09.05: Color Photometry of the Small Saturnian Satellites: Global and Regional Variaons on Prometheus and CalypsoAuthor Block: Sarah J. Morrison 1 , P. Helfenstein 1 , P. C. Thomas 1 , J. Veverka 11 Cornell University.Presentaon Time: 10/4/2010 3:48 PM - 3:50 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: We invesgate color variaons of Prometheus and Calypso using recent high resoluon calibrated Cassini Imaging Subsystem (ISS) images with theNarrow Angle Camera (NAC) broadband filters UV3 (338 nm) , GRN (568 nm), and IR3 (930 nm) in comparison to those of Pandora, Janus, Epimetheus, and Telestoexamined previously (Morrison et al., 2009, <strong>DPS</strong> 45.04). The average UV3/IR3 rao values are as follows: Prometheus- 0.47, Pandora- 0.53, Janus- 0.57,Epimetheus- 0.58, Telesto- 0.95, and Calypso- 0.77 with formal uncertaines < 0.01 due to noise. While both Prometheus and Calypso connue the trend ofincreasing blueness toward the E-ring, Calypso differs in color from Telesto with a lower UV3/IR3 rao and a mean UV3/GRN rao value of ~0.7 compared toTelesto’s mean UV3/GRN value of ~0.9 despite both being Trojans of Tethys. Calypso’s surface also exhibits wider color and albedo variaons than on Telesto anddisnct UV3-bright units undergoing downslope transport with UV3/IR3 rao values of ~0.05 greater than the mean. Calypso's mean global CLR (611 nm) albedoat normal incidence and 35° phase is ~13% higher than Telesto's, but its albedo range is broader and overlaps Telesto's. The color differences between these twomoons may reflect varying degrees of surface burial and contaminaon from ring parcles.09.06: Mapping the Thermal Inera of IapetusAuthor Block: Edgard G. Rivera-Valenn 1 , D. G. Blackburn 1 , R. Ulrich 11 University of Arkanss.Presentaon Time: 10/4/2010 3:50 PM - 3:52 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: Nighme temperatures on a slow rotang airless body, such as Iapetus, are a crical indicator of the surface thermal inera since during this methe only acve heat source is the stored thermal energy within the surface material. During a PRIME data set for ISS in 2007, the Cassini CIRS instrument wasgiven the opportunity to record data at such a me. Surface temperatures deduced from thermal emissions are thus far the lowest recorded for Iapetus. Toaccount for the observed low temperatures, a much lower thermal inera than previously esmated is required. Surface thermal inera is expected to vary if darkmaterial overburden thickness varies on the surface of Iapetus. This arises from the finding that for a heterogeneous mixture where the surface material has alower thermal inera than the underlying layer, the surface proximity of the high thermal inera material strongly affects the observed surface thermal inera(Mellon et al., 2004, Icarus, 169, 324-340). Indeed, it has been suggested that albedo is a funcon of dark material thickness (Spencer and Denk, 2010, Science,327, 432-435) thus it can be shown that surface thermal inera is a funcon of albedo. Via the use of a heat transfer model and the recently published Iapetusbolometric Bond albedo map (Blackburn et al., 2010, Icarus, Submied), surface thermal inera can now be extrapolated for several albedo points on Iapetus.This allows for an esmate of the albedo/thermal inera relaonship and thus the development of a global thermal inera map. We will discuss the implicaonsfor surface material composion focusing on the material properes of the dark terrain.09.07: Resonant Structure and Chaoc Diffusion of the Jovian Irregular Satellites.Author Block: Julien Frouard 11 IM CCE/LAL - Paris Observatory, France.Presentaon Time: 10/4/2010 3:52 PM - 3:54 PMLocaon: Exhibit Hall<strong>Abs</strong>tract.<strong>Abs</strong>tract: The dynamical region of the Jovian irregular satellites presents an interesng web of resonances. Along with secular and mean moonresonances which shape the stability regions, we report a number of resonances involving the Great Inequality which are present in the system thanks to thewide range of the frequency of pericenter value available for the satellites in the stable regions. Using extensive numerical integraons of the satellites alongwith an indicator of chaos (MEGNO), we give global and detailled views of the retrograde and prograde regions for various dynamical models and show theapparion of the different types of resonances. The chaoc diffusion of the satellites is also studied and shows the long term stability of the Ananke and Carmefamilies, in contrast with the Pasiphae family.09.08: Towards a Comprehensive Explanaon of Iapetus' Albedo AsymmetryAuthor Block: Charles A. Peterson 11 Atmospheric & Environmental Research, Inc..Presentaon Time: 10/4/2010 3:54 PM - 3:56 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: Saturn’s satellite Iapetus, which is 6 mes brighter on its trailing hemisphere than on its leading hemisphere, has an albedo asymmetry that is uniquein our Solar System. From the me of its discovery by Cassini in 1671 unl the present, no explanaon for this extreme appearance has gained