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: 16FL59 # Created Wed Dec 25 02:10:36 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 98 observations of 98 # Arc: 10.92y # First observation: 2011/03/31 # Last observation: 2022/03/02 # Chi-squared of fit: 229.01 DOF: 190 RMS: 0.27 # Min/Max residuals: -0.77 1.04 # Exact a, adot, b, bdot, g, gdot: 1.489319E-05 2.396018E-02 -4.443450E-07 -4.994908E-04 2.436919E-02 -1.709083E-04 # Covariance matrix: 2.2720E-13 -7.9287E-14 -2.1404E-15 1.1730E-15 -2.9372E-14 -2.5741E-13 -7.9287E-14 3.4275E-14 1.1800E-15 -5.9194E-16 9.9911E-15 1.2995E-13 -2.1404E-15 1.1800E-15 1.0742E-13 -1.9697E-14 -8.0541E-16 5.1476E-15 1.1730E-15 -5.9194E-16 -1.9697E-14 4.2340E-15 -1.8955E-16 -2.5598E-15 -2.9372E-14 9.9911E-15 -8.0541E-16 -1.8955E-16 6.0427E-14 4.1055E-14 -2.5741E-13 1.2995E-13 5.1476E-15 -2.5598E-15 4.1055E-14 5.6197E-13 # lat0 lon0 xBary yBary zBary JD0 -6.993069 177.205134 -0.223456 -0.119060 -0.970408 2455651.857746 # Heliocentric elements and errors Epoch: 2455652.5000 = 2011/04/01 Mean Anomaly: 357.34172 +/- 0.072 Argument of Peri: 263.25440 +/- 0.075 Long of Asc Node: 277.12275 +/- 0.001 Inclination: 6.92757 +/- 0.000 Eccentricity: 0.02457152 +/- 0.0000 Semi-Major Axis: 43.05939917 +/- 0.0018 Time of Perihelion: 2456414.5779 +/- 21.5 Perihelion: 42.00136412 +/- 0.0022 Aphelion: 44.11743422 +/- 0.0022 Period (y) 282.5597 +/- 0.02 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X -41.66509088 +/- 0.0004 Ecliptic Y 1.80971749 +/- 0.0000 Ecliptic Z -4.99603849 +/- 0.0001 Ecliptic XDOT -0.00010701 +/- 0.0000 Ecliptic YDOT -0.00268397 +/- 0.0000 Ecliptic ZDOT -0.00005334 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 42.00256348 +/- 0.0004 Geocenter to KBO 41.03547115 +/- 0.0004 # Hcoef: 6.89
The following table shows the complete astrometric record for 16FL59. 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 (16FL59) followed by the observatory code and reference code for the source of the astrometry.
2011 03 31.35698 11 38 36.100 -05 18 16.73 23.0G 16FL59 F51 C~36rx 2011 03 31.37250 11 38 36.023 -05 18 15.98 22.7G 16FL59 F51 C~36rx 2011 03 31.38906 11 38 35.959 -05 18 15.65 23.0G 16FL59 F51 C~36rx 2011 03 31.40462 11 38 35.900 -05 18 15.29 22.8G 16FL59 F51 C~36rx 2012 03 02.45820 11 45 42.356 -06 05 45.56 22.4G 16FL59 F51 C~36rx 2012 03 20.36745 11 44 22.094 -05 57 38.98 22.9G 16FL59 F51 C~36rx 2013 03 06.44750 