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: 10LB136
# Created Thu Apr 25 01:13:18 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 171 observations of 171
# Arc: 13.43y
# First observation: 2010/06/04
# Last observation: 2023/11/08
# Chi-squared of fit: 82.35 DOF: 336 RMS: 0.12
# Min/Max residuals: -0.78 0.42
# Exact a, adot, b, bdot, g, gdot:
2.052217E-05 4.477422E-02 -4.370194E-06 -8.465326E-03 3.517602E-02 -2.891131E-03
# Covariance matrix:
9.0776E-14 -1.9624E-14 -6.5683E-15 2.9035E-15 -2.2489E-15 -2.0257E-14
-1.9624E-14 7.3943E-15 3.1046E-15 -1.3619E-15 2.4267E-15 9.5007E-15
-6.5683E-15 3.1046E-15 6.0909E-14 -5.7018E-15 9.5306E-16 4.2843E-15
2.9035E-15 -1.3619E-15 -5.7018E-15 7.6056E-16 -3.2188E-16 -1.8880E-15
-2.2489E-15 2.4267E-15 9.5306E-16 -3.2188E-16 1.3283E-14 2.2333E-15
-2.0257E-14 9.5007E-15 4.2843E-15 -1.8880E-15 2.2333E-15 1.3172E-14
# lat0 lon0 xBary yBary zBary JD0
9.602332 -87.559536 0.331107 0.159761 -0.944713 2455352.004966
# Heliocentric elements and errors
Epoch: 2455352.5000 = 2010/06/05
Mean Anomaly: 348.31825 +/- 0.001
Argument of Peri: 159.06099 +/- 0.001
Long of Asc Node: 132.54715 +/- 0.000
Inclination: 14.06644 +/- 0.000
Eccentricity: 0.26524308 +/- 0.0000
Semi-Major Axis: 39.44280177 +/- 0.0008
Time of Perihelion: 2458288.4959 +/- 2.5
Perihelion: 28.98087164 +/- 0.0007
Aphelion: 49.90473190 +/- 0.0011
Period (y) 247.7193 +/- 0.01
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X 0.90822810 +/- 0.0000
Ecliptic Y -28.97811126 +/- 0.0001
Ecliptic Z 4.74204776 +/- 0.0000
Ecliptic XDOT 0.00347850 +/- 0.0000
Ecliptic YDOT 0.00026630 +/- 0.0000
Ecliptic ZDOT -0.00068722 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 29.37763405 +/- 0.0001
Geocenter to KBO 28.42852844 +/- 0.0001
# Hcoef: 5.99
The following table shows the complete astrometric record for 10LB136. 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 (10LB136) followed by the observatory code and reference code for the source of the astrometry.
2010 06 04.50420 18 09 54.717 -13 48 57.49 20.5i 10LB136 F51 C~1w3i 2010 06 04.51533 18 09 54.643 -13 48 57.54 20.3i 10LB136 F51 C~1w3i 2010 06 06.52982 18 09 41.996 -13 48 57.35 20.8r 10LB136 F51 C~1w3i 2010 06 06.54257 18 09 41.912 -13 48 57.38 21.1r 10LB136 F51 C~1w3i 2010 07 20.29036 18 04 58.835 -13 54 26.53 20.9G 10LB136 F51 C~2jgo 2010 07 20.30221 18 04 58.769 -13 54 26.64 20.9G 10LB136 F51 C~2jgo 2010 09 02.23013 18 02 14.324 -14 08 40.95 21.4G 10LB136 F51 C~2jgo 2010 09 02.24107 18 02 14.311 -14 08 41.18 21.2G 10LB136 F51 C~2jgo 2011 05 23.50329 18 21 44.121 -14 14 44.09 20.8G 10LB136 F51 C~2jgo 2011 05 23.51498 18 