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: 10RJ190 # Created Sun Nov 24 02:09:06 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 105 observations of 105 # Arc: 14.08y # First observation: 2010/09/04 # Last observation: 2024/10/01 # Chi-squared of fit: 73.13 DOF: 204 RMS: 0.15 # Min/Max residuals: -0.58 0.43 # Exact a, adot, b, bdot, g, gdot: 1.612551E-05 2.428679E-02 -1.136343E-06 -4.882986E-04 2.441247E-02 -1.344162E-03 # Covariance matrix: 1.0725E-13 -3.1020E-14 -9.6442E-16 4.4751E-16 -1.7547E-14 -7.2533E-14 -3.1020E-14 1.1731E-14 4.5084E-16 -1.9575E-16 2.5195E-15 3.2594E-14 -9.6442E-16 4.5084E-16 5.3965E-14 -8.7126E-15 -1.3095E-16 1.5195E-15 4.4751E-16 -1.9575E-16 -8.7126E-15 1.8865E-15 -6.7154E-17 -6.4594E-16 -1.7547E-14 2.5195E-15 -1.3095E-16 -6.7154E-17 5.1706E-14 2.6420E-15 -7.2533E-14 3.2594E-14 1.5195E-15 -6.4594E-16 2.6420E-15 1.0851E-13 # lat0 lon0 xBary yBary zBary JD0 -2.833111 -26.319725 -0.137085 -0.049213 -0.993491 2455443.811016 # Heliocentric elements and errors Epoch: 2455444.5000 = 2010/09/05 Mean Anomaly: 321.93591 +/- 0.015 Argument of Peri: 291.82538 +/- 0.018 Long of Asc Node: 86.26346 +/- 0.002 Inclination: 2.99088 +/- 0.000 Eccentricity: 0.08004695 +/- 0.0000 Semi-Major Axis: 44.65525843 +/- 0.0018 Time of Perihelion: 2466968.9532 +/- 7.4 Perihelion: 41.08074106 +/- 0.0019 Aphelion: 48.22977579 +/- 0.0022 Period (y) 298.4126 +/- 0.02 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 37.62820637 +/- 0.0003 Ecliptic Y -18.45884686 +/- 0.0002 Ecliptic Z -2.02467483 +/- 0.0000 Ecliptic XDOT 0.00107086 +/- 0.0000 Ecliptic YDOT 0.00251568 +/- 0.0000 Ecliptic ZDOT -0.00004727 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 41.96085201 +/- 0.0003 Geocenter to KBO 40.96273522 +/- 0.0004 # Hcoef: 6.73
The following table shows the complete astrometric record for 10RJ190. 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 (10RJ190) followed by the observatory code and reference code for the source of the astrometry.
2010 09 04.31025 22 26 33.956 -12 47 49.56 22.4G 10RJ190 F51 C~345E 2010 09 04.32162 22 26 33.914 -12 47 49.90 22.6G 10RJ190 F51 C~345E 2010 09 13.30728 22 25 53.791 -12 51 33.67 22.6G 10RJ190 F51 C~345E 2010 09 13.31873 22 25 53.727 -12 51 34.14 22.7G 10RJ190 F51 C~345E 2010 09 14.29503 22 25 49.482 -12 51 57.50 22.4G 10RJ190 F51 C~345E 2010 09 14.30643 22 25 49.402 -12 51 57.67 21.8G 10RJ190 F51 C~345E 2011 07 27.47959 22 34 43.720 -12 01 24.82 22.9G 10RJ190 F51 C~345E 2011 07 27.49431 22 34 43.666 -12 01 25.11 22.7G 10RJ190 F51 C~345E 2011 07 27.50899 22 34 43.625 -12 01 25.63 23.1G 10RJ190 F51 C~345E 