We use cookies to distinguish you from other users and to provide you with a better experience on our websites. Close this message to accept cookies or find out how to manage your cookie settings.
To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure no-reply@cambridge.org
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
By
P. D. Nicholson, Cornell University Ithaca, New York, USA,
I. De Pater, University of California, Berkeley Berkeley, California, USA,
R. G. French, Wellesley College Wellesley, Massachusetts, USA,
M. R. Showalter, SETI Institute Mountain View, California, USA
By
I. De Pater, University of California, Berkeley Berkeley, California, USA,
S. Renner, University of Lille Lille, FRANCE,
M. R. Showalter, SETI Institute Mountain View, California, USA,
B. Sicardy, Observatoire de Paris and University Pierre et Marie Curie Paris, FRANCE
By
B. Sicardy, Observatoire de Paris and University Pierre et Marie Curie Paris, FRANCE,
M. El Moutamid, Cornell University Ithaca, New York, USA,
A. C. Quillen, University of Rochester Rochester, New York, USA,
P. M. Schenk, Lunar and Planetary Institute Houston, Texas, USA,
M. R. Showalter, SETI Institute Mountain View, California, USA,
K. Walsh, Southwest Research Institute Boulder, Colorado, USA
By
I. De Pater, University of California, Berkeley Berkeley, California, USA,
D. P. Hamilton, University of Maryland College Park, Maryland, USA,
M. R. Showalter, SETI Institute Mountain View, California, USA,
H. B. Throop, Planetary Science Institute Tucson, Arizona, USA,
J. A. Burns, Cornell University Ithaca, New York, USA
Most studies of light scattering in planetary rings have assumed layers which are many particles thick, plane parallel, and homogeneous. However, real rings may be thin, vertically warped, and clumpy. We have developed a ray tracing code which calculates the light scattered by an arbitrary distribution of particles. This approach promises to clarify a number of puzzling observations of the Saturnian and Uranian rings.
(1) Many studies have concluded that Saturn's rings are many particles thick (e.g. Lumme et al. 1983), whereas dynamical calculations predict that optically thick rings should be physically thin (Wisdom & Tremaine 1988 and references therein). Lumme et al. argue that the particles in Saturn's B Ring fill only 2% of the volume of the ring, while Wisdom and Tremaine predict a filling factor of 20% or more.
The claim that Saturn's rings are thick is based on their observed opposition surge, a rapid brightening (0.3 mag in the V band) which occurs at phase angles below about 1.5°. The surge is attributed to particles covering their own shadows near opposition. Shadowing can occur either between discrete particles, or within the surface structure of a particle. The range in phase angle over which the brightening takes place is proportional to the volume filling factor of the ring or surface. Thus the very narrow opposition effect of Saturn's rings implies a very porous ring, unless individual particles backscatter extremely strongly.
Recommend this
Email your librarian or administrator to recommend adding this to your organisation's collection.