21 44.061 -14 14 44.14 20.5G 10LB136 F51 C~2jgo 2011 05 29.54469 18 21 10.789 -14 14 31.53 22.1g 10LB136 F51 C~1w3i 2011 05 29.56037 18 21 10.665 -14 14 31.50 22.0g 10LB136 F51 C~1w3i 2011 06 02.45111 18 20 47.819 -14 14 29.78 21.7g 10LB136 F51 C~1w3i 2011 06 02.46220 18 20 47.754 -14 14 29.71 21.7g 10LB136 F51 C~1w3i 2011 06 02.47408 18 20 47.688 -14 14 29.91 20.8r 10LB136 F51 C~1w3i 2011 06 02.48464 18 20 47.610 -14 14 29.92 20.8r 10LB136 F51 C~1w3i 2012 08 08.34531 18 24 32.892 -14 51 24.34 21.2g 10LB136 F51 C~1w3i 2012 08 08.35561 18 24 32.843 -14 51 24.44 21.2g 10LB136 F51 C~1w3i 2012 08 08.36658 18 24 32.798 -14 51 24.78 21.1r 10LB136 F51 C~1w3i 2012 08 08.37669 18 24 32.745 -14 51 25.00 20.8r 10LB136 F51 C~1w3i 2013 07 01.45174 18 39 11.797 -15 04 06.19 20.5G 10LB136 F51 C~2jgo 2013 07 01.46235 18 39 11.724 -15 04 06.25 20.6G 10LB136 F51 C~2jgo 2013 07 04.39985 18 38 51.912 -15 04 43.14 21.6g 10LB136 F51 C~1w3i 2016 05 16.53928 19 16 19.076 -15 53 46.46 20.9G 10LB136 F51 C~2jgo 2016 05 16.55093 19 16 19.041 -15 53 46.49 20.8G 10LB136 F51 C~2jgo 2016 05 16.57418 19 16 18.958 -15 53 46.62 20.8G 10LB136 F51 C~2jgo 2016 08 07.34002 19 08 12.886 -16 12 47.09 10LB136 F51 C~2jgo 2016 08 07.35213 19 08 12.818 -16 12 47.24 10LB136 F51 C~2jgo 2016 08 07.36423 19 08 12.752 -16 12 47.42 20.7G 10LB136 F51 C~2jgo 2016 08 07.37639 19 08 12.675 -16 12 47.73 20.7G 10LB136 F51 C~2jgo 2016 08 31.28546 19 06 24.164 -16 21 37.99 20.6G 10LB136 F51 C~2jgo 2016 08 31.29735 19 06 24.124 -16 21 38.24 20.7G 10LB136 F51 C~2jgo 2016 08 31.30922 19 06 24.079 -16 21 38.50 20.9G 10LB136 F51 C~2jgo 2016 08 31.32108 19 06 24.042 -16 21 38.83 20.9G 10LB136 F51 C~2jgo 2017 05 04.57628 19 27 44.965 -16 07 28.36 21.0G 10LB136 F51 C~2jgo 2017 05 04.58192 19 27 44.961 -16 07 28.41 20.9G 10LB136 F51 C~2jgo 2017 05 04.58753 19 27 44.952 -16 07 28.38 20.8G 10LB136 F51 C~2jgo 2017 05 04.59314 19 27 44.940 -16 07 28.40 20.9G 10LB136 F51 C~2jgo 2017 06 21.52297 19 24 23.783 -16 12 38.76 20.5G 10LB136 F51 C~2jgo 2017 06 21.53375 19 24 23.710 -16 12 39.03 20.7G 10LB136 F51 C~2jgo 2017 06 21.54454 19 24 23.640 -16 12 39.15 20.7G 10LB136 F51 C~2jgo 2018 05 21.57156 19 38 02.829 -16 19 17.24 20.8G 10LB136 F51 C~2jgo 2018 05 21.58145 19 38 02.794 -16 19 17.22 20.8G 10LB136 F51 C~2jgo 2018 05 21.59133 19 38 02.759 -16 19 17.23 20.7G 10LB136 F51 C~2jgo 2018 05 21.60125 19 38 02.727 -16 19 17.29 20.8G 10LB136 F51 C~2jgo 2020 08 15.43851 19 52 01.81 -17 04 27.0 20.3R 10LB136 F65 C~43wn 2020 08 15.44148 19 52 01.79 -17 04 27.2 20.4R 10LB136 F65 C~43wn 2020 08 15.44444 19 52 01.77 -17 04 27.3 20.4R 10LB136 F65 C~43wn 2021 05 