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: 13UZ17 # Created Fri Nov 22 02:09:47 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 39 observations of 39 # Arc: 7.28y # First observation: 2013/08/02 # Last observation: 2020/11/14 # Chi-squared of fit: 9.60 DOF: 72 RMS: 0.09 # Min/Max residuals: -0.29 0.28 # Exact a, adot, b, bdot, g, gdot: 1.679039E-05 2.723651E-02 2.536867E-06 3.425822E-03 2.551368E-02 2.203602E-03 # Covariance matrix: 1.2708E-13 -6.5126E-14 4.1959E-15 -9.1580E-15 6.7902E-14 -3.7532E-13 -6.5126E-14 1.5968E-13 -9.4356E-15 2.2217E-14 2.2101E-14 9.2210E-13 4.1959E-15 -9.4356E-15 4.9727E-14 -1.4677E-14 -3.9157E-16 -6.0600E-14 -9.1580E-15 2.2217E-14 -1.4677E-14 1.8032E-14 1.8433E-15 1.4214E-13 6.7902E-14 2.2101E-14 -3.9157E-16 1.8433E-15 1.0011E-13 8.2580E-14 -3.7532E-13 9.2210E-13 -6.0600E-14 1.4214E-13 8.2580E-14 5.8956E-12 # lat0 lon0 xBary yBary zBary JD0 -0.766299 17.650499 0.939637 -0.005165 -0.388428 2456507.032638 # Heliocentric elements and errors Epoch: 2456506.5000 = 2013/08/02 Mean Anomaly: 14.54802 +/- 0.018 Argument of Peri: 332.90135 +/- 0.028 Long of Asc Node: 22.32829 +/- 0.000 Inclination: 7.17769 +/- 0.000 Eccentricity: 0.17739384 +/- 0.0001 Semi-Major Axis: 47.65095140 +/- 0.0039 Time of Perihelion: 2451651.2994 +/- 6.2 Perihelion: 39.19796622 +/- 0.0049 Aphelion: 56.10393657 +/- 0.0059 Period (y) 328.9392 +/- 0.04 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 38.00101318 +/- 0.0005 Ecliptic Y 11.10866413 +/- 0.0001 Ecliptic Z -0.52404981 +/- 0.0000 Ecliptic XDOT -0.00066243 +/- 0.0000 Ecliptic YDOT 0.00285750 +/- 0.0000 Ecliptic ZDOT 0.00036457 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 39.59483769 +/- 0.0004 Geocenter to KBO 39.19463040 +/- 0.0005 # Hcoef: 7.90
The following table shows the complete astrometric record for 13UZ17. 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 (13UZ17) followed by the observatory code and reference code for the source of the astrometry.
2013 08 02.53186 01 06 16.459 +06 13 08.34 23.9r 13UZ17 568 C~2NKb 2013 08 02.57457 01 06 16.404 +06 13 08.08 23.9r 13UZ17 568 C~2NKb 2013 08 30.44895 01 05 10.415 +06 06 52.04 23.8r 13UZ17 568 C~2NKb 2013 08 31.45170 01 05 06.968 +06 06 31.92 23.8r 13UZ17 568 C~2NKb 2013 08 31.51259 01 05 06.754 +06 06 30.83 24.1r 13UZ17 568 C~2NKb 2013 08 31.51726 01 05 06.742 +06 06 30.46 24.3r 13UZ17 568 C~2NKb 2013 09 04.43153 01 04 52.731 +06 05 09.70 24.1r 13UZ17 568 C~2NKb 2013 09 04.47439 01 04 52.577 +06 05 08.56 24.4r 13UZ17 568 C~2NKb 2013 09 04.50640 01 04 52.430 +06 05 08.09 24.2r 13UZ17 568 C~2NKb 2013 10 06.41277 01 02 32.992 +05 51 41.31 23.7r 13UZ17 568 C~2NKb 2013 10 06.50014 01 02 32.575 +05 51 39.00 24.0r 13UZ17 568 C~2NKb 2013 10 06.50554 01 02 32.540 +05 51 38.82 23.8r 13UZ17 568 C~2NKb 2013 10 06.51103 01 02 32.519 +05 51 38.72 23.7r 13UZ17 568 C~2NKb 2013 10 06.51584 01 02 32.496 +05 51 38.57 23.8r 13UZ17 568 C~2NKb 2013 10 31.25446 01 00 37.161 +05 40 41.54 23.5r 13UZ17 568 C~2NKb 2013 10 31.29744 01 00 36.974 +05 40 40.56 23.9r 13UZ17 568 C~2NKb 2013 10 31.34016 01 00 36.777 +05 40 39.50 24.0r 13UZ17 568 C~2NKb 2013 11 01.28119 01 00 32.690 +05 40 16.49 23.5r 13UZ17 568 C~2NKb 2013 11 01.40856 01 00 32.115 +05 40 13.45 23.7r 13UZ17 568 C~2NKb 2013 