2011 07 27.52372 22 34 43.551 -12 01 26.01 22.5G 10RJ190 F51 C~345E 2011 08 24.43082 22 32 46.394 -12 13 37.14 22.5G 10RJ190 F51 C~345E 2011 08 24.44481 22 32 46.338 -12 13 37.58 22.7G 10RJ190 F51 C~345E 2011 08 24.45878 22 32 46.274 -12 13 37.90 22.5G 10RJ190 F51 C~345E 2011 08 24.47276 22 32 46.213 -12 13 38.32 22.4G 10RJ190 F51 C~345E 2012 08 17.44162 22 38 35.166 -11 41 01.31 22.8G 10RJ190 F51 C~345E 2012 08 17.45590 22 38 35.087 -11 41 01.84 22.8G 10RJ190 F51 C~345E 2012 08 17.47016 22 38 35.024 -11 41 02.25 22.4G 10RJ190 F51 C~345E 2012 08 17.48444 22 38 34.979 -11 41 02.29 22.1G 10RJ190 F51 C~345E 2012 09 04.43310 22 37 13.840 -11 49 09.80 23.2G 10RJ190 F51 C~345E 2012 09 04.44468 22 37 13.768 -11 49 09.97 22.5G 10RJ190 F51 C~345E 2013 08 26.47528 22 43 15.859 -11 14 52.67 23.3G 10RJ190 F51 C~345E 2013 08 26.50173 22 43 15.779 -11 14 53.15 22.7G 10RJ190 F51 C~345E 2013 08 26.51405 22 43 15.727 -11 14 53.64 22.5G 10RJ190 F51 C~345E 2013 08 31.42431 22 42 53.429 -11 17 08.57 22.9G 10RJ190 F51 C~345E 2013 08 31.42890 22 42 53.399 -11 17 09.07 22.3G 10RJ190 F51 C~345E 2013 08 31.44336 22 42 53.354 -11 17 09.33 22.9G 10RJ190 F51 C~345E 2013 08 31.45784 22 42 53.280 -11 17 09.81 22.7G 10RJ190 F51 C~345E 2013 09 14.38470 22 41 50.389 -11 23 18.86 22.3G 10RJ190 F51 C~345E 2014 06 26.56062 22 51 52.254 -10 21 34.93 22.9G 10RJ190 F51 C~345E 2014 06 28.51572 22 51 49.740 -10 21 59.04 22.6G 10RJ190 F51 C~345E 2014 06 28.52783 22 51 49.707 -10 21 59.19 22.7G 10RJ190 F51 C~345E 2014 06 28.53987 22 51 49.699 -10 21 59.24 22.9G 10RJ190 F51 C~345E 2014 06 28.55193 22 51 49.677 -10 21 59.34 22.9G 10RJ190 F51 C~345E 2014 07 25.52861 22 50 45.065 -10 30 13.48 22.6G 10RJ190 F51 C~345E 2014 07 25.54072 22 50 45.044 -10 30 13.66 23.7G 10RJ190 F51 C~345E 2014 07 25.55285 22 50 44.978 -10 30 13.77 22.9G 10RJ190 F51 C~345E 2014 07 25.56495 22 50 44.933 -10 30 14.29 22.4G 10RJ190 F51 C~345E 2014 08 03.48106 22 50 13.178 -10 33 51.58 22.7G 10RJ190 F51 C~345E 2014 08 03.49450 22 50 13.140 -10 33 51.80 22.8G 10RJ190 F51 C~345E 2014 08 03.50793 22 50 13.091 -10 33 52.19 22.9G 10RJ190 F51 C~345E 2014 08 03.52136 22 50 13.034 -10 33 52.82 23.1G 10RJ190 F51 C~345E 2014 08 05.50186 22 50 05.428 -10 34 43.27 23.5G 10RJ190 F51 C~345E 2014 08 05.51536 22 50 05.371 -10 34 43.57 22.2G 10RJ190 F51 C~345E 2014 08 20.43159 22 49 03.315 -10 41 25.63 22.8G 10RJ190 F51 C~345E 2014 08 20.44444 22 49 03.260 -10 41 25.86 22.3G 10RJ190 F51 C~345E 2014 09 02.36762 22 48 05.191 -10 47 24.98 22.7G 10RJ190 F51 C~345E 2014 09 02.38118 22 48 05.130 -10 47 25.44 22.7G 10RJ190 F51 C~345E 2014 09 02.39474 22 48 05.069 -10 47 25.66 22.6G 10RJ190 F51 C~345E 2014 09 18.29406 22 46 53.696 -10 54 27.47 23.1G 10RJ190 F51 C~345E 2014 09 18.29472 22 46 53.702 -10 54 27.46 23.4G 10RJ190 F51 C~345E 2014 09 18.30566 22 46 53.641 -10 54 28.04 22.6G 10RJ190 F51 C~345E 2014 09 18.30632 22 46 53.632 -10 54 27.92 23.4G 10RJ190 F51 C~345E 2014 09 18.36391 22 46 53.387 -10 54 29.42 22.8G 10RJ190 F51 C~345E 2014 09 18.36457 22 46 53.393 -10 54 29.56 22.0G 10RJ190 F51 C~345E 2014 09 18.37562 22 46 53.322 -10 54 29.59 22.7G 10RJ190 F51 C~345E 2014 09 18.37628 22 46 53.339 -10 54 29.73 22.6G 10RJ190 F51 C~345E 2014 11 10.24840 22 44 13.703 -11 07 52.72 23.2G 10RJ190 F51 C~345E 2015 07 12.50489 22 56 39.001 -09 54 44.57 22.2G 10RJ190 F51 C~345E 2015 07 12.51602 22 56 38.976 -09 54 44.82 22.9G 10RJ190 F51 C~345E 2015 07 12.52719 22 56 38.952 -09 54 45.29 22.9G 10RJ190 F51 C~345E 2015 07 12.53834 22 56 38.920 -09 54 45.38 22.2G 10RJ190 F51 C~345E 2015 10 26.26583 22 49 56.695 -10 35 51.86 22.3G 10RJ190 F51 C~345E 2015 11 03.27352 22 49 39.353 -10 37 06.16 23.0G 10RJ190 F51 C~345E 2015 11 03.28580 22 49 39.330 -10 37 06.42 22.9G 10RJ190 F51 C~345E 2015 11 03.29808 22 49 39.293 -10 37 06.43 22.4G 10RJ190 F51 C~345E 2015 11 03.31032 22 49 39.282 -10 37 06.38 23.3G 10RJ190 F51 C~345E 2016 07 07.53556 23 02 02.794 -09 22 22.53 22.9G 10RJ190 F51 C~345E 2016 07 07.54681 23 02 02.748 -09 22 22.48 22.8G 10RJ190 F51 C~345E 2016 07 07.55802 23 02 02.732 -09 22 22.49 22.5G 10RJ190 F51 C~345E 2016 07 07.56922 23 02 02.701 -09 22 22.77 22.7G 10RJ190 F51 C~345E 2016 07 11.55846 23 01 54.505 -09 23 29.75 23.2G 10RJ190 F51 C~345E 2016 07 11.57098 23 01 54.498 -09 23 30.03 22.9G 10RJ190 F51 C~345E 2016 07 11.58347 23 01 54.446 -09 23 30.06 22.7G 10RJ190 F51 C~345E 2016 07 11.59596 23 01 54.439 -09 23 30.43 23.1G 10RJ190 F51 C~345E 2016 08 02.51371 23 00 49.790 -09 31 23.69 22.4G 10RJ190 F51 C~345E 2016 08 02.52476 23 00 49.740 -09 31 24.23 22.6G 10RJ190 F51 C~345E 2016 08 02.53582 23 00 49.700 -09 31 24.46 22.7G 10RJ190 F51 C~345E 2016 08 02.54687 23 00 49.659 -09 31 24.67 23.2G 10RJ190 F51 C~345E 2016 08 27.45365 22 59 07.199 -09 42 40.75 22.8G 10RJ190 F51 C~345E 2016 08 27.46474 22 59 07.122 -09 42 40.83 22.4G 10RJ190 F51 C~345E 2016 08 27.47587 22 59 07.059 -09 42 41.18 22.1G 10RJ190 F51 C~345E 2016 08 27.48697 22 59 07.016 -09 42 41.80 22.7G 10RJ190 F51 C~345E 2016 10 06.36273 22 56 14.259 -09 59 47.54 22.6G 10RJ190 F51 C~345E 2016 10 06.37459 22 56 14.211 -09 59 48.08 22.7G 10RJ190 F51 C~345E 2016 10 06.38650 22 56 14.165 -09 59 48.35 22.4G 10RJ190 F51 C~345E 2016 10 06.39843 22 56 14.115 -09 59 48.64 22.6G 10RJ190 