14.560354 20 11 17.670 -16 39 55.50 20.9w 10LB136 F51 C~4mz6 2021 05 14.571435 20 11 17.651 -16 39 55.64 20.8w 10LB136 F51 C~4mz6 2021 05 14.581813 20 11 17.640 -16 39 55.63 20.8w 10LB136 F51 C~4mz6 2021 05 23.556679 20 11 00.120 -16 40 50.24 20.9w 10LB136 F51 C~4qDg 2021 05 23.563375 20 11 00.105 -16 40 50.16 20.8w 10LB136 F51 C~4qDg 2021 05 23.570146 20 11 00.089 -16 40 50.19 20.8w 10LB136 F51 C~4qDg 2021 05 23.576953 20 11 00.069 -16 40 50.35 20.8w 10LB136 F51 C~4qDg 2021 05 24.559145 20 10 57.545 -16 40 58.53 20.3i 10LB136 F51 C~4qDg 2021 05 24.565803 20 10 57.519 -16 40 58.80 20.4i 10LB136 F51 C~4qDg 2021 05 24.572389 20 10 57.506 -16 40 58.72 20.3i 10LB136 F51 C~4qDg 2021 05 24.578953 20 10 57.486 -16 40 58.84 20.2i 10LB136 F51 C~4qDg 2021 06 03.522655 20 10 25.440 -16 42 45.87 20.6w 10LB136 F51 C~4qDg 2021 06 03.533685 20 10 25.394 -16 42 46.19 20.8w 10LB136 F51 C~4qDg 2021 06 03.544707 20 10 25.347 -16 42 46.30 20.7w 10LB136 F51 C~4qDg 2021 06 03.555736 20 10 25.300 -16 42 46.41 20.7w 10LB136 F51 C~4qDg 2021 06 05.580345 20 10 17.407 -16 43 13.40 20.6w 10LB136 F51 C~4qDg 2021 06 05.586638 20 10 17.381 -16 43 13.49 20.6w 10LB136 F51 C~4qDg 2021 06 05.592556 20 10 17.354 -16 43 13.52 20.6w 10LB136 F51 C~4qDg 2021 06 05.598623 20 10 17.334 -16 43 13.75 20.6w 10LB136 F51 C~4qDg 2021 06 11.506315 20 09 51.836 -16 44 42.16 21.3w 10LB136 F51 C~4qDg 2021 06 11.517316 20 09 51.838 -16 44 42.13 21.4w 10LB136 F51 C~4qDg 2021 06 11.528323 20 09 51.735 -16 44 42.58 21.3w 10LB136 F51 C~4qDg 2021 06 18.472606 20 09 17.588 -16 46 43.64 20.8w 10LB136 F51 C~4qDg 2021 06 18.484034 20 09 17.529 -16 46 43.89 20.6w 10LB136 F51 C~4qDg 2021 06 18.493838 20 09 17.479 -16 46 44.06 20.7w 10LB136 F51 C~4qDg 2021 07 09.309110 20 07 14.543 -16 54 19.55 20.8G 10LB136 G37 C~4urh 2021 07 09.355840 20 07 14.235 -16 54 20.82 10LB136 G37 C~4urh 2021 08 03.368648 20 04 29.621 -17 05 20.40 20.4w 10LB136 F51 C~4wE9 2021 08 03.377943 20 04 29.554 -17 05 20.74 20.4w 10LB136 F51 C~4wE9 2021 08 03.387222 20 04 29.489 -17 05 21.00 20.4w 10LB136 F51 C~4wE9 2021 08 03.396491 20 04 29.428 -17 05 21.22 20.5w 10LB136 F51 C~4wE9 2021 08 10.395854 20 03 45.077 -17 08 32.41 20.7w 10LB136 F51 C~4yKh 2021 08 10.404334 20 03 45.025 -17 08 32.48 20.6w 10LB136 F51 C~4yKh 2021 08 10.412830 20 03 44.966 -17 08 32.77 20.6w 10LB136 F51 C~4yKh 2021 08 10.421323 20 03 44.911 -17 08 33.04 20.6w 10LB136 F51 C~4yKh 2021 09 04.314955 20 01 32.126 -17 19 14.78 20.1w 10LB136 F51 C~4yKh 2021 09 04.322428 20 01 32.090 -17 19 14.76 20.2w 10LB136 F51 C~4yKh 2021 09 04.330235 20 01 32.058 -17 19 14.98 20.0w 10LB136 F51 C~4yKh 2021 09 04.337905 