11 05.45881 01 00 14.910 +05 38 37.36 23.8r 13UZ17 568 C~2NKb 2013 11 29.32101 00 58 52.362 +05 31 13.64 23.7r 13UZ17 568 C~2NKb 2013 11 29.32791 00 58 52.345 +05 31 13.25 23.5r 13UZ17 568 C~2NKb 2013 12 04.27126 00 58 40.308 +05 30 13.73 23.7r 13UZ17 568 C~2NKb 2013 12 04.32344 00 58 40.195 +05 30 13.10 24.0r 13UZ17 568 C~2NKb 2014 06 27.60171 01 11 26.656 +06 56 49.52 23.9r 13UZ17 568 C~2NKb 2014 06 28.60677 01 11 28.809 +06 57 03.81 24.1r 13UZ17 568 C~2NKb 2014 07 24.56479 01 11 52.795 +06 59 58.84 24.0r 13UZ17 568 C~2NKb 2014 07 27.59560 01 11 51.556 +06 59 54.94 23.8r 13UZ17 568 C~2NKb 2014 08 22.56814 01 11 08.124 +06 56 02.96 23.6r 13UZ17 568 C~2NKb 2014 08 22.58822 01 11 08.078 +06 56 02.94 23.8r 13UZ17 568 C~2NKb 2014 08 28.43091 01 10 50.872 +06 54 26.05 23.9r 13UZ17 568 C~2NKb 2014 10 23.35237 01 06 48.531 +06 31 27.99 23.6r 13UZ17 568 C~2NKb 2014 10 26.44781 01 06 34.177 +06 30 07.04 23.7r 13UZ17 568 C~2NKc 2014 10 27.39107 01 06 29.857 +06 29 42.78 23.9r 13UZ17 568 C~2NKc 2015 01 17.30307 01 03 56.421 +06 17 44.08 23.7r 13UZ17 568 C~2NKc 2015 08 20.51903 01 16 45.757 +07 42 51.44 23.9r 13UZ17 568 C~2NKc 2015 12 07.38190 01 09 35.492 +07 03 10.23 24.1w 13UZ17 568 C~2NKc 2020 11 14.124350 01 38 31.221 +10 56 40.55 22.9G 13UZ17 G37 C~4Nl8 2020 11 14.181420 01 38 30.973 +10 56 39.35 13UZ17 G37 C~4Nl8
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 0.05 0.00 -0.07
2 0.0001 0.00 0.06 0.00 -0.05
3 0.0764 0.00 0.10 0.00 0.12
4 0.0792 0.00 -0.09 0.00 -0.14
5 0.0793 0.00 -0.06 0.00 -0.01
6 0.0794 0.00 0.01 0.00 -0.29
7 0.0901 0.00 0.04 0.00 0.10
8 0.0902 0.00 0.16 0.00 -0.12
9 0.0903 0.00 -0.23 0.00 0.10
10 0.1776 0.00 0.02 0.00 -0.06
11 0.1779 0.00 0.13 0.00 0.03
12 0.1779 0.00 -0.01 0.00 0.00
13 0.1779 0.00 0.08 0.00 0.05
14 0.1779 0.00 0.08 0.00 0.04
15 0.2456 0.00 -0.07 0.00 -0.08
16 0.2458 0.00 -0.00 0.00 -0.01
17 0.2459 0.00 -0.10 0.00 -0.02
18 0.2485 0.00 0.03 0.00 -0.04
19 0.2488 0.00 -0.15 0.00 0.01
20 0.2599 0.00 -0.03 0.00 -0.05
21 0.3252 0.00 0.09 0.00 0.28
22 0.3252 0.00 0.12 0.00 -0.01
23 0.3388 0.00 -0.08 0.00 0.01
24 0.3389 0.00 0.04 0.00 -0.06
25 0.9009 0.00 -0.01 0.00 -0.02
26 0.9037 0.00 -0.03 0.00 0.02
27 0.9748 0.00 0.12 0.00 0.00
28 0.9831 0.00 0.00 0.00 0.08
29 1.0542 0.00 -0.12 0.00 -0.11
30 1.0542 0.00 0.04 0.00 0.17
31 1.0702 0.00 -0.05 0.00 -0.07
32 1.2233 0.00 -0.03 0.00 0.12
33 1.2318 0.00 -0.02 0.00 0.02
34 1.2344 0.00 -0.04 0.00 0.07
35 1.4586 0.00 -0.07 0.00 -0.02
36 2.0479 0.00 -0.01 0.00 0.05
37 2.3459 0.00 0.02 0.00 0.05
38 7.2843 0.00 0.01 0.00 -0.09
39 7.2845 0.00 0.02 0.00 0.02
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.
13UZ17 quality flag:3 Type: 2:1E 2:1E 2:1E axisobj 47.962 47.962 47.962 ecceobj 0.183 0.183 0.183 incobj 7.161 7.161 7.161 qmin 38.547 38.547 38.547 qmax 57.918 57.917 57.918 amean 47.797 47.797 47.797 amin 47.169 47.168 47.169 amax 48.504 48.499 48.506 emean 0.174 0.174 0.174 emin 0.150 0.151 0.150 emax 0.194 0.194 0.194 imean 7.560 7.562 7.560 imin 6.996 7.000 6.994 imax 8.300 8.304 8.298 excite_mean 0.218 0.218 0.218 fracstop 1.000 1.000 1.000 cjmean 3.089 3.089 3.089 libcent 0 180.8 180.8 180.9 libamp 0 158.2 158.3 158.1 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 152.4 152.5 152.4 kozaiamp 180.0 179.9 180.0