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Introduction to Planetary Science

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290 chapter 14<br />

Figure 14.8. Relation of the Main ring of Jupiter <strong>to</strong> the<br />

inner satellites: Metis and Adrastea, Amalthera, and Thebe.<br />

The outer edge of the Main ring coincides with the orbits<br />

of Metis and Adrastea whose periods of revolution resonate<br />

with the period of Amalthea (<strong>Science</strong> Brief 14.7.1). In<br />

addition, the Main ring is located inside the Roche limit<br />

for objects having a density of 20g/cm 3 in a region where<br />

particles cannot accrete <strong>to</strong> form a solid body because of<br />

tidal forces exerted by Jupiter. The satellites of Jupiter<br />

are located outside the Roche limit, except Metis and<br />

Adrastea, both of which appear <strong>to</strong> be rocky objects having<br />

superior mechanical strength. Adapted from Hartmann<br />

(2005, Figure 3.14)<br />

For this reason, rings can exist only inside the<br />

Roche limit. Particles that orbit a planet outside<br />

of the Roche limit could, in principle, form a<br />

larger solid body in case that body can withstand<br />

the stresses caused by planetary tides.<br />

The Roche limit r R is expressed by the<br />

equation (Hartmann, 2005, p. 60):<br />

r R = 244<br />

1/3 M<br />

S<br />

R (14.1)<br />

where M is the density of the planet, R is its<br />

radius, and S is the density of the satellite. In<br />

case M = S, the Roche limit is r R = 244 R.<br />

Note that equation 14.1 implies that the Roche<br />

limit for a satellite orbiting a planet such as<br />

Jupiter decreases with increasing density of the<br />

satellite. In other words, satellites composed of<br />

rocks can approach more closely than satellites<br />

composed of ice before they are broken up by<br />

the tidal force of the planet. Therefore, the rings<br />

that orbit the large gas planets may have formed<br />

when objects composed of rocks or ice came<br />

<strong>to</strong>o close <strong>to</strong> a planet and were broken up by<br />

tidal forces. Alternatively, particles that initially<br />

formed a disk around a planet at the time of its<br />

accretion may have been preserved in the rings<br />

by the fact that tidal forces prevented them from<br />

coalescing in<strong>to</strong> a satellite.<br />

An additional constraint on ring particles is<br />

provided by the Poynting-Robertson effect which<br />

arises from the way in which centimeter-sized<br />

particles in stable orbits absorb and reradiate<br />

sunlight (Duncan and Lissauer, 1999). The effect<br />

causes particles <strong>to</strong> lose energy and <strong>to</strong> spiral<br />

<strong>to</strong>ward the mother planet. As ring particles<br />

descend in<strong>to</strong> lower orbits, they are further slowed<br />

by atmospheric friction and eventually fall in<strong>to</strong><br />

the atmosphere of their mother planet. Consequently,<br />

a gap is observed between the <strong>to</strong>p of the<br />

atmosphere and the innermost ring of a planet.<br />

14.4 The Spacecraft Galileo<br />

Much of what is known about Jupiter and its<br />

satellites was learned during flybys of the robotic<br />

spacecraft Pioneers 10 and 11 and by Voyagers<br />

1 and 2. The Voyagers recorded spectacular<br />

images of Jupiter and its Galilean satellites,<br />

which provided a great deal of information that

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