11 50 27.425 -06 38 16.29 22.3G 16FL59 F51 C~36rx 2013 04 05.33533 11 48 14.403 -06 23 58.65 23.4G 16FL59 F51 C~36rx 2013 06 30.28585 11 46 00.431 -05 57 33.58 23.3G 16FL59 F51 C~36rx 2014 02 26.50719 11 56 04.982 -07 15 24.48 22.0G 16FL59 F51 C~36rx 2014 03 06.45205 11 55 31.038 -07 12 18.11 22.6G 16FL59 F51 C~36rx 2014 03 06.46397 11 55 30.978 -07 12 18.09 23.2G 16FL59 F51 C~36rx 2014 03 24.40493 11 54 10.426 -07 04 06.41 23.6G 16FL59 F51 C~36rx 2014 03 24.44184 11 54 10.290 -07 04 05.33 22.9G 16FL59 F51 C~36rx 2014 04 28.30882 11 51 49.665 -06 46 49.38 23.2G 16FL59 F51 C~36rx 2014 04 28.32111 11 51 49.608 -06 46 48.74 22.6G 16FL59 F51 C~36rx 2014 04 28.33339 11 51 49.580 -06 46 48.73 23.0G 16FL59 F51 C~36rx 2014 04 28.34568 11 51 49.533 -06 46 48.05 23.3G 16FL59 F51 C~36rx 2014 05 04.33102 11 51 31.097 -06 44 06.67 22.9G 16FL59 F51 C~36rx 2014 05 24.29860 11 50 47.823 -06 36 32.23 22.8G 16FL59 F51 C~36rx 2014 05 24.31185 11 50 47.786 -06 36 32.06 22.4G 16FL59 F51 C~36rx 2015 01 23.49538 12 02 57.132 -07 56 18.31 23.1G 16FL59 F51 C~36rx 2015 01 23.50684 12 02 57.117 -07 56 18.34 22.8G 16FL59 F51 C~36rx 2015 01 23.51828 12 02 57.114 -07 56 17.98 22.8G 16FL59 F51 C~36rx 2015 01 23.54987 12 02 57.026 -07 56 18.12 23.6G 16FL59 F51 C~36rx 2015 01 23.56526 12 02 56.981 -07 56 17.78 23.0G 16FL59 F51 C~36rx 2015 01 25.54224 12 02 52.877 -07 56 11.17 23.3G 16FL59 F51 C~36rx 2015 04 13.05663 11 57 49.76 -07 28 13.8 23.5V 16FL59 W84 C~36rx 2015 04 13.15360 11 57 49.35 -07 28 10.8 16FL59 W84 C~36rx 2015 04 13.22315 11 57 49.07 -07 28 08.7 16FL59 W84 C~36rx 2015 04 13.27117 11 57 48.86 -07 28 07.2 16FL59 W84 C~36rx 2015 04 15.129132 11 57 41.36 -07 27 10.9 16FL59 W84 C~3jrk 2015 04 15.130127 11 57 41.36 -07 27 10.8 16FL59 W84 C~3jrk 2016 01 08.62910 12 08 17.348 -08 28 41.39 22.8G 16FL59 F51 C~36rx 2016 01 08.63754 12 08 17.333 -08 28 41.39 22.8G 16FL59 F51 C~36rx 2016 01 08.64600 12 08 17.300 -08 28 41.49 22.6G 16FL59 F51 C~36rx 2016 01 16.67055 12 08 09.739 -08 29 21.34 22.0G 16FL59 F51 C~36rx 2016 01 18.60531 12 08 07.107 -08 29 24.52 22.8G 16FL59 F51 C~36rx 2016 01 18.61720 12 08 07.085 -08 29 24.44 23.1G 16FL59 F51 C~36rx 2016 01 18.62907 12 08 07.055 -08 29 24.97 22.7G 16FL59 F51 C~36rx 2016 01 18.64096 12 08 07.034 -08 29 24.37 22.5G 16FL59 F51 C~36rx 2016 02 03.56584 12 07 33.391 -08 28 25.83 22.6G 16FL59 F51 C~36rx 2016 02 03.57770 12 07 33.335 -08 28 25.76 22.5G 16FL59 