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: 523787 # Created Fri Nov 22 02:07:22 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 93 observations of 93 # Arc: 10.20y # First observation: 2014/01/26 # Last observation: 2024/04/09 # Chi-squared of fit: 52.37 DOF: 180 RMS: 0.13 # Min/Max residuals: -0.52 0.54 # Exact a, adot, b, bdot, g, gdot: 2.253254E-05 5.843011E-02 1.014474E-05 2.625519E-02 4.205310E-02 1.957945E-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 -19.096962 174.575657 0.732773 -0.213885 -0.618111 2456684.048938 # Heliocentric elements and errors Epoch: 2456684.5000 = 2014/01/27 Mean Anomaly: 8.46358 +/- 0.000 Argument of Peri: 277.80763 +/- 0.000 Long of Asc Node: 209.29180 +/- 0.000 Inclination: 29.45758 +/- 0.000 Eccentricity: 0.61389009 +/- 0.0000 Semi-Major Axis: 57.10216344 +/- 0.0000 Time of Perihelion: 2452979.1529 +/- 0.0 Perihelion: 22.04771109 +/- 0.0000 Aphelion: 92.15661579 +/- 0.0000 Period (y) 431.5062 +/- 0.00 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X -22.95330099 +/- 0.0000 Ecliptic Y 2.91720296 +/- 0.0000 Ecliptic Z -7.77966042 +/- 0.0000 Ecliptic XDOT -0.00212146 +/- 0.0000 Ecliptic YDOT -0.00362292 +/- 0.0000 Ecliptic ZDOT 0.00119836 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 24.41064008 +/- 0.0000 Geocenter to KBO 23.77930992 +/- 0.0000 # Hcoef: 7.57
The following table shows the complete astrometric record for 523787. 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 (523787) followed by the observatory code and reference code for the source of the astrometry.
2014 01 26.54816 11 09 10.695 -15 20 43.51 21.9G 523787 F51 C~2kRY 2014 02 13.55456 11 07 27.250 -15 14 57.94 21.2G 523787 F51 C~2kRY 2014 02 21.48797 11 06 34.138 -15 10 14.68 21.4i 523787 F51 C~2dZl 2014 02 21.50021 11 06 34.079 -15 10 14.60 21.2i 523787 F51 C~2dZl 2014 02 21.51244 11 06 33.974 -15 10 14.39 21.2i 523787 F51 C~2dZl 2014 12 18.60666 11 25 11.215 -15 07 10.21 22.1G 523787 F51 C~2kRZ 2015 02 23.46403 11 21 30.382 -15 08 23.67 21.7w 523787 F51 C~1vYK 2015 02 23.47553 11 21 30.301 -15 08 23.18 21.5w 523787 F51 C~1vYK 2015 02 23.48703 11 21 30.231 -15 08 22.75 21.6w 523787 F51 C~1vYK 2015 02 23.49853 11 21 30.150 -15 08 22.28 21.5w 523787 F51 C~1vYK 2015 04 10.34692 11 16 25.553 -14 23 03.58 21.8w 523787 F51 C~1vYK 2015 04 10.35754 11 16 25.498 -14 23 02.79 21.6w 523787 F51 C~1vYK 2015 04 10.36817 11 16 25.431 -14 23 02.05 21.8w 523787 F51 C~1vYK 2015 04 10.37882 11 16 25.384 -14 23 01.23 22.2w 523787 F51 C~1vYK 2015 04 16.30100 11 15 54.074 -14 15 56.72 21.6w 523787 F51 C~1vYK 2015 04 16.31185 11 15 54.017 -14 15 55.98 21.5w 523787 F51 C~1vYK 2015 04 16.32270 11 15 53.962 -14 15 54.97 21.7w 523787 F51 C~1vYK 2015 04 16.33358 11 15 53.911 -14 15 54.35 21.6w 523787 F51 C~1vYK 2015 04 18.30133 11 15 44.287 -14 13 32.63 21.7w 523787 F51 C~1vYK 