generalacceptance. An updated hypothesis, originally proposed in 1975 (Icarus 24, 499-503) and revisited in light of recent observaons, is presented with the centralassumpon that Iapetus started out with a dark surface that connues to be coated asymmetrically with bright reflecve water ice. This ice is stable for longperiods of me in the region of the outer Solar System that includes Saturn and, therefore, can be conveyed to the satellite’s surface by three disnct populaonsof exogenic impactors whose sources are all exterior to Iapetus’ orbit. Evidence for the existence of these populaons is provided by the recent discovery by theSpitzer Observatory of a very large dust ring orbing Saturn at the distance expected for ejecta from its 38 known irregular satellites including Phoebe. Althoughjust one parcular impactor populaon could account for a hemispherical albedo asymmetry, the combined effect of all three populaons acng togetherenhances and characterizes this asymmetry even further. Relevant aspects of impact dynamics involving the collision of these ice-bearing parcles with Iapetus’surface will be summarized. Proving this revised hypothesis will require the extensive modeling of ejecta modificaon and transport on the surface of Iapetus.Such an effort should contribute significantly towards not only resolving this 300-year old problem in planetary science, but also providing a beer understandingof the much less extreme hemispheric asymmetries observed for most other regular satellites in the Solar System.09.09: Heat Conducon: An Important Process for the Shape of Iapetus’s Dark Spots?Author Block: Goetz Galuba 1 , T. Denk 1 , G. Neukum 11 Freie Universität Berlin, Planetology & Remote Sensing, Germany.Presentaon Time: 10/4/2010 3:56 PM - 3:58 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: The saturnian moon Iapetus is famous for its global black-and-white dichotomy. While its leading side (Cassini Regio) is covered by very darkmaterial, the poles and trailing side are relavely bright. However, craters and troughs with dark floors are located within the bright area, especially at lowlatudes. The boundaries of these smaller-scaled dark areas are very sharp. Even within the best-resolved images from the Cassini imaging experiment (ISS), thetypical length of a drop-off in albedo is below the resoluon limit.
Thermal segregaon, driven by a feedback process, has been proposed as the cause for the global dichotomy (Spencer and Denk 2010; Denk et al. 2010). Inaddion, for local features like craters and troughs, we explain the local darkening by an increased amount of insolaon caused by the concave curvature of thesefeatures. We studied the insolaon geometry using varying reflectance models. A model of linear interpolaon between lunar and Lambert-like scaeringreproduces the dark paerns relavely well. However, the increased insolaon by itself neither explains the abundance of darkened terrain, nor the temporalbehavior of darkening of fresh bright craters from the outside inward within the Cassini Regio area.A comparison of me scales and spaal scales shows that heat conducon might act as a major contributor to the growth of local dark areas within the brightterrain, despite its short range. Due to the repeve nature of the processes needed for the growth of darkened terrain, the significant processes should not be aslong-ranged as saltaon of ice or CO2.We gratefully acknowledge funding of this work by the German Space Agency (DLR) Bonn through grant no. 50 OH 0305.09.10: Segregaon Of Ice And Dark Materials On The Saturnian SatellitesAuthor Block: Gary B. Hansen 11 Univ. of Washington.Presentaon Time: 10/4/2010 3:58 PM - 4:00 PMLocaon: Exhibit Hall<strong>Abs</strong>tract.<strong>Abs</strong>tract: The water ice on the Galilean satellites is segregated spaally from the darker non-ice materials by a well known thermal process thatdepends on the temperature of the different materials (for the Galilean satellites, pure water snow has temperatures under full sun of 120-130 K while thesegregated dark materials reach 160 K. The Saturnian satellites with the darkest materials (1-3 % albedo), i.e., Iapetus, Phoebe, and Hyperion, also have beenshown to have spaally segregated dark material which reaches ~130 K. But the bright material need not be pure water ice, and in fact is mostly slightly dirty icewith an albedo of 30-50%. This is evident from the overall albedo of extended bright areas such as on the trailing hemisphere of Iapetus, and from the lack ofweak bands of water ice near 1.04 and 1.25 microns in its near-infrared spectrum. These bands are the first to disappear when you mix water ice with darksubstances. We will run radiave transfer models to show how much dark material needs to be mixed into the ice to remove these bands (we expect <<0.1%mass rao) and calculate the modified area of icy material in models we have done for Phoebe using Cassini-VIMS data, where we assumed pure water snow asthe icy component. Such modeling, even for these segregated terrains, is complicated because the amount of dark material