F51 C~36rx 2016 02 03.58956 12 07 33.306 -08 28 25.51 23.2G 16FL59 F51 C~36rx 2016 02 03.60146 12 07 33.284 -08 28 25.45 22.8G 16FL59 F51 C~36rx 2016 02 10.53560 12 07 12.706 -08 27 12.18 23.2G 16FL59 F51 C~36rx 2016 03 10.40604 12 05 19.643 -08 17 48.02 22.7G 16FL59 F51 C~36rx 2016 03 13.43972 12 05 06.117 -08 16 28.55 22.1G 16FL59 F51 C~36rx 2016 03 13.45480 12 05 06.080 -08 16 28.17 23.1G 16FL59 F51 C~36rx 2016 03 13.46983 12 05 06.033 -08 16 27.88 23.4G 16FL59 F51 C~36rx 2016 03 28.26107 12 03 59.25 -08 09 29.8 23.6V 16FL59 W84 C~1qoJ 2016 03 28.26801 12 03 59.25 -08 09 29.8 16FL59 W84 C~1qoJ 2016 03 28.27495 12 03 59.25 -08 09 29.8 16FL59 W84 C~1qoJ 2016 03 29.21769 12 03 54.98 -08 09 01.4 16FL59 W84 C~1qoJ 2016 03 29.22463 12 03 54.98 -08 09 01.4 16FL59 W84 C~1qoJ 2016 03 29.23157 12 03 54.98 -08 09 01.5 16FL59 W84 C~1qoJ 2016 03 30.23576 12 03 50.41 -08 08 31.0 16FL59 W84 C~1qoJ 2016 03 30.24270 12 03 50.41 -08 08 31.0 16FL59 W84 C~1qoJ 2016 03 30.24964 12 03 50.43 -08 08 31.0 16FL59 W84 C~1qoJ 2016 03 31.22827 12 03 45.99 -08 08 01.3 16FL59 W84 C~1qoK 2016 03 31.23521 12 03 45.99 -08 08 01.4 16FL59 W84 C~1qoK 2016 03 31.24215 12 03 45.99 -08 08 01.4 16FL59 W84 C~1qoK 2016 04 01.24230 12 03 41.47 -08 07 30.8 16FL59 W84 C~1qoK 2016 04 01.24924 12 03 41.47 -08 07 30.9 16FL59 W84 C~1qoK 2016 04 01.25618 12 03 41.46 -08 07 30.8 16FL59 W84 C~1qoK 2016 04 01.36426 12 03 40.968 -08 07 27.72 23.4G 16FL59 F51 C~36rx 2016 04 01.37656 12 03 40.893 -08 07 27.35 22.6G 16FL59 F51 C~36rx 2016 04 01.38887 12 03 40.843 -08 07 27.04 22.7G 16FL59 F51 C~36rx 2016 04 01.40120 12 03 40.783 -08 07 26.45 23.0G 16FL59 F51 C~36rx 2016 04 02.32383 12 03 36.702 -08 06 59.08 23.7G 16FL59 F51 C~36rx 2016 04 02.34880 12 03 36.587 -08 06 58.27 22.6G 16FL59 F51 C~36rx 2016 04 02.37712 12 03 36.479 -08 06 57.29 23.7G 16FL59 F51 C~36rx 2016 04 02.38880 12 03 36.425 -08 06 56.96 22.9G 16FL59 F51 C~36rx 2016 04 02.40050 12 03 36.367 -08 06 56.59 23.3G 16FL59 F51 C~36rx 2016 04 10.147818 12 03 02.89 -08 03 01.0 16FL59 W84 C~3jrk 2016 04 10.149091 12 03 02.91 -08 03 01.1 16FL59 W84 C~3jrk 2016 04 30.75535 12 01 44.95 -07 52 53.4 16FL59 B31 C~1s3l 2016 04 30.75809 12 01 44.89 -07 52 54.2 16FL59 B31 C~1s3l 2016 04 30.90125 12 01 44.47 -07 52 49.8 16FL59 B31 C~1s3l 2016 04 30.90632 12 01 44.48 -07 52 49.6 22.5R 16FL59 B31 C~1s3l 2016 04 30.92154 12 01 44.39 -07 52 49.2 16FL59 B31 C~1s3l 2017 01 28.62004 12 