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: 14JO80
# Created Sun Dec 22 02:09:55 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 82 observations of 82
# Arc: 12.91y
# First observation: 2010/05/18
# Last observation: 2023/04/17
# Chi-squared of fit: 54.62 DOF: 158 RMS: 0.14
# Min/Max residuals: -0.73 0.32
# Exact a, adot, b, bdot, g, gdot:
1.922998E-05 4.181793E-02 4.695936E-06 9.536016E-03 3.431719E-02 7.763036E-03
# Covariance matrix:
3.1225E-13 -9.9064E-14 4.4837E-14 -1.8087E-14 -6.3945E-14 -1.5506E-13
-9.9064E-14 3.5760E-14 -1.7602E-14 7.1445E-15 2.8265E-14 6.1141E-14
4.4837E-14 -1.7602E-14 1.1683E-13 -2.2117E-14 -1.2398E-14 -3.3859E-14
-1.8087E-14 7.1445E-15 -2.2117E-14 5.3410E-15 5.9993E-15 1.3668E-14
-6.3945E-14 2.8265E-14 -1.2398E-14 5.9993E-15 8.9726E-14 4.8986E-14
-1.5506E-13 6.1141E-14 -3.3859E-14 1.3668E-14 4.8986E-14 1.1715E-13
# lat0 lon0 xBary yBary zBary JD0
9.383445 -129.213041 -0.109148 0.163970 -0.992614 2455334.929846
# Heliocentric elements and errors
Epoch: 2455334.5000 = 2010/05/18
Mean Anomaly: 27.27134 +/- 0.003
Argument of Peri: 346.79903 +/- 0.004
Long of Asc Node: 196.45693 +/- 0.000
Inclination: 15.72466 +/- 0.000
Eccentricity: 0.28791999 +/- 0.0000
Semi-Major Axis: 39.08976840 +/- 0.0017
Time of Perihelion: 2448572.1585 +/- 0.8
Perihelion: 27.83504271 +/- 0.0015
Aphelion: 50.34449409 +/- 0.0024
Period (y) 244.4009 +/- 0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X -18.72287037 +/- 0.0002
Ecliptic Y -23.12648741 +/- 0.0002
Ecliptic Z 4.75118122 +/- 0.0000
Ecliptic XDOT 0.00227872 +/- 0.0000
Ecliptic YDOT -0.00248055 +/- 0.0000
Ecliptic ZDOT 0.00085155 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 30.13217111 +/- 0.0002
Geocenter to KBO 29.13984721 +/- 0.0003
# Hcoef: 7.68
The following table shows the complete astrometric record for 14JO80. 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 (14JO80) followed by the observatory code and reference code for the source of the astrometry.
2010 05 18.42908 15 23 24.484 -08 53 13.36 22.0G 14JO80 F51 C~2rY4 2011 01 30.60694 15 37 42.668 -09 47 31.10 22.5G 14JO80 F51 C~2rY4 2011 04 28.45094 15 35 19.473 -09 07 39.25 23.0G 14JO80 F51 C~2rY4 2011 05 29.37683 15 32 10.194 -08 53 03.82 22.5G 14JO80 F51 C~2rY4 2011 06 02.33542 15 31 46.525 -08 51 38.18 22.5G 14JO80 F51 C~2rY4 2012 04 24.52109 15 45 17.889 -09 12 16.58 22.6G 14JO80 F51 C~2rY4 2012 05 01.45354 15 44 38.276 -09 08 37.89 21.7G 14JO80 F51 C~2rY4 2013 02 14.63054 15 57 02.634 -09 47 14.02 23.1G 14JO80 F51 C~2rY4 2013 04 19.51609 15 55 15.663 -09 16 57.94 22.3G 14JO80 F51 C~2rY4 2013 05 12.44181 15 53 05.798 -09 05 28.37 22.6w 14JO80 F51 C~1vXT 2013 05 12.45506 15 53 05.724 -09 05 28.08 22.5w 14JO80 F51 C~1vXT 2013 05 12.46830 15 53 05.636 -09 05 27.69 22.7w 14JO80 F51 C~1vXT 2013 06 16.40859 15 49 36.718 -08 53 37.51 21.0G 14JO80 F51 C~2rY4 2014 02 28.59030 16 06 29.601 -09 42 43.42 22.5G 14JO80 F51 C~2rY4 2014 05 07.49237 16 02 59.607 -09 09 03.79 22.5w 14JO80 F51 C~1vXT 2014 05 07.50503 16 02 59.541 -09 09 03.41 22.2w 14JO80 F51 C~1vXT 2014 05 07.51771 16 02 59.456 -09 09 03.02 22.2w 14JO80 F51 C~1vXT 2014 05 07.53037 16 02 59.382 -09 09 02.77 22.7w 14JO80 F51 C~1vXT 2014 05 22.43543 16 01 29.082 -09 02 40.32 23.3G 14JO80 F51 C~2rY4 2014 05 23.35910 16 01 23.392 -09 02 19.18 22.5G 14JO80 F51 C~2rY4 2014 05 23.41054 16 01 23.073 -09 02 18.03 22.5G 14JO80 F51 C~2rY4 2014 05 23.42345 16 01 22.988 -09 02 17.85 22.2G 14JO80 F51 C~2rY4 2014 05 23.43629 16 01 22.916 -09 02 17.22 22.3G 14JO80 F51 C~2rY4 2014 05 23.44915 16 01 22.821 -09 02 17.24 22.4G 14JO80 F51 C~2rY4 2014 05 24.38699 16 01 17.044 -09 01 55.87 22.6w 14JO80 F51 C~1vXT 2014 05 24.44104 16 01 16.711 -09 01 54.81 22.6w 14JO80 F51 C~1vXT 2014 05 24.45367 16 01 16.629 -09 01 54.35 22.8w 14JO80 F51 C~1vXT 2014 05 28.40275 16 00 52.296 -09 00 29.60 22.7G 14JO80 F51 C~2rY4 2014 06 03.41839 16 00 15.660 -08 58 33.24 22.5w 14JO80 F51 C~1vXT 2014 06 03.43110 16 00 15.563 -08 58 32.91 22.4w 14JO80 F51 C~1vXT 2014 06 03.45646 16 00 15.401 -08 58 32.23 22.5w 14JO80 F51 C~1vXT 2014 06 24.38632 15 58 18.188 -08 54 02.98 22.6w 14JO80 F51 C~1vXT 2014 06 24.39915 15 58 18.110 -08 54 02.84 22.5w 14JO80 F51 C~1vXT 2014 06 24.41195 15 58 18.054 -08 54 02.46 22.7w 14JO80 F51 C~1vXT 2014 07 02.32171 15 57 40.677 -08 53 20.43 22.4w 14JO80 F51 C~1vXT 2014 07 02.33434 15 57 40.613 -08 53 20.26 22.6w 14JO80 F51 C~1vXT 2014 07 02.34696 15 57 40.570 -08 53 20.07 22.3w 14JO80 F51 C~1vXT 2014 07 02.35954 15 57 40.518 -08 53 20.03 22.7w 14JO80 F51 C~1vXT 2014 07 03.37606 15 57 36.072 -08 53 17.22 23.0G 14JO80 F51 C~2rY4 2014 07 04.33973 15 57 31.941 -08 53 14.84 22.2G 14JO80 F51 C~2rY4 2014 07 27.31638 15 56 20.318 -08 54 49.28 23.0G 14JO80 F51 C~2rY4 2014 07 28.27396 15 56 18.566 -08 54 59.07 23.0G 14JO80 F51 C~2rY4 2015 02 27.62766 16 15 26.373 -09 42 50.59 22.8G 14JO80 F51 C~2rY4 2015 05 21.47859 16 10 50.691 -09 03 35.94 22.7G 14JO80 F51 C~2rY4 2015 05 21.49103 16 10 50.616 -09 03 35.57 22.9G 14JO80 F51 C~2rY4 2015 05 21.51574 16 10 50.459 -09 03 34.86 22.2G 14JO80 F51 C~2rY4 2015 05 22.48015 16 10 44.563 -09 03 13.25 22.3w 14JO80 F51 C~1vXT 2015 05 22.49273 16 10 44.490 -09 03 13.10 22.3w 14JO80 F51 C~1vXT 2015 05 22.50531 16 10 44.422 -09 03 12.70 22.5w 14JO80 F51 C~1vXT 2015 06 15.34060 16 08 21.252 -08 56 20.34 22.1G 14JO80 F51 C~2rY4 2015 06 15.35314 16 08 21.180 -08 56 20.14 22.8G 14JO80 F51 C~2rY4 2015 06 15.36564 16 08 21.103 -08 56 19.97 22.6G 14JO80 F51 C~2rY4 2015 06 15.37816 16 08 21.031 -08 56 19.76 23.1G 14JO80 F51 C~2rY4 2015 06 24.42011 16 07 31.912 -08 54 54.70 22.5G 14JO80 F51 C~2rY4 2015 07 13.37630 16 06 07.538 -08 54 15.32 22.9G 14JO80 F51 C~2rY4 2015 07 14.33804 16 06 04.116 -08 54 18.44 22.7w 14JO80 F51 C~1vXT 2015 07 14.35014 16 06 04.070 -08 54 18.26 22.6w 14JO80 F51 C~1vXT 2015 07 14.37486 16 06 03.985 -08 54 18.71 22.3w 14JO80 F51 C~1vXT 2015 07 14.37496 16 06 03.969 -08 54 18.57 22.7G 14JO80 F51 C~2rY4 2015 08 09.31722 16 05 08.384 -08 58 38.29 23.7G 14JO80 F51 C~2rY4 2015 08 10.27417 16 05 07.834 -08 58 54.15 23.0G 14JO80 F51 C~2rY4 2016 03 15.66135 16 24 21.037 -09 34 22.45 21.1G 14JO80 F51 C~2rY4 2016 04 03.53824 16 23 45.901 -09 25 04.38 22.7G 14JO80 F51 C~2rY4 2016 04 03.57399 16 23 45.794 -09 25 03.31 23.2G 14JO80 F51 C~2rY4 2016 04 04.52233 16 23 42.940 -09 24 34.39 22.5G 14JO80 F51 C~2rY4 2016 05 02.53700 16 21 41.196 -09 10 46.16 22.8G 14JO80 F51 C~2rY4 2016 06 05.44858 16 18 20.040 -08 58 15.98 22.5G 14JO80 F51 C~2rY4 2016 06 05.45997 16 18 19.969 -08 58 15.88 22.4G 14JO80 F51 C~2rY4 2016 06 05.47135 16 18 19.903 -08 58 15.60 22.7G 14JO80 F51 C~2rY4 2016 06 05.48281 16 18 19.822 -08 58 15.33 22.7G 14JO80 F51 C~2rY4 2016 06 28.43663 16 16 11.497 -08 54 28.09 22.0G 14JO80 F51 C~2rY4 2017 04 04.56672 16 32 31.947 -09 22 55.93 22.6G 14JO80 F51 C~2rY4 2017 05 22.47998 16 28 42.677 -09 01 27.74 22.5G 14JO80 F51 C~2rY4 2017 06 23.34968 16 25 34.367 -08 54 06.29 22.6G 14JO80 F51 C~2rY4 2017 06 23.37755 16 25 34.179 -08 54 06.47 23.4G 14JO80 F51 C~2rY4 2017 06 23.39147 16 25 34.139 -08 54 06.30 23.3G 14JO80 F51 C~2rY4 2017 06 24.40590 16 25 28.670 -08 53 59.91 23.0G 14JO80 F51 C~2rY4 2020 07 13.30272 16 49 43.854 -08 46 52.96 22.9w 14JO80 F51 C~3ztm 2020 07 13.31660 16 49 43.791 -08 46 53.00 22.7w 14JO80 F51 C~3ztm 2020 07 13.33047 16 49 43.722 -08 46 53.13 22.8w 14JO80 F51 C~3ztm 2023 04 17.44996 17 21 33.37 -08 52 01.3 14JO80 G37 C~7X6P 2023 04 17.46967 17 21 33.32 -08 52 00.8 14JO80 G37 C~7X6P
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 -0.01 0.00 -0.06
2 0.7041 0.00 0.16 0.00 0.01
3 0.9446 0.00 0.06 0.00 -0.36
4 1.0293 0.00 0.32 0.00 0.12
5 1.0401 0.00 -0.02 0.00 -0.04
6 1.9359 0.00 -0.04 0.00 0.06
7 1.9549 0.00 -0.73 0.00 -0.55
8 2.7466 0.00 0.08 0.00 0.02
9 2.9215 0.00 -0.05 0.00 -0.14
10 2.9843 0.00 0.04 0.00 0.18
11 2.9843 0.00 0.17 0.00 0.11
12 2.9844 0.00 0.08 0.00 0.14
13 3.0800 0.00 0.20 0.00 0.05
14 3.7842 0.00 0.10 0.00 0.10
15 3.9701 0.00 -0.03 0.00 -0.01
16 3.9701 0.00 0.12 0.00 0.02
17 3.9701 0.00 -0.02 0.00 0.05
18 3.9702 0.00 0.01 0.00 -0.05
