Table 2
Summary of TPM results.
Asteroid | Model | D0 | D | Γ | ρ (rms) | ![]() |
![]() |
Γ1au | Comments |
---|---|---|---|---|---|---|---|---|---|
(km) | (km) | (SI units) | (SI units) | ||||||
(1) Ceres | Dawn SPC | 939.5 | ![]() |
![]() |
~1 | 0.2 | 2.80 | 43 | Modelled PACS data only |
Spherical model | ![]() |
![]() |
0.5 | Similar conclusion but larger error bars | |||||
(2) Pallas | ADAM | 520 | ![]() |
![]() |
~0.65 | 0.4 | 2.95 | 67 | AKARI data show a small slope in the OMR vs. λ plot |
Spherical model | – | ![]() |
![]() |
0.6 | D ~ 5% larger than ADAM → higher Γ | ||||
(3) Juno | ADAM | 248 | ![]() |
![]() |
~1 | 0.5 | 2.70 | 126 | Feature in the OMR-vs.-aspect angle plot |
Spherical model | – | ![]() |
![]() |
1.0 | Formally acceptable fit, consistent thermal properties | ||||
SAGE | – | ![]() |
![]() |
~1 | 1.27 | 147 | Formally acceptable fit, consistent thermal properties | ||
(4) Vesta | Gaskell | 522 | ![]() |
![]() |
~0.9 | 0.8 | 2.36 | 66 | Shallow χ2 minimum, slope in the OMR-vs.-wavelength plot |
Spherical model | – | ![]() |
![]() |
1.1 | Formally acceptable fit | ||||
(8) Flora | ADAM | 143 | ![]() |
![]() |
~0.4 | 0.4 | 2.20 | 90 | IRAS data: slope in the OMR vs. λ plot |
Spherical model | – | ![]() |
![]() |
0.5 | Low χ2 too, but significantly higher Γ | ||||
(10) Hygiea | ADAM | 433.6 | ![]() |
![]() |
~0.9 | 0.6 | 3.02 | 114 | IRAS data: slope in the OMR vs. λ plot. IR insensitive to albedo variegation |
Spherical model | – | ![]() |
![]() |
0.65 | Virtually the same results | ||||
(18) Melpomene | ADAM | 146 | ![]() |
![]() |
~1 | 0.3 | 2.35 | 95 | Shallow and asymmetric ![]() |
Spherical model | – | ![]() |
![]() |
0.3 | Similar fit, but only small rescaling required (2%) | ||||
(19) Fortuna | ADAM | 212 | ![]() |
![]() |
~0.50 | 0.5 | 2.45 | 78 | rms > 0.2 at 3σ level. Few data but low pole obliquity |
Spherical model | – | ![]() |
![]() |
1.1 | Lower Γ, formally acceptable fit | ||||
(20) Massalia | SAGE1 | – | ![]() |
![]() |
~0.2 | 0.45 | 2.40 | 67 | No mirror solution can be rejected. Very low roughness favoured |
Spherical model | – | 146 | 35 | 1.6 | ![]() |
||||
(21) Lutetia | Jorda | 98.15 | ![]() |
![]() |
~0.6 | 0.7 | 2.40 | 20 | 0.4 < rms < 0.9. Possible rotational phase shift (see Appendix A.4) |
Spherical model | 104 | 60 | >3 | Spherical approximation fails | |||||
(29) Amphitrite | ADAM | 205.5 | ![]() |
![]() |
~0.4 | 0.4 | 2.55 | 50 | IRAS data: strong slope in the OMR vs. λ plot |
Spherical model | ![]() |
![]() |
0.9 | Formally acceptable fit but significantly higher Γ | |||||
(52) Europa | ADAM | 313.7 | ![]() |
![]() |
~0.5 | 0.5 | 3.05 | 23 | Very shallow ![]() |
Spherical model | – | 342 | 200 | > 2 | Sphere greatly overestimates diameter and Γ | ||||
(54) Alexandra | ADAM | 143. | ![]() |
![]() |
~0.3 | 0.2 | 2.60 | 20 | Few data, Southern hemisphere not well sampled in the IR data |
Spherical model | – | ![]() |
![]() |
0.8 | Formally acceptable fit, but inconsistent Γ | ||||
(65) Cybele | ADAM | 313.3 | ![]() |
![]() |
~0.45 | 0.7 | 3.30 | 73 | Required 12% rescaling. Southern hemisphere not well sampled in the IR |
Spherical model | ![]() |
![]() |
1.1 | Formally acceptable fit, size in better agreement with ADAM | |||||
(88) Thisbe | ADAM | 220 | ![]() |
![]() |
~0.9 | 0.3 | 3.00 | 137 | IRAS data: slight slope in the OMR vs. λ plot |
Spherical model | ![]() |
![]() |
0.5 | Very low ![]() |
|||||
(93) Minerva | ADAM | 160 | ![]() |
![]() |
~0.2 | 0.5 | 3.01 | 57 | Removed MSX and IRAS 12-μm data from analysis |
Spherical model | ![]() |
![]() |
0.2 | Sphere gets lower ![]() |
|||||
(423) Diotima | ADAM | 209 | ![]() |
![]() |
~0.45 | 0.6 | 3.07 | 93 | IRAS data: slope in the OMR vs. λ plot. Southern hemisph. not sampled |
Spherical model | 205 | 150 | > 2 | Bad fit | |||||
(511) Davida | ADAM | 313 | ![]() |
![]() |
~0.5 | 0.4 | 3.35 | 87 | IRAS data: slight slope in the OMR vs. λ plot. North. Hemisph. not sampled |
Spherical model | ![]() |
![]() |
0.6 | Low ![]() |
Notes. D0 is the sphere-equivalent diameter of the ADAM or in-situ shape models. Spherical model refers to a sphere (~3000 facets) with the same spin axis. The symbols D, Γ (SI units = J m −2 s−1∕2 K−1) and ρ denote the best-fitting diameter, thermal inertia and surface roughness (rms) of the corresponding model. To normalise Γ at 1 au (Γ1au), we took the mid-point () between the shortest and longest heliocentric distance at which the data were taken. The surface roughness (rms) were not constrained at the 1σ level unless otherwise stated. For more information we refer to Appendix A and Table A.1.
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