The following information shows the result of the orbit fit based on Gary Bernstein's method. Most of the information should be self-explanatory. Take special note that while the original Bernstein software works with barycentric coordinates, we convert these results into a heliocentric coordinate system.
# Object: 601690 # Created Fri Nov 22 02:07:38 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 117 observations of 117 # Arc: 13.05y # First observation: 2010/08/05 # Last observation: 2023/08/24 # Chi-squared of fit: 101.64 DOF: 228 RMS: 0.16 # Min/Max residuals: -0.57 0.79 # Exact a, adot, b, bdot, g, gdot: 2.240247E-05 7.401303E-02 1.569585E-05 5.292518E-02 5.406516E-02 -1.328847E-02 # Covariance matrix: 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 0.0000E+00 # lat0 lon0 xBary yBary zBary JD0 -0.173913 -44.545445 0.048541 -0.003113 -1.009246 2455413.986696 # Heliocentric elements and errors Epoch: 2455414.5000 = 2010/08/06 Mean Anomaly: 350.55735 +/- 0.000 Argument of Peri: 27.13349 +/- 0.000 Long of Asc Node: 315.54781 +/- 0.000 Inclination: 35.54333 +/- 0.000 Eccentricity: 0.45228854 +/- 0.0000 Semi-Major Axis: 34.37438885 +/- 0.0000 Time of Perihelion: 2457345.3229 +/- 0.0 Perihelion: 18.82724676 +/- 0.0000 Aphelion: 49.92153095 +/- 0.0000 Period (y) 201.5397 +/- 0.00 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 13.87177311 +/- 0.0000 Ecliptic Y -13.71846661 +/- 0.0000 Ecliptic Z -0.05581749 +/- 0.0000 Ecliptic XDOT 0.00215627 +/- 0.0000 Ecliptic YDOT 0.00314376 +/- 0.0000 Ecliptic ZDOT 0.00268212 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 19.50969928 +/- 0.0000 Geocenter to KBO 18.49630223 +/- 0.0000 # Hcoef: 8.75
The following table shows the complete astrometric record for 601690. The first three columns show the date of observation. The next six columns are RA and DEC. The next column (when provided) is the observed magnitude and filter. The next column is the object name (601690) followed by the observatory code and reference code for the source of the astrometry.
2010 08 05.48593 21 11 52.861 -16 22 06.65 21.6G 601690 F51 C~2jhD 2010 08 30.42401 21 07 40.814 -16 27 38.29 21.4G 601690 F51 C~2jhD 2010 08 31.40510 21 07 31.618 -16 27 48.00 21.8G 601690 F51 C~2jhD 2010 08 31.41682 21 07 31.514 -16 27 48.20 21.6G 601690 F51 C~2jhD 2011 08 03.48309 21 25 20.678 -12 07 52.53 21.1G 601690 F51 C~2jhD 2011 08 17.37913 21 22 58.194 -12 11 42.45 21.5G 601690 F51 C~2jhD 2012 08 13.42343 21 36 28.188 -07 49 18.30 21.4w 601690 F51 C~1vWz 2012 08 13.43797 21 36 28.034 -07 49 18.66 