19 4.0110 0.00 -0.06 0.00 0.02
20 4.0135 0.00 -0.05 0.00 -0.00
21 4.0136 0.00 0.01 0.00 -0.02
22 4.0137 0.00 -0.05 0.00 -0.13
23 4.0137 0.00 0.08 0.00 0.21
24 4.0137 0.00 -0.13 0.00 -0.10
25 4.0163 0.00 -0.09 0.00 0.15
26 4.0165 0.00 0.01 0.00 0.01
27 4.0165 0.00 -0.03 0.00 0.19
28 4.0273 0.00 -0.18 0.00 0.04
29 4.0438 0.00 0.29 0.00 -0.08
30 4.0438 0.00 0.01 0.00 0.02
31 4.0439 0.00 -0.09 0.00 0.24
32 4.1012 0.00 0.05 0.00 -0.08
33 4.1012 0.00 -0.13 0.00 -0.03
34 4.1013 0.00 0.01 0.00 0.25
35 4.1229 0.00 -0.01 0.00 0.01
36 4.1229 0.00 -0.11 0.00 0.14
37 4.1230 0.00 0.10 0.00 0.29
38 4.1230 0.00 0.17 0.00 0.29
39 4.1258 0.00 0.07 0.00 0.15
40 4.1284 0.00 -0.08 0.00 0.26
41 4.1913 0.00 -0.01 0.00 -0.04
42 4.1940 0.00 -0.04 0.00 0.13
43 4.7808 0.00 0.02 0.00 -0.09
44 5.0077 0.00 -0.17 0.00 -0.07
45 5.0077 0.00 -0.13 0.00 0.02
46 5.0078 0.00 -0.18 0.00 0.16
47 5.0104 0.00 -0.04 0.00 0.02
48 5.0104 0.00 0.04 0.00 -0.12
49 5.0105 0.00 0.20 0.00 0.00
50 5.0757 0.00 0.07 0.00 -0.02
51 5.0758 0.00 0.08 0.00 0.03
52 5.0758 0.00 0.01 0.00 0.06
53 5.0758 0.00 0.01 0.00 0.12
54 5.1006 0.00 0.18 0.00 -0.07
55 5.1525 0.00 -0.33 0.00 -0.14
56 5.1551 0.00 0.04 0.00 -0.18
57 5.1552 0.00 0.01 0.00 0.04
58 5.1552 0.00 0.09 0.00 -0.32
59 5.1552 0.00 -0.15 0.00 -0.18
60 5.2263 0.00 -0.10 0.00 0.08
61 5.2289 0.00 0.09 0.00 -0.09
62 5.8268 0.00 -0.06 0.00 -0.01
63 5.8785 0.00 0.04 0.00 -0.10
64 5.8786 0.00 0.07 0.00 -0.11
65 5.8812 0.00 -0.05 0.00 -0.06
66 5.9579 0.00 0.09 0.00 0.03
67 6.0507 0.00 -0.05 0.00 -0.07
68 6.0507 0.00 -0.07 0.00 -0.15
69 6.0508 0.00 -0.01 0.00 -0.04
70 6.0508 0.00 -0.17 0.00 0.05
71 6.1136 0.00 0.13 0.00 -0.02
72 6.8806 0.00 0.19 0.00 0.14
73 7.0118 0.00 -0.03 0.00 0.02
74 7.0990 0.00 0.12 0.00 0.00
75 7.0991 0.00 -0.38 0.00 -0.35
76 7.0991 0.00 0.17 0.00 -0.27
77 7.1019 0.00 0.16 0.00 -0.02
78 10.1543 0.00 0.08 0.00 0.04
79 10.1544 0.00 0.08 0.00 0.07
80 10.1544 0.00 -0.01 0.00 0.01
81 12.9145 0.00 -0.12 0.00 0.06
82 12.9146 0.00 -0.00 0.00 0.04
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.
14JO80 quality flag:3 Type: 3:2E 3:2E 3:2E axisobj 38.870 38.870 38.870 ecceobj 0.285 0.285 0.285 incobj 15.744 15.744 15.744 qmin 27.386 27.380 27.413 qmax 52.444 52.420 52.396 amean 39.455 39.455 39.456 amin 38.869 38.870 38.863 amax 40.162 40.170 40.158 emean 0.293 0.293 0.292 emin 0.279 0.278 0.278 emax 0.307 0.307 0.307 imean 16.238 16.208 16.258 imin 15.580 15.524 15.551 imax 16.884 16.874 16.895 excite_mean 0.405 0.405 0.405 fracstop 1.000 1.000 1.000 cjmean 2.865 2.865 2.865 libcent 0 180.8 179.2 180.4 libamp 0 136.2 136.1 135.9 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 168.3 168.0 168.3 kozaiamp 179.9 179.9 180.0