Table 4
Results obtained through modelling with the Convex Inversion Thermophysical Model.
Target name | Pole | λ (°) | β (°) | Period (h) | D (km) | pV | Γ (![]() |
![]() |
---|---|---|---|---|---|---|---|---|
(215) Oenone | 1 | ![]() |
![]() |
27.90773 ± 0.00005 | ![]() |
![]() |
![]() |
68 |
2 | ![]() |
![]() |
27.90774 ± 0.00006 | ![]() |
![]() |
![]() |
42 | |
(279) Thule | 1 | ![]() |
![]() |
23.8964 ± 0.0003 | ![]() |
![]() |
![]() |
68 |
2 | ![]() |
![]() |
23.8963 ± 0.0004 | ![]() |
![]() |
![]() |
68 | |
(357) Ninina | 1 | ![]() |
![]() |
35.9845 ± 0.0005 | ![]() |
![]() |
![]() |
59 |
2 | ![]() |
![]() |
35.9845 ± 0.0004 | ![]() |
![]() |
![]() |
34 | |
(366) Vincentina | 1 | ![]() |
![]() |
17.3484 ± 0.0002 | ![]() |
![]() |
![]() |
25 |
2 | ![]() |
![]() |
17.3484 ± 0.0003 | ![]() |
![]() |
![]() |
24 | |
(373) Melusina | 1 | ![]() |
![]() |
12.986274 ± 0.00003 | ![]() |
![]() |
![]() |
19 |
2 | ![]() |
![]() |
12.986283 ± 0.00002 | ![]() |
![]() |
![]() |
13 | |
(395) Delia | 1 | ![]() |
![]() |
19.68097 ± 0.00005 | ![]() |
![]() |
![]() |
45 |
2 | ![]() |
![]() |
19.68103 ± 0.00008 | ![]() |
![]() |
![]() |
59 | |
(429) Lotis | 1 | ![]() |
![]() |
13.58081 ± 0.00002 | ![]() |
![]() |
![]() |
21 |
2 | ![]() |
![]() |
13.58081 ± 0.00003 | ![]() |
![]() |
![]() |
21 | |
(527) Euryanthe | 1 | ![]() |
![]() |
42.8379 ± 0.0004 | ![]() |
![]() |
![]() |
3 |
2 | ![]() |
![]() |
42.8378 ± 0.0002 | ![]() |
![]() |
![]() |
28 | |
(541) Deborah | 1 | ![]() |
![]() |
29.4223 ± 0.0001 | ![]() |
![]() |
![]() |
38 |
2 | ![]() |
![]() |
29.422425 ± 0.0002 | ![]() |
![]() |
![]() |
17 | |
(672) Astarte | 1 | ![]() |
![]() |
22.57993 ± 0.00004 | ![]() |
![]() |
![]() |
55 |
2 | ![]() |
![]() |
22.57990 ± 0.00005 | ![]() |
![]() |
![]() |
59 | |
(814) Tauris | 1 | ![]() |
![]() |
36.0581 ± 0.0001 | ![]() |
![]() |
![]() |
38 |
2 | ![]() |
![]() |
36.05858 ± 0.0002 | ![]() |
![]() |
![]() |
10 | |
(859) Bouzareah | 1 | ![]() |
![]() |
24.9287 ± 0.0003 | ![]() |
![]() |
![]() |
38 |
2 | ![]() |
![]() |
24.9286 ± 0.0002 | ![]() |
![]() |
![]() |
32 | |
(907) Rhoda | 1 | ![]() |
![]() |
22.4511 ± 0.0001 | ![]() |
![]() |
![]() |
16 |
2 | ![]() |
![]() |
22.45117 ± 0.00007 | ![]() |
![]() |
![]() |
13 | |
(931) Whittemora | 1 | ![]() |
![]() |
19.17588 ± 0.00006 | ![]() |
![]() |
![]() |
45 |
2 | ![]() |
![]() |
19.17589 ± 0.00006 | ![]() |
![]() |
![]() |
21 | |
(1062) Ljuba | 1 | ![]() |
![]() |
33.7907 ± 0.0006 | ![]() |
![]() |
![]() |
42 |
2 | ![]() |
![]() |
33.7909 ± 0.0005 | ![]() |
![]() |
![]() |
55 |
Notes. The columns present parameters derived from the CITPM for the pole 1 and pole 2 solutions of each target: J2000 ecliptic pole longitude (λ) and latitude (β), sidereal rotation period, diameter (D), geometric albedo pv, thermal inertia (Γ), and Hapke’s mean surface slope . The diameter corresponds to the diameter of a sphere with a volume equivalent to that of the model. Pole solutions preferred by occultations are marked with boldface.
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