20 01 32.005 -17 19 15.53 20.3w 10LB136 F51 C~4yKh 2021 09 08.285476 20 01 16.025 -17 20 46.74 20.7w 10LB136 F51 C~52Lu 2021 09 08.293756 20 01 15.990 -17 20 46.89 20.8w 10LB136 F51 C~52Lu 2021 09 08.301917 20 01 15.959 -17 20 47.09 20.7w 10LB136 F51 C~52Lu 2021 09 08.310082 20 01 15.921 -17 20 47.20 20.8w 10LB136 F51 C~52Lu 2022 05 25.522895 20 21 54.293 -16 43 43.21 20.6w 10LB136 F52 C~5ffu 2022 05 25.523524 20 21 54.293 -16 43 43.26 20.8w 10LB136 F52 C~5ffu 2022 05 25.534400 20 21 54.271 -16 43 43.31 20.6w 10LB136 F52 C~5ffu 2022 05 25.535030 20 21 54.268 -16 43 43.41 20.7w 10LB136 F52 C~5ffu 2022 05 25.545917 20 21 54.233 -16 43 43.39 20.5w 10LB136 F52 C~5ffu 2022 05 25.546546 20 21 54.239 -16 43 43.45 20.9w 10LB136 F52 C~5ffu 2022 05 25.557462 20 21 54.197 -16 43 43.51 20.5w 10LB136 F52 C~5ffu 2022 05 25.558100 20 21 54.204 -16 43 43.54 20.8w 10LB136 F52 C~5ffu 2022 05 31.526691 20 21 37.827 -16 44 48.24 20.8w 10LB136 F52 C~5ffu 2022 05 31.536234 20 21 37.794 -16 44 48.38 20.7w 10LB136 F52 C~5ffu 2022 05 31.545784 20 21 37.764 -16 44 48.49 20.7w 10LB136 F52 C~5ffu 2022 05 31.555328 20 21 37.732 -16 44 48.56 20.8w 10LB136 F52 C~5ffu 2022 07 21.395094 20 17 08.059 -17 03 00.60 20.6w 10LB136 F52 C~6hK8 2022 07 21.405343 20 17 07.971 -17 03 00.91 20.4w 10LB136 F52 C~6hK8 2022 07 21.430122 20 17 07.823 -17 03 01.63 20.5w 10LB136 F52 C~6hK8 2022 07 21.440299 20 17 07.747 -17 03 01.72 20.6w 10LB136 F52 C~6hK8 2022 08 01.373821 20 15 55.547 -17 08 11.26 20.5w 10LB136 F52 C~5ils 2022 08 01.384630 20 15 55.469 -17 08 11.60 20.6w 10LB136 F52 C~5ils 2022 08 01.395458 20 15 55.400 -17 08 11.92 20.5w 10LB136 F52 C~5ils 2022 08 01.406258 20 15 55.327 -17 08 12.19 20.5w 10LB136 F52 C~5ils 2022 09 01.253084 20 12 54.050 -17 22 22.03 20.6w 10LB136 F52 C~5lcw 2022 09 01.265422 20 12 53.989 -17 22 22.41 20.7w 10LB136 F52 C~5lcw 2022 09 01.277759 20 12 53.930 -17 22 22.74 20.6w 10LB136 F52 C~5lcw 2022 09 01.290164 20 12 53.868 -17 22 22.86 20.7w 10LB136 F52 C~5lcw 2022 09 15.252803 20 11 56.340 -17 27 49.02 20.7w 10LB136 F52 C~5o9O 2022 09 15.263690 20 11 56.303 -17 27 49.20 20.6w 10LB136 F52 C~5o9O 2022 09 15.274549 20 11 56.258 -17 27 49.40 20.6w 10LB136 F52 C~5o9O 2022 09 15.285443 20 11 56.227 -17 27 49.66 20.7w 10LB136 F52 C~5o9O 2022 09 25.245382 20 11 28.685 -17 31 04.96 20.7w 10LB136 F52 C~5o9O 2022 09 25.257507 20 11 28.659 -17 31 05.16 20.8w 10LB136 F52 C~5o9O 2022 09 25.269698 20 11 28.625 -17 31 05.33 20.7w 10LB136 F52 C~5o9O 2022 09 25.281911 20 11 28.603 -17 31 05.59 20.8w 10LB136 F52 C~5o9O 2022 09 29.246029 20 11 21.162 -17 32 13.08 20.8w 10LB136 F51 C~5qt5 2022 09 29.257200 