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: 135742 # Created Fri Nov 22 02:06:54 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 40 observations of 40 # Arc: 17.08y # First observation: 2002/08/05 # Last observation: 2019/09/04 # Chi-squared of fit: 38.23 DOF: 74 RMS: 0.17 # Min/Max residuals: -0.47 0.44 # Exact a, adot, b, bdot, g, gdot: 1.625053E-05 2.547709E-02 2.240172E-06 2.408910E-03 2.523536E-02 2.861591E-03 # 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 -0.822801 -31.257637 0.282447 -0.014113 -0.978430 2452491.960733 # Heliocentric elements and errors Epoch: 2452492.5000 = 2002/08/06 Mean Anomaly: 51.45327 +/- 0.000 Argument of Peri: 288.11881 +/- 0.000 Long of Asc Node: 336.77526 +/- 0.000 Inclination: 5.46378 +/- 0.000 Eccentricity: 0.12181389 +/- 0.0000 Semi-Major Axis: 43.46145551 +/- 0.0000 Time of Perihelion: 2437534.7830 +/- 0.0 Perihelion: 38.16724671 +/- 0.0000 Aphelion: 48.75566431 +/- 0.0000 Period (y) 286.5264 +/- 0.00 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 34.56131944 +/- 0.0000 Ecliptic Y -21.30316220 +/- 0.0000 Ecliptic Z -0.56893170 +/- 0.0000 Ecliptic XDOT 0.00169504 +/- 0.0000 Ecliptic YDOT 0.00219724 +/- 0.0000 Ecliptic ZDOT 0.00025707 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 40.60329911 +/- 0.0000 Geocenter to KBO 39.62689275 +/- 0.0000 # Hcoef: 6.91
The following table shows the complete astrometric record for 135742. 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 (135742) followed by the observatory code and reference code for the source of the astrometry.
2002 08 05.45999 22 04 43.02 -12 40 58.5 22.5R 135742 568 Cp2010 2002 08 05.52244 22 04 42.73 -12 41 00.0 22.6R 135742 568 Cp2010 2002 08 05.58780 22 04 42.43 -12 41 01.5 22.7R 135742 568 Cp2010 2002 09 02.98961 22 02 28.16 -12 52 29.2 135742 493 Cp2010 2002 09 03.03341 22 02 27.97 -12 52 30.0 135742 493 Cp2010 2002 09 03.99461 22 02 23.50 -12 52 52.2 135742 950 Cp2010 2002 09 04.03060 22 02 23.33 -12 52 53.3 22.7R 135742 950 Cp2010 2002 09 04.07120 22 02 23.14 -12 52 54.4 135742 950 Cp2010 2002 09 05.99491 22 02 14.26 -12 53 38.9 135742 493 Cp2010 2002 09 06.00801 22 02 14.20 -12 53 39.1 135742 493 Cp2010 2002 09 06.07281 22 02 13.91 -12 53 40.9 135742 493 Cp2010 2002 09 06.08571 22 02 13.81 -12 53 41.2 135742 493 Cp2010 2002 09 07.02081 22 02 09.54 -12 54 02.4 135742 493 Cp2010 2002 09 07.03351 22 02 09.49 -12 54 02.7 135742 493 Cp2010 2002 09 07.10061 22 02 09.17 -12 54 04.2 135742 493 Cp2010 2002 09 30.26756 22 00 34.19 -13 01 47.7 22.4R 135742 568 Cp2010 2002 09 30.32329 22 00 33.98 -13 01 48.7 22.4R 135742 568 Cp2010 2002 09 30.38512 22 00 33.75 -13 01 49.9 22.6R 135742 568 Cp2010 2002 10 03.86081 22 00 22.02 -13 02 44.9 135742 493 Cp2010 2002 10 03.94101 22 00 21.79 -13 02 46.4 135742 493 Cp2010 2002 10 03.95391 22 00 21.74 -13 02 46.2 135742 493 Cp2010 2003 06 24.52643 22 12 29.94 -11 49 48.8 23.2i 135742 568 Cp2010 2003 06 25.50024 22 12 27.97 -11 49 59.6 23.0i 135742 568 Cp2010 2003 06 25.55086 22 12 