2015 04 18.31196 11 15 44.232 -14 13 32.06 21.8w 523787 F51 C~1vYK 2015 04 18.32260 11 15 44.174 -14 13 31.43 22.0w 523787 F51 C~1vYK 2015 04 18.33321 11 15 44.124 -14 13 30.39 21.7w 523787 F51 C~1vYK 2015 05 17.26828 11 14 16.977 -13 40 26.95 21.7w 523787 F51 C~1vYK 2015 05 17.27989 11 14 16.948 -13 40 26.37 21.7w 523787 F51 C~1vYK 2015 05 17.29148 11 14 16.929 -13 40 25.51 21.7w 523787 F51 C~1vYK 2015 05 17.30310 11 14 16.913 -13 40 24.88 21.7w 523787 F51 C~1vYK 2015 05 18.29168 11 14 15.951 -13 39 23.51 21.7G 523787 F51 C~2kRZ 2016 03 01.43869 11 35 19.682 -14 59 49.27 21.1G 523787 F51 C~2kRZ 2016 03 01.44941 11 35 19.604 -14 59 48.60 21.6G 523787 F51 C~2kRZ 2016 03 01.45979 11 35 19.530 -14 59 48.17 21.1G 523787 F51 C~2kRZ 2016 03 01.47020 11 35 19.471 -14 59 47.81 21.2G 523787 F51 C~2kRZ 2016 03 15.38876 11 33 44.252 -14 47 59.27 21.0G 523787 F51 C~2kRZ 2016 04 03.34432 11 31 38.273 -14 28 14.78 21.7G 523787 F51 C~2kRZ 2016 04 03.35557 11 31 38.202 -14 28 13.98 21.7G 523787 F51 C~2kRZ 2016 04 03.36683 11 31 38.132 -14 28 13.33 21.8G 523787 F51 C~2kRZ 2016 04 03.37808 11 31 38.058 -14 28 12.42 21.6G 523787 F51 C~2kRZ 2016 04 29.30339 11 29 24.298 -13 58 28.39 21.3G 523787 F51 C~2kRZ 2016 04 29.31502 11 29 24.246 -13 58 27.53 21.8G 523787 F51 C~2kRZ 2016 04 29.32665 11 29 24.205 -13 58 26.72 21.2G 523787 F51 C~2kRZ 2016 04 29.33826 11 29 24.145 -13 58 26.11 21.0G 523787 F51 C~2kRZ 2016 05 21.32754 11 28 30.485 -13 35 05.23 22.0G 523787 F51 C~2kRZ 2017 01 30.54419 11 52 00.448 -15 06 22.32 22.2G 523787 F51 C~2kRZ 2017 01 30.55581 11 52 00.394 -15 06 22.30 21.7G 523787 F51 C~2kRZ 2017 01 30.56743 11 52 00.350 -15 06 22.19 22.1G 523787 F51 C~2kRZ 2017 01 30.57906 11 52 00.305 -15 06 22.04 21.8G 523787 F51 C~2kRZ 2017 02 17.51763 11 50 33.651 -15 00 30.76 22.4G 523787 F51 C~2kRZ 2017 02 17.53010 11 50 33.580 -15 00 30.24 22.0G 523787 F51 C~2kRZ 2017 02 17.54259 11 50 33.502 -15 00 29.96 21.7G 523787 F51 C~2kRZ 2017 02 17.55506 11 50 33.436 -15 00 29.68 21.4G 523787 F51 C~2kRZ 2017 03 21.39117 11 47 07.774 -14 36 34.49 21.9G 523787 F51 C~2kRZ 2017 03 21.40236 11 47 07.693 -14 36 33.91 21.9G 523787 F51 C~2kRZ 2017 03 21.41358 11 47 07.626 -14 36 33.28 21.7G 523787 F51 C~2kRZ 2017 03 21.42479 11 47 07.548 -14 36 32.62 21.6G 523787 F51 C~2kRZ 2017 03 31.36541 11 46 01.461 -14 26 29.68 21.6G 523787 F51 C~2kRZ 2017 03 31.37728 11 46 01.381 -14 26 28.99 21.6G 523787 F51 C~2kRZ 2017 03 31.38916 11 46 01.301 -14 26 28.24 21.5G 523787 F51 C~2kRZ 2017 03 31.40104 11 46 01.227 -14 26 27.32 21.9G 523787 F51 C~2kRZ 2017 04 25.32379 11 43 39.159 -13 59 03.84 22.1G 523787 F51 C~2kRZ 2017 04 25.33424 11 43 39.125 -13 59 03.12 22.1G 523787 F51 C~2kRZ 2017 04 25.34470 11 43 39.079 -13 59 02.44 22.8G 523787 F51 C~2kRZ 2017 04 25.35520 11 43 39.017 -13 59 01.67 21.9G 523787 F51 C~2kRZ 2017 12 31.62545 12 05 54.482 -14 52 19.09 22.3G 523787 F51 C~2kRZ 2018 02 11.55147 12 04 25.543 -14 53 28.72 22.1G 523787 F51 C~2kRZ 2018 02 11.56330 12 04 25.482 -14 53 28.46 21.8G 523787 F51 C~2kRZ 2018 02 11.57515 12 04 25.431 -14 53 28.23 22.0G 523787 F51 C~2kRZ 2018 02 11.58698 12 04 25.375 -14 53 27.95 22.2G 523787 F51 C~2kRZ 2018 03 22.41861 12 00 30.753 -14 27 25.81 22.3G 523787 F51 C~2kRZ 2018 04 10.17619 11 58 29.527 -14 08 38.19 21.7R 523787 G37 C~2dZl 2018 04 10.22848 11 58 29.179 -14 08 34.63 523787 G37 C~2dZl 2019 04 05.37240 12 11 55.267 -14 03 48.11 21.8w 523787 F51 C~343d 2019 04 05.38491 12 11 55.180 -14 03 47.32 21.7w 523787 F51 C~343d 2019 04 05.40993 12 11 55.009 -14 03 45.35 21.9w 523787 F51 C~343d 2021 02 11.542583 12 40 53.373 -14 12 20.84 22.0w 523787 F51 C~4fLB 2021 02 11.553587 12 40 53.343 -14 12 20.80 22.1w 523787 F51 C~4fLB 2021 02 11.575626 12 40 53.258 -14 12 19.93 22.3w 523787 F51 C~4fLB 2021 04 03.364458 12 36 14.234 -13 39 11.71 21.7w 523787 F51 C~4mlI 2021 04 03.377515 12 36 14.141 -13 39 11.30 21.7w 523787 F51 C~4mlI 2021 04 03.390551 12 36 14.050 -13 39 10.44 21.6w 523787 F51 C~4mlI 2021 04 03.403617 12 36 13.967 -13 39 09.62 21.7w 523787 F51 C~4mlI 2021 05 09.334407 12 32 51.832 -13 05 32.13 21.8w 523787 F51 C~4pOP 2021 05 09.347441 12 32 51.786 -13 05 31.39 21.9w 523787 F51 C~4pOP 2021 05 09.360485 12 32 51.716 -13 05 30.67 21.9w 523787 F51 C~4pOP 2021 05 09.373559 12 32 51.659 -13 05 29.99 21.8w 523787 F51 C~4pOP 2022 03 25.406061 12 48 28.728 -13 31 33.70 21.9w 523787 F52 C~5XLL 2022 03 25.416546 12 48 28.668 -13 31 33.14 21.9w 523787 F52 C~5XLL 2022 03 25.426855 12 48 28.592 -13 31 32.56 21.9w 523787 F52 C~5XLL 2022 03 25.437171 12 48 28.541 -13 31 31.91 21.7w 523787 F52 C~5XLL 2023 04 17.390988 12 56 55.120 -12 55 48.14 21.7w 523787 F52 C~6mnC 2023 04 17.403170 12 56 55.028 -12 55 47.12 21.8w 523787 F52 C~6mnC 2023 04 17.415369 12 56 54.969 -12 55 46.80 21.8w 523787 F52 C~6mnC 2024 04 09.401803 13 07 58.409 -12 44 53.88 21.8w 523787 F52 C~7zY6 2024 04 09.414293 13 07 58.336 -12 44 53.30 21.8w 523787 F52 C~7zY6 2024 04 09.439334 13 07 58.190 -12 44 51.90 21.9w 523787 F52 C~7zY6
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 -0.13 0.00 -0.00
2 0.0493 0.00 -0.25 0.00 0.43
3 0.0710 0.00 -0.28 0.00 0.19
4 0.0711 0.00 0.13 0.00 -0.23
5 0.0711 0.00 -0.15 0.00 -0.52
6 0.8927 0.00 0.01 0.00 0.06
7 1.0757 0.00 0.02 0.00 0.08
8 1.0758 0.00 -0.02 0.00 0.11
9 1.0758 0.00 0.11 0.00 0.08
10 1.0758 0.00 0.07 0.00 0.09
11 1.2014 0.00 0.05 0.00 0.05
12 1.2014 0.00 0.13 0.00 0.09
13 1.2014 0.00 0.04 0.00 0.07
14 1.2015 0.00 0.25 0.00 0.13
15 1.2177 0.00 0.14 0.00 -0.01
16 1.2177 0.00 0.12 0.00 -0.05
17 1.2177 0.00 0.14 0.00 0.18
18 1.2178 0.00 0.21 0.00 0.02
19 1.2231 0.00 0.22 0.00 0.11
20 1.2232 0.00 0.18 0.00 -0.08
21 1.2232 0.00 0.10 0.00 -0.22
22 1.2232 0.00 0.14 0.00 0.06
