• Satellite Accretion/Migration in Circum-Planetary Disk
Canup & Ward (2002, 2006) + Ida & Lin (2004, 2008, in prep.)
• The Ideas of Disk Boundary Conditions
Difference of inner cavity opening and gap opening conditions
• Monte Carlo Simulations
Difference of Jovian/Saturnian system are naturally reproduced