27.84 -11 50 00.0 23.0i 135742 568 Cp2010 2003 06 25.59926 22 12 27.76 -11 50 00.5 23.2i 135742 568 Cp2010 2003 07 28.26119 22 10 41.90 -11 59 24.8 135742 809 Cp2010 2003 07 28.37330 22 10 41.42 -11 59 27.7 135742 809 Cp2010 2003 07 28.41532 22 10 41.26 -11 59 28.7 135742 809 Cp2010 2003 07 29.23289 22 10 37.84 -11 59 46.9 135742 809 Cp2010 2003 08 31.33942 22 08 04.97 -12 13 08.0 23.5g 135742 568 Cp2010 2003 08 31.37380 22 08 04.82 -12 13 08.8 22.9g 135742 568 Cp2010 2003 08 31.40015 22 08 04.70 -12 13 09.3 23.1g 135742 568 Cp2010 2004 09 06.30305 22 12 53.68 -11 37 28.3 22.6R 135742 695 Cp2010 2004 09 07.28000 22 12 49.18 -11 37 51.6 22.4R 135742 695 Cp2010 2004 09 07.35414 22 12 48.87 -11 37 53.4 22.7R 135742 695 Cp2010 2006 06 21.32536 22 28 08.69 -09 54 32.2 23.0R 135742 304 Cr4824 2006 06 21.36792 22 28 08.63 -09 54 32.4 135742 304 Cr4824 2019 09 04.350820 23 27 44.805 -01 55 29.95 23.1G 135742 G37 C~3WTu 2019 09 04.407620 23 27 44.556 -01 55 31.46 135742 G37 C~3WTu 2019 09 04.469780 23 27 44.292 -01 55 33.16 135742 G37 C~3WTu
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 -0.00 0.00 -0.16
2 0.0002 0.00 -0.00 0.00 -0.18
3 0.0003 0.00 0.05 0.00 -0.14
4 0.0781 0.00 -0.24 0.00 -0.15
5 0.0782 0.00 0.03 0.00 0.08
6 0.0809 0.00 0.03 0.00 0.35
7 0.0810 0.00 0.04 0.00 0.09
8 0.0811 0.00 0.06 0.00 -0.07
9 0.0863 0.00 0.21 0.00 0.03
10 0.0864 0.00 0.23 0.00 0.13
11 0.0866 0.00 0.42 0.00 -0.18
12 0.0866 0.00 -0.18 0.00 -0.19
13 0.0891 0.00 0.01 0.00 0.06
14 0.0892 0.00 0.14 0.00 0.05
15 0.0894 0.00 0.00 0.00 0.07
16 0.1528 0.00 0.07 0.00 0.05
17 0.1529 0.00 -0.08 0.00 -0.03
18 0.1531 0.00 -0.21 0.00 -0.22
19 0.1626 0.00 -0.17 0.00 -0.18
20 0.1629 0.00 0.39 0.00 -0.47
21 0.1629 0.00 0.29 0.00 -0.08
22 0.8845 0.00 -0.14 0.00 0.06
23 0.8872 0.00 0.22 0.00 -0.10
24 0.8873 0.00 -0.09 0.00 0.07
25 0.8874 0.00 0.30 0.00 0.11
26 0.9769 0.00 -0.30 0.00 0.44
27 0.9772 0.00 -0.33 0.00 0.03
28 0.9773 0.00 -0.06 0.00 -0.05
29 0.9795 0.00 -0.02 0.00 0.01
30 1.0702 0.00 -0.32 0.00 0.05
31 1.0703 0.00 -0.10 0.00 0.09
32 1.0703 0.00 -0.00 0.00 0.23
33 2.0886 0.00 0.05 0.00 0.04
34 2.0912 0.00 -0.34 0.00 0.09
35 2.0914 0.00 0.18 0.00 0.06
36 3.8764 0.00 0.03 0.00 0.04
37 3.8765 0.00 0.07 0.00 0.14
38 17.0812 0.00 -0.06 0.00 -0.00
39 17.0813 0.00 -0.02 0.00 -0.02
40 17.0815 0.00 0.13 0.00 -0.09
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.
135742 quality flag:2 Type: 7:4EEE CLASSICAL 7:4EEE axisobj 43.797 43.797 43.797 ecceobj 0.125 0.125 0.125 incobj 5.442 5.442 5.442 qmin 37.019 36.833 37.018 qmax 50.758 51.027 50.861 amean 43.727 43.727 43.727 amin 43.355 43.364 43.364 amax 44.140 44.142 44.166 emean 0.109 0.110 0.113 emin 0.050 0.045 0.051 emax 0.152 0.157 0.152 imean 7.309 7.536 7.068 imin 5.979 5.494 5.733 imax 8.882 9.873 8.784 excite_mean 0.170 0.175 0.170 fracstop 1.000 1.000 1.000 cjmean 3.064 3.061 3.064 libcent 0 176.0 -180.0 196.7 libamp 0 175.5 -180.0 125.4 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 267.9 275.6 269.6 kozaiamp 49.1 80.1 59.0