21.5w 601690 F51 C~1vWz 2012 08 13.45249 21 36 27.888 -07 49 18.78 21.6w 601690 F51 C~1vWz 2012 08 16.40707 21 35 57.687 -07 50 15.00 21.2G 601690 F51 C~2jhD 2012 08 16.41708 21 35 57.593 -07 50 15.20 21.1G 601690 F51 C~2jhD 2012 08 16.42722 21 35 57.475 -07 50 15.49 21.4G 601690 F51 C~2jhD 2012 08 16.43759 21 35 57.377 -07 50 15.39 21.6G 601690 F51 C~2jhD 2012 08 26.35091 21 34 17.137 -07 53 40.80 21.8G 601690 F51 C~2jhD 2012 08 26.36261 21 34 17.010 -07 53 41.21 22.2G 601690 F51 C~2jhD 2012 08 26.44451 21 34 16.161 -07 53 43.11 21.5G 601690 F51 C~2jhD 2013 05 16.56257 21 57 02.941 -03 58 43.14 22.0w 601690 F51 C~1vWz 2013 05 16.56783 21 57 02.952 -03 58 42.96 22.2w 601690 F51 C~1vWz 2013 05 16.57309 21 57 02.968 -03 58 42.67 21.7w 601690 F51 C~1vWz 2013 05 16.57834 21 57 02.979 -03 58 42.25 21.7w 601690 F51 C~1vWz 2013 05 20.58423 21 57 11.138 -03 54 03.97 20.9G 601690 F51 C~2jhD 2013 05 20.58950 21 57 11.103 -03 54 03.72 21.2G 601690 F51 C~2jhD 2013 06 20.56107 21 56 29.368 -03 27 26.85 21.9w 601690 F51 C~1vWz 2013 06 20.57412 21 56 29.323 -03 27 26.25 21.8w 601690 F51 C~1vWz 2013 06 20.58716 21 56 29.250 -03 27 25.93 21.6w 601690 F51 C~1vWz 2013 06 20.60018 21 56 29.193 -03 27 25.21 21.8w 601690 F51 C~1vWz 2013 07 15.47414 21 53 53.571 -03 18 49.90 20.9G 601690 F51 C~2jhD 2013 07 15.51709 21 53 53.243 -03 18 49.64 21.5G 601690 F51 C~2jhD 2013 08 01.53510 21 51 21.560 -03 19 07.87 21.3i 601690 F51 C~1vWz 2013 08 01.54733 21 51 21.467 -03 19 07.77 21.2i 601690 F51 C~1vWz 2013 08 01.57260 21 51 21.212 -03 19 08.23 21.3r 601690 F51 C~1vWz 2013 08 12.44684 21 49 33.451 -03 21 30.97 21.7w 601690 F51 C~1vWz 2013 08 12.46189 21 49 33.296 -03 21 31.28 21.6w 601690 F51 C~1vWz 2013 08 12.47738 21 49 33.138 -03 21 31.47 21.4w 601690 F51 C~1vWz 2013 08 12.49235 21 49 32.976 -03 21 31.75 21.6w 601690 F51 C~1vWz 2013 08 17.43808 21 48 42.805 -03 23 04.13 22.2G 601690 F51 C~2jhD 2013 08 17.44953 21 48 42.704 -03 23 04.17 21.9G 601690 F51 C~2jhD 2013 08 18.44452 21 48 32.565 -03 23 24.46 21.2i 601690 F51 C~1vWz 2013 08 18.45520 21 48 32.455 -03 23 24.70 21.3i 601690 F51 C~1vWz 2013 08 18.47608 21 48 32.252 -03 23 25.26 21.4r 601690 F51 C~1vWz 2013 09 27.29208 21 42 29.370 -03 40 48.15 21.4G 601690 F51 C~2jhD 2013 09 27.30629 21 42 29.304 -03 40 47.78 22.2G 601690 F51 C~2jhD 2013 09 27.32052 21 42 29.154 -03 40 48.87 21.8G 601690 F51 C~2jhD 2013 09 27.33475 21 42 29.038 -03 40 48.97 21.8G 601690 F51 C~2jhD 2014 06 30.51697 22 08 17.734 +01 02 43.34 21.6w 601690 F51 C~1vWz 2014 06 30.53060 22 08 17.658 +01 02 43.76 21.7w 601690 F51 