F51 C~345E 2016 10 25.25817 22 55 13.431 -10 05 02.54 22.4G 10RJ190 F51 C~345E 2016 10 25.26931 22 55 13.389 -10 05 02.54 22.1G 10RJ190 F51 C~345E 2016 10 25.28048 22 55 13.354 -10 05 03.34 22.8G 10RJ190 F51 C~345E 2016 10 25.29166 22 55 13.343 -10 05 03.42 21.8G 10RJ190 F51 C~345E 2017 09 15.40076 23 03 01.245 -09 19 43.33 23.0G 10RJ190 F51 C~345E 2017 09 15.41188 23 03 01.190 -09 19 43.61 22.4G 10RJ190 F51 C~345E 2017 09 15.42308 23 03 01.146 -09 19 43.81 22.4G 10RJ190 F51 C~345E 2017 09 15.43418 23 03 01.107 -09 19 44.12 22.9G 10RJ190 F51 C~345E 2017 11 07.31320 23 00 01.190 -09 35 56.50 23.0G 10RJ190 F51 C~345E 2018 07 12.54856 23 12 22.852 -08 20 11.20 22.6G 10RJ190 F51 C~345E 2018 07 12.55962 23 12 22.815 -08 20 11.32 23.1G 10RJ190 F51 C~345E 2018 08 08.49356 23 11 03.781 -08 29 58.41 23.5G 10RJ190 F51 C~345E 2018 08 08.50536 23 11 03.752 -08 29 58.43 23.3G 10RJ190 F51 C~345E 2018 08 08.51719 23 11 03.680 -08 29 58.79 23.4G 10RJ190 F51 C~345E 2018 08 08.52902 23 11 03.659 -08 29 59.25 22.7G 10RJ190 F51 C~345E 2018 08 18.55034 23 10 24.033 -08 34 28.87 23.1G 10RJ190 F51 C~345E 2024 10 01.253960 23 39 00.333 -05 36 07.80 22.9G 10RJ190 G37 C~8Gqy 2024 10 01.292830 23 39 00.166 -05 36 08.92 10RJ190 G37 C~8Gqy 2024 10 01.332090 23 38 59.985 -05 36 09.88 10RJ190 G37 C~8Gqy
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 0.13
2 0.0000 0.00 0.01 0.00 0.08
3 0.0246 0.00 0.15 0.00 0.04
4 0.0247 0.00 -0.04 0.00 -0.15
5 0.0273 0.00 0.05 0.00 -0.22
6 0.0274 0.00 -0.39 0.00 -0.12
7 0.8930 0.00 0.01 0.00 0.16
8 0.8930 0.00 0.03 0.00 0.22
9 0.8931 0.00 0.24 0.00 0.06
10 0.8931 0.00 -0.05 0.00 0.03
11 0.9695 0.00 -0.10 0.00 0.00
12 0.9696 0.00 0.03 0.00 -0.06
13 0.9696 0.00 0.04 0.00 -0.00
14 0.9696 0.00 0.09 0.00 -0.04
15 1.9524 0.00 0.08 0.00 0.04
16 1.9525 0.00 -0.14 0.00 -0.10
17 1.9525 0.00 -0.12 0.00 -0.12
18 1.9526 0.00 0.17 0.00 0.23
19 2.0017 0.00 0.30 0.00 -0.01
20 2.0017 0.00 0.02 0.00 0.13
21 2.9765 0.00 -0.58 0.00 0.06
22 2.9766 0.00 0.04 0.00 0.31
23 2.9766 0.00 0.11 0.00 0.16
24 2.9900 0.00 0.03 0.00 0.24
25 2.9901 0.00 -0.10 0.00 -0.14
26 2.9901 0.00 0.23 0.00 -0.00
27 2.9901 0.00 0.13 0.00 -0.09
28 3.0283 0.00 -0.16 0.00 0.15
29 3.8090 0.00 -0.01 0.00 0.07
30 3.8144 0.00 0.07 0.00 -0.16
31 3.8144 0.00 -0.17 0.00 -0.15
32 3.8145 0.00 -0.03 0.00 -0.05
33 3.8145 0.00 -0.09 0.00 0.00
34 3.8883 0.00 0.02 0.00 -0.06
35 3.8884 0.00 0.32 0.00 0.04
36 3.8884 0.00 -0.05 0.00 0.21
37 3.8884 0.00 -0.10 0.00 -0.03
38 3.9129 0.00 -0.17 0.00 -0.15
39 3.9129 0.00 0.04 0.00 -0.02
40 3.9129 0.00 0.09 0.00 -0.07
41 3.9130 0.00 0.01 0.00 -0.36
42 3.9184 0.00 -0.09 0.00 -0.03
