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: 13GQ136
# Created Sun Nov 24 02:09:22 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 37 observations of 37
# Arc: 11.10y
# First observation: 2013/03/07
# Last observation: 2024/04/14
# Chi-squared of fit: 11.42 DOF: 68 RMS: 0.10
# Min/Max residuals: -0.18 0.31
# Exact a, adot, b, bdot, g, gdot:
1.174721E-05 1.451163E-02 4.020481E-08 4.978227E-04 1.842113E-02 -1.525243E-03
# Covariance matrix:
1.3348E-13 -4.8538E-14 9.1910E-16 -1.4371E-15 7.6634E-14 -2.5752E-13
-4.8538E-14 6.0722E-14 -1.3976E-15 2.0376E-15 1.5270E-15 3.7074E-13
9.1910E-16 -1.3976E-15 5.3170E-14 -9.0448E-15 -1.7046E-16 -9.4558E-15
-1.4371E-15 2.0376E-15 -9.0448E-15 5.9090E-15 1.0297E-16 1.3769E-14
7.6634E-14 1.5270E-15 -1.7046E-16 1.0297E-16 1.1658E-13 2.4673E-14
-2.5752E-13 3.7074E-13 -9.4558E-15 1.3769E-14 2.4673E-14 2.5059E-12
# lat0 lon0 xBary yBary zBary JD0
0.479297 -142.340901 0.766321 0.005315 -0.631210 2456359.090898
# Heliocentric elements and errors
Epoch: 2456358.5000 = 2013/03/07
Mean Anomaly: 228.24310 +/- 0.027
Argument of Peri: 158.08163 +/- 0.022
Long of Asc Node: 203.41029 +/- 0.002
Inclination: 2.03634 +/- 0.000
Eccentricity: 0.17386860 +/- 0.0001
Semi-Major Axis: 48.60318361 +/- 0.0030
Time of Perihelion: 2501655.1791 +/- 11.7
Perihelion: 40.15261605 +/- 0.0048
Aphelion: 57.05375118 +/- 0.0054
Period (y) 338.8483 +/- 0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X -43.94079218 +/- 0.0008
Ecliptic Y -32.94219527 +/- 0.0006
Ecliptic Z 0.45412742 +/- 0.0000
Ecliptic XDOT 0.00149141 +/- 0.0000
Ecliptic YDOT -0.00156789 +/- 0.0000
Ecliptic ZDOT 0.00007223 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 54.91990843 +/- 0.0007
Geocenter to KBO 54.28559094 +/- 0.0010
# Hcoef: 6.48
The following table shows the complete astrometric record for 13GQ136. 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 (13GQ136) followed by the observatory code and reference code for the source of the astrometry.
2013 03 07.59012 14 21 50.657 -13 36 42.70 23.0r 13GQ136 568 C~1WkW 2013 03 07.64267 14 21 50.536 -13 36 42.20 24.1r 13GQ136 568 C~1WkW 2013 04 04.53472 14 20 32.252 -13 29 52.19 24.0r 13GQ136 568 C~1WkW 2013 04 07.39521 14 20 22.527 -13 29 01.69 23.6r 13GQ136 568 C~1WkW 2013 04 07.43903 14 20 22.386 -13 29 01.13 23.8r 13GQ136 568 C~1WkW 2013 04 08.42769 14 20 18.959 -13 28 43.50 24.2r 13GQ136 568 C~1WkW 2013 04 08.47292 14 20 18.813 -13 28 42.77 23.8r 13GQ136 568 C~1WkW 2013 04 09.37434 14 20 15.673 -13 28 26.58 23.5r 13GQ136 568 C~1WkW 2013 04 09.41746 14 20 15.531 -13 28 25.76 23.8r 13GQ136 568 C~1WkW 2013 04 09.46061 14 20 15.371 -13 28 24.99 23.5r 13GQ136 568 C~1WkW 2013 05 11.46227 14 18 18.918 -13 18 27.38 23.7r 13GQ136 568 C~1WkW 2013 06 12.35950 14 16 40.276 -13 10 06.14 23.8r 13GQ136 568 C~1WkW 2013 06 12.40439 14 16 40.164 -13 10 05.53 23.7r 13GQ136 568 C~1WkW 2013 07 04.31926 14 16 00.297 -13 06 46.08 24.2r 13GQ136 568 C~1WkW 2013 07 06.32704 14 15 58.093 -13 06 35.37 23.7r 13GQ136 568 C~1WkW 2013 08 02.25463 14 15 55.147 -13 06 27.40 23.9r 13GQ136 568 C~1WkW 2013 08 05.25536 14 15 57.922 -13 06 42.34 23.7r 13GQ136 568 C~1WkW 2014 02 