C~1vWz 2014 06 30.54433 22 08 17.591 +01 02 44.36 21.8w 601690 F51 C~1vWz 2014 06 30.55811 22 08 17.507 +01 02 44.73 21.8w 601690 F51 C~1vWz 2014 07 10.54294 22 07 16.417 +01 07 35.74 21.2i 601690 F51 C~1vWz 2014 07 10.55648 22 07 16.321 +01 07 36.17 21.3i 601690 F51 C~1vWz 2014 07 10.57009 22 07 16.221 +01 07 36.47 21.3i 601690 F51 C~1vWz 2014 09 04.37757 21 58 38.808 +01 00 41.64 22.0G 601690 F51 C~2jhD 2014 09 04.38917 21 58 38.696 +01 00 41.29 21.7G 601690 F51 C~2jhD 2014 09 04.40078 21 58 38.570 +01 00 40.76 20.9G 601690 F51 C~2jhD 2014 09 15.39004 21 56 55.254 +00 54 43.21 21.2i 601690 F51 C~1vWz 2014 09 15.40226 21 56 55.146 +00 54 42.76 21.1i 601690 F51 C~1vWz 2014 09 15.41455 21 56 55.035 +00 54 42.56 21.3i 601690 F51 C~1vWz 2014 09 15.42686 21 56 54.925 +00 54 41.64 21.1i 601690 F51 C~1vWz 2014 10 09.37748 21 53 55.785 +00 40 58.79 21.2G 601690 F51 C~2jhD 2014 11 19.21443 21 52 40.772 +00 28 19.29 21.9w 601690 F51 C~1vWz 2014 11 19.22635 21 52 40.813 +00 28 19.40 22.0w 601690 F51 C~1vWz 2014 11 19.23826 21 52 40.844 +00 28 19.37 21.7w 601690 F51 C~1vWz 2014 11 19.25014 21 52 40.868 +00 28 19.42 21.7w 601690 F51 C~1vWz 2015 07 18.55054 22 19 10.923 +05 38 54.93 21.5w 601690 F51 C~1vWz 2015 07 18.55118 22 19 10.914 +05 38 54.69 21.5w 601690 F51 C~1vWz 2015 07 18.56247 22 19 10.824 +05 38 55.22 21.6w 601690 F51 C~1vWz 2015 07 18.56331 22 19 10.802 +05 38 54.99 21.4w 601690 F51 C~1vWz 2015 07 18.57480 22 19 10.752 +05 38 55.21 21.5w 601690 F51 C~1vWz 2015 07 18.57545 22 19 10.728 +05 38 55.48 21.5w 601690 F51 C~1vWz 2015 07 18.58689 22 19 10.643 +05 38 55.55 21.7w 601690 F51 C~1vWz 2015 07 18.58753 22 19 10.663 +05 38 56.01 21.8w 601690 F51 C~1vWz 2015 07 19.51263 22 19 03.665 +05 39 16.82 21.5w 601690 F51 C~1vWz 2015 07 19.51328 22 19 03.656 +05 39 16.81 21.6G 601690 F51 C~2jhD 2015 07 19.52450 22 19 03.570 +05 39 17.10 21.5w 601690 F51 C~1vWz 2015 07 19.52465 22 19 03.570 +05 39 17.07 21.5G 601690 F51 C~2jhD 2015 07 19.52529 22 19 03.558 +05 39 17.12 21.4G 601690 F51 C~2jhD 2015 07 19.53672 22 19 03.479 +05 39 17.40 21.4w 601690 F51 C~1vWz 2015 07 19.54889 22 19 03.380 +05 39 17.56 21.4w 601690 F51 C~1vWz 2015 07 30.42748 22 17 33.529 +05 41 55.61 21.1i 601690 F51 C~1vWz 2015 07 30.43940 22 17 33.417 +05 41 55.99 21.1i 601690 F51 C~1vWz 2015 07 30.45125 22 17 33.305 +05 41 55.77 21.1i 601690 F51 C~1vWz 2015 07 30.46311 22 17 33.198 +05 41 56.09 21.3i 601690 F51 C~1vWz 2015 07 30.46316 22 17 33.212 +05 41 55.94 21.8G 601690 F51 C~2jhD 2015 10 02.38797 22 07 31.268 +05 15 17.81 21.6G 601690 F51 C~2jhD 2015 10 