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Pluto: the next decade of discovery. Leslie Young Southwest Research Institute layoung@boulder.swri.edu. I. Decade-scale surface-atmosphere interaction. 2005: 30.9 AU, 34° sub-solar lat 2015: 32.8 AU, 49° sub-solar lat Farther at 0.2 AU/year distance, More northerly at 1.5 °/year.
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Pluto: the next decade of discovery Leslie Young Southwest Research Institute layoung@boulder.swri.edu
2005: 30.9 AU, 34° sub-solar lat 2015: 32.8 AU, 49° sub-solar lat Farther at 0.2 AU/year distance, More northerly at 1.5 °/year.
2005-2015, distance increases by 6%, insolation decreases by 12%. Simplest models have temperature decreasing by 3% (~1.2K),for the pressure nearly halving.
Sicardy et al. 2003, Nature 424 Elliot et al. 2003, Nature 424
Hansen and Paige fig 3 (high thermal inertia) perihelion 1000 year 1200 Hansen and Paige 1996, Icarus 120
Hansen and Paige fig 4 (moderate thermal inertia) perihelion 1000 year 1200
Hansen and Paige fig 7 (low thermal inertia) perihelion 1000 year 1200
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
Darkening of ices following sublimation Thermal inertia Old, frost-covered winter pole coming into sunlight
1954.8 1964.4 1975.2 1982.2 Stern et al. 1988, Icarus 75 Buie et al. 1997, Icarus 125 1992/93 Changes in lightcurve mean and amplitude can be due to volatile transport or changing viewing.
Douté et al 1999, Icarus 142 CH4 CO N2 Spectra on the surface absorption in reflected sunlight is diagnostic of the volatiles on Pluto's surface, including their grain size, mixing state, and temperature. 0.8-2.5 µm range includes N2, CH4, and CO. Shorter wavelengths include weak CH4 bands, and CH4 and tholins have absorption at 3.3 µm (See Olkin 55.02).
Hansen and Paige 1996, Icarus 120 1300 µm brightess temperature 60 µm brightness temperature N2 frost temperature 1000 year 1200
Young 2004, BAAS Occultations are the most sensitive and direct measure of changes in atmospheric pressure.