23 1.3025 0.00 0.10 0.00 -0.02
24 1.3025 0.00 -0.12 0.00 -0.16
25 1.3025 0.00 -0.20 0.00 -0.03
26 1.3025 0.00 -0.23 0.00 -0.12
27 1.3053 0.00 -0.12 0.00 0.06
28 2.0942 0.00 -0.09 0.00 -0.04
29 2.0942 0.00 -0.16 0.00 0.16
30 2.0942 0.00 -0.21 0.00 0.13
31 2.0942 0.00 -0.03 0.00 0.02
32 2.1323 0.00 -0.09 0.00 -0.17
33 2.1842 0.00 -0.06 0.00 -0.02
34 2.1843 0.00 -0.05 0.00 0.02
35 2.1843 0.00 -0.02 0.00 -0.08
36 2.1843 0.00 -0.05 0.00 0.08
37 2.2553 0.00 0.04 0.00 -0.04
38 2.2554 0.00 -0.05 0.00 0.03
39 2.2554 0.00 0.04 0.00 0.05
40 2.2554 0.00 -0.17 0.00 -0.14
41 2.3156 0.00 -0.06 0.00 -0.28
42 3.0116 0.00 0.14 0.00 0.04
43 3.0117 0.00 0.03 0.00 -0.05
44 3.0117 0.00 0.07 0.00 -0.05
45 3.0117 0.00 0.10 0.00 -0.00
46 3.0608 0.00 0.05 0.00 -0.14
47 3.0609 0.00 0.08 0.00 0.01
48 3.0609 0.00 -0.01 0.00 -0.08
49 3.0609 0.00 0.09 0.00 -0.18
50 3.1481 0.00 -0.08 0.00 0.05
51 3.1481 0.00 -0.14 0.00 -0.01
52 3.1482 0.00 0.02 0.00 -0.03
53 3.1482 0.00 0.01 0.00 -0.02
54 3.1754 0.00 -0.08 0.00 0.02
55 3.1754 0.00 -0.10 0.00 -0.04
56 3.1755 0.00 -0.12 0.00 -0.04
57 3.1755 0.00 -0.05 0.00 0.13
58 3.2437 0.00 -0.17 0.00 -0.03
59 3.2438 0.00 0.08 0.00 -0.01
60 3.2438 0.00 0.14 0.00 -0.02
61 3.2438 0.00 -0.03 0.00 0.05
62 3.9290 0.00 -0.01 0.00 -0.16
63 4.0438 0.00 0.04 0.00 0.04
64 4.0438 0.00 -0.01 0.00 0.04
65 4.0439 0.00 0.09 0.00 0.02
66 4.0439 0.00 0.11 0.00 0.04
67 4.1502 0.00 -0.09 0.00 0.02
68 4.2016 0.00 -0.03 0.00 -0.01
69 4.2017 0.00 -0.38 0.00 0.25
70 5.1877 0.00 -0.01 0.00 0.01
71 5.1878 0.00 -0.09 0.00 0.06
72 5.1878 0.00 -0.21 0.00 0.54
73 7.0445 0.00 0.07 0.00 0.03
74 7.0445 0.00 0.23 0.00 -0.14
75 7.0446 0.00 0.18 0.00 0.31
76 7.1836 0.00 0.13 0.00 0.07
77 7.1837 0.00 0.00 0.00 -0.23
78 7.1837 0.00 -0.09 0.00 -0.07
79 7.1837 0.00 -0.07 0.00 0.05
80 7.2821 0.00 -0.02 0.00 -0.04
81 7.2821 0.00 0.18 0.00 -0.01
82 7.2822 0.00 0.02 0.00 -0.00
83 7.2822 0.00 0.05 0.00 -0.04
84 8.1584 0.00 -0.02 0.00 -0.13
85 8.1584 0.00 0.07 0.00 -0.08
86 8.1585 0.00 -0.09 0.00 0.01
87 8.1585 0.00 0.12 0.00 0.16
88 9.2207 0.00 0.07 0.00 -0.28
89 9.2207 0.00 -0.19 0.00 0.10
90 9.2207 0.00 0.05 0.00 -0.22
91 10.2008 0.00 -0.13 0.00 0.04
92 10.2009 0.00 -0.06 0.00 0.00
93 10.2009 0.00 0.09 0.00 0.17
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.
523787 quality flag:3 Type: CENTAURR CENTAURR CENTAURR axisobj 56.779 56.778 56.779 ecceobj 0.612 0.612 0.612 incobj 29.447 29.447 29.447 qmin 21.684 21.764 21.587 qmax 92.262 92.427 91.888 amean 56.084 55.585 55.002 amin 54.474 53.065 53.449 amax 57.162 57.374 56.981 emean 0.606 0.600 0.599 emin 0.593 0.582 0.587 emax 0.614 0.613 0.613 imean 29.953 30.338 30.106 imin 29.766 29.778 29.777 imax 30.353 30.918 30.424 excite_mean 0.785 0.784 0.781 fracstop 0.017 0.025 0.020 cjmean 2.429 2.428 2.430 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 282.4 285.6 283.1 kozaiamp 4.5 7.2 6.0