24.58951 14 25 26.778 -13 52 55.12 23.6r 13GQ136 568 C~1WkW 2014 02 25.57248 14 25 25.409 -13 52 47.66 24.1r 13GQ136 568 C~1WkW 2014 02 28.52057 14 25 20.958 -13 52 22.95 24.4r 13GQ136 568 C~1WkW 2014 04 04.42334 14 23 51.083 -13 44 34.41 23.7r 13GQ136 568 C~1WkW 2014 04 04.46261 14 23 50.957 -13 44 33.79 23.8r 13GQ136 568 C~1WkW 2014 04 05.48108 14 23 47.554 -13 44 16.01 23.6r 13GQ136 568 C~1WkW 2014 04 05.53642 14 23 47.341 -13 44 15.29 23.9r 13GQ136 568 C~1WkW 2014 04 30.10956 14 22 18.85 -13 36 45.0 13GQ136 W84 C~2fc7 2014 04 30.17846 14 22 18.59 -13 36 43.7 24.2V 13GQ136 W84 C~2fc7 2014 05 01.09622 14 22 15.18 -13 36 26.6 13GQ136 W84 C~2fc7 2014 05 01.16603 14 22 14.94 -13 36 25.1 13GQ136 W84 C~2fc7 2014 05 22.44598 14 20 58.954 -13 30 01.85 23.5r 13GQ136 568 C~1WkW 2014 05 25.43819 14 20 49.063 -13 29 12.32 23.9r 13GQ136 568 C~1WkW 2015 01 26.64290 14 28 51.762 -14 08 16.51 23.9r 13GQ136 568 C~1WkW 2016 02 14.57372 14 32 12.571 -14 22 21.16 23.8r 13GQ136 568 C~2KOF 2016 02 14.63952 14 32 12.530 -14 22 20.86 24.1r 13GQ136 568 C~2KOF 2017 05 28.27970 14 30 38.193 -14 12 02.33 23.7r 13GQ136 568 C~2KOF 2017 05 28.34479 14 30 37.977 -14 12 01.27 23.6r 13GQ136 568 C~2KOF 2024 04 14.412330 14 57 20.381 -16 01 17.18 24.0G 13GQ136 G37 C~7zmB 2024 04 14.454030 14 57 20.215 -16 01 16.57 13GQ136 G37 C~7zmB
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 0.17 0.00 0.03
2 0.0001 0.00 0.07 0.00 -0.07
3 0.0765 0.00 -0.06 0.00 0.02
4 0.0843 0.00 -0.12 0.00 0.20
5 0.0845 0.00 0.06 0.00 -0.02
6 0.0872 0.00 -0.13 0.00 -0.03
7 0.0873 0.00 0.07 0.00 -0.10
8 0.0898 0.00 -0.09 0.00 -0.11
9 0.0899 0.00 0.08 0.00 -0.06
10 0.0900 0.00 -0.02 0.00 -0.07
11 0.1776 0.00 -0.05 0.00 0.03
12 0.2649 0.00 -0.06 0.00 -0.04
13 0.2651 0.00 -0.06 0.00 0.02
14 0.3251 0.00 0.06 0.00 0.02
15 0.3306 0.00 -0.17 0.00 0.03
16 0.4043 0.00 0.03 0.00 -0.04
17 0.4125 0.00 0.17 0.00 -0.05
18 0.9692 0.00 -0.06 0.00 -0.04
19 0.9719 0.00 -0.18 0.00 -0.12
20 0.9800 0.00 0.10 0.00 0.11
21 1.0755 0.00 -0.06 0.00 0.06
22 1.0756 0.00 0.06 0.00 0.01
23 1.0784 0.00 0.26 0.00 0.31
24 1.0786 0.00 -0.08 0.00 0.07
25 1.1458 0.00 0.04 0.00 -0.03
26 1.1460 0.00 0.03 0.00 -0.02
27 1.1485 0.00 -0.17 0.00 -0.14
28 1.1487 0.00 0.17 0.00 0.05
29 1.2070 0.00 0.15 0.00 0.14
30 1.2152 0.00 -0.01 0.00 0.03
31 1.8893 0.00 0.01 0.00 0.04
32 2.9404 0.00 -0.01 0.00 -0.13
33 2.9406 0.00 -0.07 0.00 -0.05
34 4.2237 0.00 -0.05 0.00 -0.07
35 4.2238 0.00 -0.04 0.00 -0.03
36 11.1042 0.00 0.15 0.00 0.04
37 11.1044 0.00 -0.11 0.00 -0.01
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.
13GQ136 quality flag:3 Type: CLASSICAL CLASSICAL CLASSICAL axisobj 48.452 48.452 48.452 ecceobj 0.178 0.178 0.178 incobj 2.041 2.041 2.041 qmin 39.548 39.545 39.550 qmax 58.502 58.445 58.491 amean 48.781 48.781 48.781 amin 48.332 48.349 48.352 amax 49.289 49.272 49.285 emean 0.174 0.174 0.174 emin 0.162 0.162 0.162 emax 0.187 0.186 0.187 imean 2.994 2.994 2.994 imin 2.680 2.681 2.680 imax 3.325 3.325 3.324 excite_mean 0.182 0.182 0.182 fracstop 1.000 1.000 1.000 cjmean 3.120 3.120 3.120 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 183.5 183.5 183.6 kozaiamp 179.9 179.9 179.9