2009
DOI: 10.1016/j.icarus.2009.03.011
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The viscous overstability, nonlinear wavetrains, and finescale structure in dense planetary rings

Abstract: This paper addresses the fine-scale axisymmetric structure exhibited in Saturn's A and B-rings. We aim to explain both the periodic microstructure on 150-220m, revealed by the Cassini UVIS and RSS instruments, and the irregular variations in brightness on 1-10km, reported by the Cassini ISS. We propose that the former structures correspond to the peaks and troughs of the nonlinear wavetrains that form naturally in a viscously overstable disk. The latter variations on longer scales may correspond to modulations… Show more

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Cited by 23 publications
(23 citation statements)
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References 57 publications
(130 reference statements)
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“…Clear signatures of these features in a wavelet plot are presented in Appendix A for a simulation with a much longer domain. This configuration of dynamical elements reflects behaviour in the complex Ginzburg-Landau equation, which serves as a good reduced model for the overstable system (Aranson & Kramer 2002;Latter & Ogilvie 2009). It also reproduces qualitatively the hydrodynamical simulations of Latter & Ogilvie (2010), yet there exist interesting discrepancies.…”
Section: Fiducial Simulationmentioning
confidence: 89%
“…Clear signatures of these features in a wavelet plot are presented in Appendix A for a simulation with a much longer domain. This configuration of dynamical elements reflects behaviour in the complex Ginzburg-Landau equation, which serves as a good reduced model for the overstable system (Aranson & Kramer 2002;Latter & Ogilvie 2009). It also reproduces qualitatively the hydrodynamical simulations of Latter & Ogilvie (2010), yet there exist interesting discrepancies.…”
Section: Fiducial Simulationmentioning
confidence: 89%
“…However, additional theoretical and observational work is needed to validate or refute this interpretation. While established linear theories can provide information about the conditions required to initiate overstability, the non-linear processes responsible for determining the final amplitude and wavelength of the patterns are still not perfectly understood, especially for situations where the mutual selfgravity of the particles cannot be ignored (Schmit and Tscharnuter 1999;Salo et al 2001;Schmidt et al 2009;Latter and Ogilvie 2009;Rein and Latter 2013). Since we cannot compare our observations with detailed theoretical predictions for the behavior and distribution of overstabilities, we will instead discuss briefly two ways these measurements could help inform future theoretical work on overstable phenomena.…”
Section: Discussionmentioning
confidence: 99%
“…i.e. the solution is a traveling wave with constant growth (or decay) rate, determined by the imaginary part of ω (Schmit and Tscharnuter (1995); Schmidt et al (2001); Latter and Ogilvie (2009)). For q > 0, the behavior is more complicated.…”
Section: Viscous Overstability In a Perturbed Ring: Axisymmetric Apprmentioning
confidence: 99%