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Characterization of Thermal-infrared Dust Emission and Refinements to the Nucleus Properties of Centaur 29P/Schwassmann–Wachmann 1
We present analyses of Spitzer observations of 29P/Schwassmann–Wachmann 1 using 16 μ m IRS “blue” peak-up (PU) and 24 and 70 μ m MIPS images obtained on UT 2003 November 23 and 24 that characterize the Centaur’s large-grain (10–100 μ m) dust coma during a time of non-outbursting “quiescent” activity...
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Published in: | The planetary science journal 2021-08, Vol.2 (4), p.126 |
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Main Authors: | , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We present analyses of Spitzer observations of 29P/Schwassmann–Wachmann 1 using 16
μ
m IRS “blue” peak-up (PU) and 24 and 70
μ
m MIPS images obtained on UT 2003 November 23 and 24 that characterize the Centaur’s large-grain (10–100
μ
m) dust coma during a time of non-outbursting “quiescent” activity. Estimates of
ϵ
f
ρ
for each band (16
μ
m (2600 ± 43 cm), 24
μ
m (5800 ± 63 cm), and 70
μ
m (1800 ± 900 cm)) follow the trend between nucleus size versus
ϵ
f
ρ
that was observed for the WISE/NEOWISE comet ensemble. A coma model was used to derive a dust production rate in the range of 50–100 kg s
−1
. For the first time, a color temperature map of SW1's coma was constructed using the 16 and 24
μ
m imaging data. With peaks at ∼140 K, this map implies that coma water-ice grains should be slowly sublimating and producing water gas in the coma. We analyzed the persistent 24
μ
m “wing” (a curved southwestern coma) feature at 352,000 km (90″) from the nucleus attributed by Stansberry et al. to nucleus rotation and instead propose that it is largely created by solar radiation pressure and gravity acting on micron-sized grains. We performed coma removal to the 16
μ
m PU image in order to refine the nucleus’ emitted thermal flux. A new application of the Near Earth Asteroid Thermal Model at five wavelengths (5.730, 7.873, 15.80, 23.68, and 71.42
μ
m) was then used to refine SW1's effective radius measurement to
R
= 32.3 ± 3.1 km and infrared beaming parameter to
η
= 1.1 ± 0.2, respectively. |
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ISSN: | 2632-3338 2632-3338 |
DOI: | 10.3847/PSJ/abfe6f |