12 49.288 -09 01 57.26 23.4G 16FL59 F51 C~36rx 2017 02 22.49007 12 11 32.226 -08 57 04.74 23.6G 16FL59 F51 C~36rx 2017 03 17.43836 12 09 54.905 -08 48 13.29 23.6G 16FL59 F51 C~36rx 2017 03 27.48922 12 09 09.417 -08 43 29.04 22.8G 16FL59 F51 C~36rx 2018 03 20.44554 12 14 48.809 -09 20 09.13 23.6G 16FL59 F51 C~36rx 2019 01 17.60299 12 23 14.308 -10 06 50.28 22.8G 16FL59 F51 C~36rx 2019 04 06.38995 12 18 40.327 -09 45 01.76 22.1G 16FL59 F51 C~36rx 2019 04 06.40240 12 18 40.256 -09 45 01.03 22.9G 16FL59 F51 C~36rx 2019 04 06.41483 12 18 40.201 -09 45 00.88 23.0G 16FL59 F51 C~36rx 2019 04 06.42727 12 18 40.109 -09 45 00.42 22.9G 16FL59 F51 C~36rx 2019 05 01.38123 12 16 58.948 -09 32 32.90 23.2G 16FL59 F51 C~36rx 2019 05 01.39328 12 16 58.917 -09 32 32.62 22.4G 16FL59 F51 C~36rx 2019 05 01.40537 12 16 58.870 -09 32 31.96 22.5G 16FL59 F51 C~36rx 2019 05 01.41753 12 16 58.831 -09 32 31.32 22.4G 16FL59 F51 C~36rx 2019 05 09.33171 12 16 32.837 -09 28 50.69 22.6G 16FL59 F51 C~36rx 2022 03 02.413020 12 36 36.620 -11 36 26.38 23.3G 16FL59 G37 C~5SAz 2022 03 02.454140 12 36 36.493 -11 36 24.25 16FL59 G37 C~5SAz
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 -0.03
2 0.0000 0.00 0.00 0.00 0.25
3 0.0001 0.00 0.14 0.00 0.08
4 0.0001 0.00 0.28 0.00 -0.03
5 0.9229 0.00 0.11 0.00 0.02
6 0.9720 0.00 0.01 0.00 0.39
7 1.9332 0.00 -0.01 0.00 -0.03
8 2.0150 0.00 0.24 0.00 0.06
9 2.2503 0.00 -0.08 0.00 -0.00
10 2.9107 0.00 -0.43 0.00 0.01
11 2.9325 0.00 0.04 0.00 -0.08
12 2.9325 0.00 -0.06 0.00 -0.35
13 2.9817 0.00 -0.77 0.00 -0.67
14 2.9818 0.00 -0.27 0.00 -0.67
15 3.0772 0.00 0.09 0.00 -0.10
16 3.0772 0.00 -0.15 0.00 0.20
17 3.0773 0.00 0.05 0.00 -0.14
18 3.0773 0.00 -0.04 0.00 0.20
19 3.0937 0.00 -0.22 0.00 -0.18
20 3.1484 0.00 -0.18 0.00 0.21
21 3.1484 0.00 -0.44 0.00 0.13
22 3.8169 0.00 -0.12 0.00 -0.06
23 3.8170 0.00 0.01 0.00 -0.12
24 3.8170 0.00 0.32 0.00 0.21
25 3.8171 0.00 -0.01 0.00 -0.02
26 3.8171 0.00 -0.20 0.00 0.27
27 3.8225 0.00 0.18 0.00 0.02
28 4.0348 0.00 -0.12 0.00 -0.08
29 4.0350 0.00 -0.21 0.00 -0.01
30 4.0352 0.00 -0.07 0.00 -0.02
31 4.0354 0.00 -0.24 0.00 0.03
32 4.0404 0.00 -0.08 0.00 0.23
33 4.0404 0.00 -0.02 0.00 0.30
34 4.7756 0.00 0.21 0.00 0.12
35 4.7756 0.00 0.07 0.00 0.18
36 4.7756 0.00 -0.34 0.00 0.14
37 4.7976 0.00 -0.34 0.00 -0.14
38 4.8029 0.00 0.16 0.00 0.18
39 4.8029 0.00 0.10 0.00 0.28
40 4.8029 0.00 -0.07 0.00 -0.24
41 4.8030 0.00 -0.11 0.00 0.37
