Physical properties of Saturn's rings

1984 ◽  
Vol 75 ◽  
pp. 211-217 ◽  
Author(s):  
Jeffrey N. Cuzzi

A review is given of important features of the rings, touching only lightly on aspects covered by other speakers (Spokes, E ring). This extended abstract will only convey the high points of the talk.Most of the material in Saturn's rings is concentrated in the B ring, with a lesser amount in the A ring and only small amounts in the C ring and Cassini Division. There is a very different character to these classical ring regions; the C and Cassini particles are darker and more neutral in color; (Smith et al. 1981, 1982). The A and B regions contain nearly all of the “small” particles, from microns to millimeters. Overall, however, the particles are fairly well characterized by Voyager radio occultation results as roughly following an r-3powerlaw between about 1 cm and a few meters (Tyler et al. 1982, Marouf et al. 1982). A fairly sharp cutoff in the size distribution is seen at radii varying with location from about 1 to about 5 meters. The material of the ring particles is probably mostly water ice (see e.g., Pollack 1975) but the redness of the rings requires the presence of minor constitutents. Combinations of ground-based radar and radio emission observations (Pollack 1975, Cuzzi and Pollack 1978; Pettengill, this issue) strongly indicate that the non-icy component comprises a small fraction of the total bulk material. In fact, mass densities derived from density waves (e.g. Holberg et al. 1982) and CRAND measurements (Cooper et al. 1982) combined with Voyager particle size measurements indicate a particle density more like that of snow or frost than that of pure ice.

Icarus ◽  
1983 ◽  
Vol 54 (2) ◽  
pp. 189-211 ◽  
Author(s):  
Essam A. Marouf ◽  
G. Leonard Tyler ◽  
Howard A. Zebker ◽  
Richard A. Simpson ◽  
Von R. Eshleman

Icarus ◽  
1986 ◽  
Vol 68 (1) ◽  
pp. 120-166 ◽  
Author(s):  
Essam A. Marouf ◽  
G. Leonard Tyler ◽  
Paul A. Rosen

1984 ◽  
Vol GE-22 (6) ◽  
pp. 656-665 ◽  
Author(s):  
Richard A. Simpson ◽  
G. Leonard Tyler ◽  
Essam A. Marouf ◽  
Howard A. Zebker ◽  
Von R. Eshleman

Icarus ◽  
1991 ◽  
Vol 93 (1) ◽  
pp. 3-24 ◽  
Author(s):  
Paul A. Rosen ◽  
G. Leonard Tyler ◽  
Essam A. Marouf

Icarus ◽  
1982 ◽  
Vol 49 (2) ◽  
pp. 161-193 ◽  
Author(s):  
Essam A. Marouf ◽  
G.Leonard Tyler ◽  
Von R. Eshleman

Icarus ◽  
2016 ◽  
Vol 279 ◽  
pp. 36-50 ◽  
Author(s):  
Richard G. Jerousek ◽  
Joshua E. Colwell ◽  
Larry W. Esposito ◽  
Philip D. Nicholson ◽  
Matthew M. Hedman

2015 ◽  
Vol 112 (31) ◽  
pp. 9536-9541 ◽  
Author(s):  
Nikolai Brilliantov ◽  
P. L. Krapivsky ◽  
Anna Bodrova ◽  
Frank Spahn ◽  
Hisao Hayakawa ◽  
...  

Saturn’s rings consist of a huge number of water ice particles, with a tiny addition of rocky material. They form a flat disk, as the result of an interplay of angular momentum conservation and the steady loss of energy in dissipative interparticle collisions. For particles in the size range from a few centimeters to a few meters, a power-law distribution of radii, ∼r−q with q≈3, has been inferred; for larger sizes, the distribution has a steep cutoff. It has been suggested that this size distribution may arise from a balance between aggregation and fragmentation of ring particles, yet neither the power-law dependence nor the upper size cutoff have been established on theoretical grounds. Here we propose a model for the particle size distribution that quantitatively explains the observations. In accordance with data, our model predicts the exponent q to be constrained to the interval 2.75≤q≤3.5. Also an exponential cutoff for larger particle sizes establishes naturally with the cutoff radius being set by the relative frequency of aggregating and disruptive collisions. This cutoff is much smaller than the typical scale of microstructures seen in Saturn’s rings.


Maxwell determined the conditions of stability of a single ring of small particles moving round a large primary. He also made some incomplete remarks on the effects of introducing a second ring. The present investigation considers in greater detail the stability of two rings of particles moving about a primary and subject to the gravitational attractions of the primary and of each other. It is shown that such a system, under conditions satisfied by the Saturnian system, is stable, the particles oscillating finitely about their mean positions. It is inferred that the Saturnian system, considered as a number of such rings, is therefore also stable.


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