02.39994 22 07 31.181 +05 15 17.20 21.5G 601690 F51 C~2jhD 2015 10 02.41191 22 07 31.084 +05 15 16.63 21.6G 601690 F51 C~2jhD 2015 10 02.42398 22 07 30.997 +05 15 16.29 21.6G 601690 F51 C~2jhD 2015 10 03.36466 22 07 24.160 +05 14 35.82 21.8G 601690 F51 C~2jhD 2015 10 03.37676 22 07 24.065 +05 14 35.43 22.2G 601690 F51 C~2jhD 2015 10 03.38877 22 07 23.971 +05 14 34.91 21.5G 601690 F51 C~2jhD 2015 10 03.40076 22 07 23.877 +05 14 34.48 22.2G 601690 F51 C~2jhD 2015 10 27.23212 22 05 18.573 +04 58 41.56 21.5G 601690 F51 C~2jhD 2016 06 10.59294 22 34 38.246 +09 27 59.93 21.9G 601690 F51 C~2jhD 2016 07 17.44520 22 32 16.007 +10 05 39.57 21.4G 601690 F51 C~2jhD 2016 07 17.45726 22 32 15.927 +10 05 39.65 21.4G 601690 F51 C~2jhD 2016 07 17.46927 22 32 15.825 +10 05 40.02 21.3G 601690 F51 C~2jhD 2016 07 17.48123 22 32 15.755 +10 05 40.57 21.5G 601690 F51 C~2jhD 2016 08 02.40825 22 30 08.484 +10 11 41.00 21.4G 601690 F51 C~2jhD 2016 08 02.42012 22 30 08.377 +10 11 41.06 21.6G 601690 F51 C~2jhD 2016 08 02.43196 22 30 08.272 +10 11 41.15 21.5G 601690 F51 C~2jhD 2016 08 02.44382 22 30 08.161 +10 11 41.39 21.4G 601690 F51 C~2jhD 2017 08 15.50985 22 41 35.314 +14 38 54.71 21.7G 601690 F51 C~2jhD 2017 08 15.52130 22 41 35.178 +14 38 54.52 21.4G 601690 F51 C~2jhD 2017 08 15.53271 22 41 35.082 +14 38 54.60 22.0G 601690 F51 C~2jhD 2017 08 15.54417 22 41 34.980 +14 38 54.68 21.6G 601690 F51 C~2jhD 2021 10 01.287704 23 32 07.240 +30 53 08.66 21.5w 601690 F51 C~55NC 2021 10 01.300650 23 32 07.122 +30 53 07.87 21.8w 601690 F51 C~55NC 2021 10 01.332953 23 32 06.774 +30 53 06.24 21.5w 601690 F51 C~55NC 2022 10 19.264723 23 45 21.761 +34 16 14.88 21.4w 601690 F52 C~62wb 2022 10 19.289073 23 45 21.549 +34 16 13.10 21.5w 601690 F52 C~62wb 2022 10 19.301244 23 45 21.428 +34 16 12.12 21.5w 601690 F52 C~62wb 2022 10 31.213890 23 43 42.105 +34 00 48.23 21.6w 601690 F51 C~62wb 2022 10 31.238726 23 43 41.941 +34 00 46.38 21.8w 601690 F51 C~62wb 2022 10 31.251175 23 43 41.793 +34 00 45.09 21.8w 601690 F51 C~62wb 2023 08 24.493045 00 12 08.198 +37 59 46.19 21.7w 601690 F51 C~78ya 2023 08 24.504419 00 12 08.109 +37 59 46.44 21.8w 601690 F51 C~78ya 2023 08 24.515882 00 12 07.994 +37 59 47.21 21.7w 601690 F51 C~78ya
The following table shows the residuals to the orbit fit. The first coumn is the point number. The second column is the time, in years, measured from the first observation. The third and fifth columns are the regularized positions used in the orbit fit. The fourth and sixth columns are the residuals, in arc seconds, for RA and Dec respectively.