42 4.8466 0.00 0.00 0.00 -0.14
43 4.8466 0.00 -0.34 0.00 -0.17
44 4.8466 0.00 -0.27 0.00 -0.02
45 4.8467 0.00 -0.10 0.00 -0.06
46 4.8656 0.00 0.05 0.00 0.10
47 4.9447 0.00 -0.06 0.00 -0.50
48 4.9530 0.00 -0.45 0.00 0.10
49 4.9530 0.00 0.03 0.00 0.08
50 4.9531 0.00 0.35 0.00 -0.02
51 4.9936 0.00 -0.29 0.00 0.24
52 4.9936 0.00 0.18 0.00 0.04
53 4.9936 0.00 0.65 0.00 -0.17
54 4.9962 0.00 -0.02 0.00 0.26
55 4.9962 0.00 0.46 0.00 0.05
56 4.9962 0.00 0.93 0.00 -0.26
57 4.9990 0.00 -0.22 0.00 0.32
58 4.9990 0.00 0.25 0.00 0.11
59 4.9990 0.00 1.02 0.00 -0.10
60 5.0017 0.00 -0.13 0.00 0.33
61 5.0017 0.00 0.34 0.00 0.02
62 5.0017 0.00 0.81 0.00 -0.19
63 5.0045 0.00 -0.32 0.00 0.39
64 5.0045 0.00 0.15 0.00 0.08
65 5.0045 0.00 0.47 0.00 -0.03
66 5.0048 0.00 0.13 0.00 -0.01
67 5.0048 0.00 -0.16 0.00 -0.01
68 5.0049 0.00 -0.08 0.00 -0.07
69 5.0049 0.00 -0.14 0.00 0.15
70 5.0074 0.00 -0.21 0.00 -0.27
71 5.0075 0.00 -0.25 0.00 -0.21
72 5.0076 0.00 0.04 0.00 -0.08
73 5.0076 0.00 0.02 0.00 -0.11
74 5.0076 0.00 -0.06 0.00 -0.09
75 5.0289 0.00 0.21 0.00 0.24
76 5.0289 0.00 0.60 0.00 0.10
77 5.0853 0.00 0.01 0.00 0.35
78 5.0853 0.00 -0.75 0.00 -0.53
79 5.0857 0.00 0.09 0.00 -0.11
80 5.0857 0.00 0.49 0.00 -0.05
81 5.0857 0.00 -0.10 0.00 -0.07
82 5.8323 0.00 -0.05 0.00 -0.08
83 5.9004 0.00 -0.12 0.00 -0.05
84 5.9633 0.00 -0.30 0.00 0.04
85 5.9908 0.00 -0.19 0.00 0.02
86 6.9708 0.00 -0.09 0.00 -0.12
87 7.8008 0.00 0.04 0.00 -0.30
88 8.0165 0.00 0.11 0.00 -0.17
89 8.0166 0.00 -0.11 0.00 0.18
90 8.0166 0.00 -0.09 0.00 -0.04
91 8.0166 0.00 -0.62 0.00 0.04
92 8.0849 0.00 -0.19 0.00 -0.35
93 8.0850 0.00 -0.00 0.00 -0.42
94 8.0850 0.00 -0.06 0.00 -0.10
95 8.0850 0.00 0.01 0.00 0.19
96 8.1067 0.00 -0.22 0.00 0.04
97 10.9214 0.00 -0.06 0.00 -0.32
98 10.9216 0.00 0.49 0.00 1.04
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.
16FL59 quality flag:3 Type: CLASSICAL CLASSICAL CLASSICAL axisobj 43.069 43.069 43.069 ecceobj 0.024 0.024 0.024 incobj 6.923 6.923 6.923 qmin 41.405 41.405 41.405 qmax 45.362 45.362 45.362 amean 43.271 43.271 43.271 amin 42.951 42.951 42.951 amax 43.606 43.606 43.607 emean 0.025 0.025 0.025 emin 0.010 0.010 0.010 emax 0.040 0.040 0.040 imean 8.658 8.658 8.658 imin 7.988 7.987 7.988 imax 9.287 9.287 9.287 excite_mean 0.153 0.153 0.153 fracstop 1.000 1.000 1.000 cjmean 3.065 3.065 3.065 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 179.3 179.5 179.4 kozaiamp 179.9 180.0 179.9