in the ice can vary a lot and sllachieve segregaon. We will esmate the maximum dark material mixing rao beyond which the albedo is to low for effecve segregaon, while nearly pure icesnow can also exist (isolated locaons on Phoebe do show the short-wave ice bands, and are therefore purer ice than typical). Models of the areal fracon of icymaterial may have large uncertaines because of this effect.09.11: 3-D General Circulaon Model Simulaons of an N 2 Microbar AtmosphereAuthor Block: Charles Miller 1 , N. J. Chanover 1 , J. R. Murphy 11 New Mexico State University.Presentaon Time: 10/4/2010 4:00 PM - 4:02 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: Both Triton and Pluto are known to possess thin N 2 atmospheres with surface pressures in the range of 10 microbars in vapor pressure equilibriumwith N 2 surface frosts. We present inial results of a 3-D dynamical model of a microbar N 2 atmosphere using an adaptaon of the Ames Mars GeneralCirculaon Model (GCM) version 2.0. The Ames GCM incorporates several physical processes crical to modeling the atmospheres of Triton and Pluto, includingcondensaon and sublimaon of the main atmospheric constuent gas as well as subsurface storage and release of heat. We altered the Ames GCM to simulatecondions found on Triton. These alteraons included changing the size, rotaon rate, orbital inclinaon, surface gravity, and distance to the Sun of the parentbody, which produced the appropriate insolaon at the top of the atmosphere. We also changed the gas properes from those of a CO 2 atmosphere in the originalAmes GCM to those of an N 2 atmosphere, including values for latent heat, specific heat, and the proper vapor pressure-temperature relaonship for N 2 frosts. Wechose albedo and emissivity values for the surface substrate and N 2 frost from published values based on global thermal simulaons of Triton. We ransimulaons covering 70 Triton days (or 411 Earth days) to allow for the establishment of equilibrium between the surface pressure and the temperature of thesurface frosts. We examine the role of albedo and emissivity on the paern of surface frosts aer inial spin-up of the GCM. We also present results ofsimulaons that employ a Newtonian cooling algorithm based on published temperature-pressure profiles from stellar occultaons by Triton. This study wasfunded by a NASA Earth and Space Science Fellowship through grant number NNX09AQ96H.09.12: The Effect of the Satellite/Planet Mass Rao on the Co-orbital Congenital Formaon ModelAuthor Block: André Izidoro 1 , O. C. Winter 1 , M. Tsuchida 11 UNESP, Brazil.Presentaon Time: 10/4/2010 4:02 PM - 4:04 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: There are several known bodies in the solar system that share the same mean orbit. This kind of moon is denominated co-orbital and ischaracterized according to the center of libraon of the cric argument θ=λ- λ', where λ and λ' represents the mean longitude of the minor and major bodiesrespecvely. When the body librates around L4 or L5 the orbit is said tadpole, when oscillates around θ=180, involving L3, L4 e L5 the orbit is called horseshoe,and when the oscillaon occurs close to zero, the body is a quasi-satellite. In this work we studied the effects of different satellite/planet mass raos anddifferent satellite-planet distance during the formaon of co-orbital objects through of the congenital formaon model. The dynamic system studied consists of acentral body, a secondary body and a cloud of planetesimals randomly distributed in a sector around L4 or L5. The sector is delimited by an arc of 70°, centered onthe Lagrangian point, and the extreme orbital radii of the largest tadpole orbit. The preliminary results show that for satellite-planet mass rao equals to 1e-3occurs the formaon of bodies with relave mass larger than 0.6e-6 of the central body's mass, which is a the limit found by Beaugé et al. (2007). However, inthis case, we used a radial distance much smaller than Beagué et al. (2007). This shows that the liming mass of larger body created is not dependent only onthe satellite-planet mass rao.09.13: The Strongest Opposion Surges: Products of Ejecta Exchange?Author Block: Anne J. Verbiscer 1 , T. M. Fisher 1 , R. G. French 21 University of Virginia, 2 Wellesley College.Presentaon Time: 10/4/2010 4:04 PM - 4:06 PMLocaon: Exhibit Hall<strong>Abs</strong>tract: Recent evidence suggests that strong opposion surges are not necessarily correlated with albedo. We have measured the opposion surge of thebinary Trans-Neptunian Object (TNO) 2000 YW134 and find that its R-band reflectance increases by ~2 magnitudes/degree between phase angles of 0.3 and 0.05degrees. Another binary TNO, 1997 CS29, exhibits a similarly large opposion surge [1]. Spitzer Space Telescope and Herschel Space Observatory observaons
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References:[1] NRC, Europa Science
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atmospheric constuents. For computa
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most asteroids, at least in an exte