1 0.0000 0.00 -0.14 0.00 -0.09
2 0.0683 0.00 -0.04 0.00 -0.15
3 0.0710 0.00 -0.00 0.00 -0.20
4 0.0710 0.00 0.11 0.00 -0.29
5 0.9938 0.00 0.12 0.00 0.25
6 1.0319 0.00 0.06 0.00 -0.11
7 2.0231 0.00 0.04 0.00 0.03
8 2.0231 0.00 0.00 0.00 -0.06
9 2.0232 0.00 0.08 0.00 0.08
10 2.0313 0.00 -0.01 0.00 -0.10
11 2.0313 0.00 0.15 0.00 -0.10
12 2.0313 0.00 -0.04 0.00 -0.19
13 2.0314 0.00 0.11 0.00 0.11
14 2.0585 0.00 0.10 0.00 0.07
15 2.0585 0.00 -0.02 0.00 -0.09
16 2.0588 0.00 -0.32 0.00 -0.22
17 2.7791 0.00 -0.15 0.00 0.32
18 2.7791 0.00 -0.16 0.00 0.12
19 2.7792 0.00 -0.10 0.00 0.04
20 2.7792 0.00 -0.12 0.00 0.08
21 2.7901 0.00 0.58 0.00 -0.05
22 2.7902 0.00 -0.06 0.00 -0.16
23 2.8749 0.00 0.06 0.00 0.06
24 2.8750 0.00 0.25 0.00 0.21
25 2.8750 0.00 0.02 0.00 0.08
26 2.8751 0.00 0.04 0.00 0.35
27 2.9432 0.00 -0.34 0.00 -0.02
28 2.9433 0.00 0.04 0.00 -0.07
29 2.9899 0.00 -0.39 0.00 -0.04
30 2.9899 0.00 0.01 0.00 0.17
31 2.9900 0.00 -0.09 0.00 -0.07
32 3.0197 0.00 -0.07 0.00 0.04
33 3.0198 0.00 -0.07 0.00 -0.02
34 3.0198 0.00 -0.04 0.00 0.06
35 3.0199 0.00 -0.16 0.00 0.03
36 3.0334 0.00 -0.02 0.00 -0.13
37 3.0334 0.00 0.24 0.00 0.06
38 3.0362 0.00 -0.09 0.00 0.06
39 3.0362 0.00 -0.08 0.00 0.04
40 3.0362 0.00 0.12 0.00 -0.09
41 3.1453 0.00 0.23 0.00 -0.08
42 3.1453 0.00 0.79 0.00 0.66
43 3.1453 0.00 0.10 0.00 -0.06
44 3.1454 0.00 -0.09 0.00 0.21
45 3.9015 0.00 -0.01 0.00 0.08
46 3.9016 0.00 -0.03 0.00 0.01
47 3.9016 0.00 0.10 0.00 0.13
48 3.9016 0.00 -0.02 0.00 0.01
49 3.9290 0.00 0.08 0.00 -0.05
50 3.9290 0.00 0.07 0.00 0.07
51 3.9290 0.00 0.01 0.00 0.06
52 4.0818 0.00 -0.03 0.00 -0.03
53 4.0819 0.00 0.02 0.00 -0.03
54 4.0819 0.00 -0.13 0.00 -0.21
55 4.1120 0.00 -0.29 0.00 0.24
56 4.1120 0.00 -0.23 0.00 0.21
57 4.1121 0.00 -0.21 0.00 0.43
58 4.1121 0.00 -0.18 0.00 -0.07
59 4.1777 0.00 -0.09 0.00 -0.07
60 4.2895 0.00 -0.10 0.00 -0.03
61 4.2895 0.00 0.14 0.00 0.08
62 4.2895 0.00 0.23 0.00 0.05
63 4.2896 0.00 0.21 0.00 0.10
64 4.9502 0.00 0.15 0.00 -0.07
65 4.9502 0.00 0.09 0.00 -0.32
66 4.9502 0.00 0.04 0.00 -0.05
67 4.9502 0.00 -0.19 0.00 -0.30
68 4.9503 0.00 0.38 0.00 -0.35
69 4.9503 0.00 0.09 0.00 -0.10
70 4.9503 0.00 0.14 0.00 -0.29
71 4.9503 0.00 0.51 0.00 0.15
72 4.9528 0.00 0.03 0.00 -0.00
73 4.9528 0.00 -0.03 0.00 -0.03
74 4.9529 0.00 -0.01 0.00 0.02
75 4.9529 0.00 0.01 0.00 -0.02
76 4.9529 0.00 -0.09 0.00 0.02
77 4.9529 0.00 0.06 0.00 0.05
78 4.9529 0.00 -0.00 0.00 -0.06
79 4.9827 0.00 -0.16 0.00 -0.12
80 4.9828 0.00 -0.22 0.00 0.17
81 4.9828 0.00 -0.30 0.00 -0.14
82 4.9828 0.00 -0.30 0.00 0.10