43 3.9184 0.00 -0.14 0.00 0.02
44 3.9593 0.00 0.19 0.00 -0.03
45 3.9593 0.00 0.22 0.00 0.10
46 3.9947 0.00 0.02 0.00 0.08
47 3.9947 0.00 0.04 0.00 -0.00
48 3.9948 0.00 0.07 0.00 0.15
49 4.0383 0.00 -0.02 0.00 0.05
50 4.0383 0.00 0.11 0.00 0.08
51 4.0383 0.00 -0.08 0.00 -0.22
52 4.0383 0.00 -0.17 0.00 -0.09
53 4.0385 0.00 -0.01 0.00 -0.14
54 4.0385 0.00 0.13 0.00 -0.26
55 4.0385 0.00 -0.20 0.00 -0.01
56 4.0385 0.00 0.10 0.00 -0.14
57 4.1833 0.00 -0.21 0.00 0.06
58 4.8520 0.00 -0.13 0.00 0.13
59 4.8520 0.00 -0.11 0.00 0.08
60 4.8521 0.00 -0.06 0.00 -0.18
61 4.8521 0.00 -0.14 0.00 -0.07
62 5.1416 0.00 0.11 0.00 -0.17
63 5.1635 0.00 0.11 0.00 -0.02
64 5.1635 0.00 0.12 0.00 -0.19
65 5.1636 0.00 -0.08 0.00 -0.11
66 5.1636 0.00 0.11 0.00 0.02
67 5.8405 0.00 0.42 0.00 -0.23
68 5.8405 0.00 0.07 0.00 -0.00
69 5.8405 0.00 0.16 0.00 0.16
70 5.8405 0.00 0.03 0.00 0.06
71 5.8515 0.00 -0.08 0.00 -0.09
72 5.8515 0.00 0.24 0.00 -0.15
73 5.8515 0.00 -0.11 0.00 0.04
74 5.8516 0.00 0.22 0.00 -0.11
75 5.9116 0.00 0.08 0.00 0.21
76 5.9116 0.00 -0.06 0.00 -0.05
77 5.9116 0.00 -0.04 0.00 -0.00
78 5.9117 0.00 -0.04 0.00 0.06
79 5.9799 0.00 0.32 0.00 0.03
80 5.9799 0.00 -0.08 0.00 0.27
81 5.9799 0.00 -0.26 0.00 0.23
82 5.9800 0.00 -0.15 0.00 -0.07
83 6.0891 0.00 0.11 0.00 0.43
84 6.0892 0.00 0.08 0.00 0.13
85 6.0892 0.00 0.08 0.00 0.10
86 6.0892 0.00 0.02 0.00 0.06
87 6.1409 0.00 0.19 0.00 0.08
88 6.1409 0.00 0.01 0.00 0.22
89 6.1409 0.00 -0.07 0.00 -0.44
90 6.1409 0.00 0.22 0.00 -0.39
91 7.0310 0.00 -0.12 0.00 -0.03
92 7.0311 0.00 -0.18 0.00 -0.01
93 7.0311 0.00 -0.08 0.00 0.09
94 7.0311 0.00 0.10 0.00 0.08
95 7.1759 0.00 -0.14 0.00 -0.03
96 7.8528 0.00 0.09 0.00 -0.06
97 7.8528 0.00 -0.12 0.00 0.01
98 7.9266 0.00 -0.13 0.00 -0.13
99 7.9266 0.00 0.11 0.00 0.16
100 7.9266 0.00 -0.30 0.00 0.11
101 7.9267 0.00 0.07 0.00 -0.05
102 7.9541 0.00 -0.08 0.00 0.11
103 14.0751 0.00 0.00 0.00 0.02
104 14.0752 0.00 0.08 0.00 -0.06
105 14.0754 0.00 -0.04 0.00 0.03
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.
10RJ190 quality flag:3 Type: CLASSICAL CLASSICAL CLASSICAL axisobj 44.531 44.531 44.531 ecceobj 0.079 0.079 0.080 incobj 2.994 2.994 2.994 qmin 39.989 39.996 39.988 qmax 49.114 49.117 49.114 amean 44.430 44.430 44.430 amin 44.073 44.076 44.071 amax 44.807 44.810 44.806 emean 0.081 0.081 0.081 emin 0.065 0.064 0.065 emax 0.096 0.096 0.096 imean 1.365 1.365 1.365 imin 0.614 0.614 0.614 imax 1.991 1.991 1.992 excite_mean 0.084 0.084 0.084 fracstop 1.000 1.000 1.000 cjmean 3.098 3.098 3.098 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 165.7 165.8 165.9 kozaiamp 180.0 180.0 180.0