83 4.9828 0.00 -0.08 0.00 -0.05
84 5.1578 0.00 0.03 0.00 0.07
85 5.1579 0.00 0.08 0.00 -0.03
86 5.1579 0.00 -0.02 0.00 -0.08
87 5.1579 0.00 0.03 0.00 0.09
88 5.1605 0.00 0.17 0.00 -0.17
89 5.1605 0.00 0.09 0.00 -0.04
90 5.1606 0.00 0.01 0.00 -0.05
91 5.1606 0.00 -0.07 0.00 0.03
92 5.2259 0.00 0.06 0.00 -0.07
93 5.8483 0.00 0.12 0.00 -0.04
94 5.9492 0.00 -0.01 0.00 0.27
95 5.9493 0.00 0.08 0.00 -0.07
96 5.9493 0.00 -0.17 0.00 -0.12
97 5.9493 0.00 0.06 0.00 0.01
98 5.9929 0.00 -0.04 0.00 0.00
99 5.9930 0.00 -0.03 0.00 -0.07
100 5.9930 0.00 0.01 0.00 -0.10
101 5.9930 0.00 -0.04 0.00 0.01
102 7.0281 0.00 0.01 0.00 0.05
103 7.0282 0.00 -0.33 0.00 -0.13
104 7.0282 0.00 -0.07 0.00 -0.04
105 7.0282 0.00 0.10 0.00 0.06
106 11.1562 0.00 -0.02 0.00 0.20
107 11.1562 0.00 0.25 0.00 0.07
108 11.1563 0.00 0.12 0.00 0.09
109 12.2047 0.00 -0.09 0.00 0.08
110 12.2048 0.00 0.15 0.00 0.03
111 12.2048 0.00 0.05 0.00 -0.09
112 12.2374 0.00 -0.13 0.00 0.02
113 12.2375 0.00 0.23 0.00 0.20
114 12.2376 0.00 -0.57 0.00 -0.07
115 13.0514 0.00 -0.04 0.00 -0.11
116 13.0514 0.00 0.18 0.00 -0.31
117 13.0514 0.00 0.02 0.00 0.01
The following table comes from a 10My integration of the orbit of the object. Three columns are shown. The first column is the result of integrating the nominal orbit. The other two columns are based on clones of the nominal orbit that are +/- 3 sigma from the nominal orbit. If all three types agree then the classificiation is deemed secure. The basis for these calculations is described in more detail in AJ, 129, 1117 (2005). Any use made of these calculations should refer to and credit this publication and the Deep Ecliptic Survey Team.
601690 quality flag:3 Type: CENTAURR CENTAURR CENTAURR axisobj 34.057 34.057 34.058 ecceobj 0.449 0.449 0.449 incobj 35.577 35.577 35.577 qmin 18.740 18.717 18.740 qmax 50.896 51.508 50.381 amean 34.316 34.495 34.201 amin 33.950 33.883 33.950 amax 34.913 35.345 34.728 emean 0.449 0.383 0.448 emin 0.443 0.244 0.443 emax 0.458 0.463 0.455 imean 37.014 39.332 37.001 imin 36.865 36.819 36.871 imax 37.125 42.961 37.125 excite_mean 0.751 0.743 0.750 fracstop 0.003 0.079 0.002 cjmean 2.393 2.386 2.395 libcent 0 -180.0 -180.0 -180.0 libamp 0 -180.0 -180.0 -180.0 libcent 1 -180.0 -180.0 -180.0 libamp 1 -180.0 -180.0 -180.0 libcent 2 -180.0 -180.0 -180.0 libamp 2 -180.0 -180.0 -180.0 libcent 3 -180.0 -180.0 -180.0 libamp 3 -180.0 -180.0 -180.0 libcent 4 -180.0 -180.0 -180.0 libamp 4 -180.0 -180.0 -180.0 kozaimean 27.9 57.8 27.7 kozaiamp 0.9 22.8 0.7