20 11 21.134 -17 32 13.20 20.8w 10LB136 F51 C~5qt5 2022 09 29.268248 20 11 21.112 -17 32 13.48 20.9w 10LB136 F51 C~5qt5 2022 09 29.279476 20 11 21.098 -17 32 13.52 20.8w 10LB136 F51 C~5qt5 2023 06 14.572525 20 31 46.151 -16 48 57.38 20.8w 10LB136 F51 C~6pk3 2023 06 14.581899 20 31 46.099 -16 48 57.66 20.7w 10LB136 F51 C~6pk3 2023 06 14.591248 20 31 46.067 -16 48 57.86 20.8w 10LB136 F51 C~6pk3 2023 06 14.600598 20 31 46.014 -16 48 57.92 20.8w 10LB136 F51 C~6pk3 2023 06 18.510355 20 31 28.599 -16 50 14.96 21.1w 10LB136 F51 C~6r51 2023 06 18.532378 20 31 28.499 -16 50 15.31 21.5w 10LB136 F51 C~6r51 2023 06 18.543370 20 31 28.392 -16 50 15.86 21.3w 10LB136 F51 C~6r51 2023 06 23.465666 20 31 04.445 -16 52 01.37 20.8w 10LB136 F51 C~6r51 2023 06 23.477428 20 31 04.386 -16 52 01.62 20.8w 10LB136 F51 C~6r51 2023 06 23.489186 20 31 04.313 -16 52 01.56 20.9w 10LB136 F51 C~6r51 2023 06 23.500966 20 31 04.267 -16 52 01.78 20.7w 10LB136 F51 C~6r51 2023 06 27.504314 20 30 43.262 -16 53 34.16 20.7w 10LB136 F52 C~6r51 2023 06 27.515817 20 30 43.194 -16 53 34.33 20.7w 10LB136 F52 C~6r51 2023 06 27.527319 20 30 43.129 -16 53 34.65 20.9w 10LB136 F52 C~6r51 2023 06 27.538822 20 30 43.061 -16 53 34.81 20.8w 10LB136 F52 C~6r51 2023 07 16.391440 20 28 50.586 -17 01 50.02 20.4w 10LB136 F52 C~6whK 2023 07 16.401566 20 28 50.528 -17 01 50.20 20.5w 10LB136 F52 C~6whK 2023 07 16.411709 20 28 50.451 -17 01 50.37 20.5w 10LB136 F52 C~6whK 2023 08 18.301012 20 25 18.609 -17 17 59.77 20.7w 10LB136 F51 C~77nO 2023 08 18.310676 20 25 18.544 -17 17 59.99 20.9w 10LB136 F51 C~77nO 2023 08 18.320325 20 25 18.491 -17 18 00.25 20.8w 10LB136 F51 C~77nO 2023 08 18.329983 20 25 18.433 -17 18 00.53 20.8w 10LB136 F51 C~77nO 2023 08 21.322637 20 25 00.659 -17 19 26.45 20.8w 10LB136 F52 C~77nO 2023 08 21.332813 20 25 00.600 -17 19 26.71 20.8w 10LB136 F52 C~77nO 2023 08 21.343020 20 25 00.529 -17 19 27.03 20.7w 10LB136 F52 C~77nO 2023 08 21.353231 20 25 00.473 -17 19 27.31 20.7w 10LB136 F52 C~77nO 2023 09 03.245265 20 23 50.926 -17 25 17.85 21.0w 10LB136 F52 C~795l 2023 09 03.254777 20 23 50.873 -17 25 18.16 20.9w 10LB136 F52 C~795l 2023 09 03.264293 20 23 50.831 -17 25 18.35 21.0w 10LB136 F52 C~795l 2023 09 03.273816 20 23 50.774 -17 25 18.59 20.9w 10LB136 F52 C~795l 2023 09 07.811216 20 23 29.505 -17 27 12.62 21.0V 10LB136 M49 B~7Mfk 2023 09 07.899703 20 23 29.122 -17 27 14.06 21.2V 10LB136 M49 B~7Mfk 2023 09 07.987232 20 23 28.699 -17 27 16.93 20.8V 10LB136 M49 B~7Mfk 2023 09 14.260777 20 23 02.897 -17 29 43.71 20.9w 10LB136 F51 C~7Aj2 2023 09 14.271138 20 23 02.845 -17 29 43.91 20.9w 10LB136 F51 C~7Aj2 2023 09 14.281507 20 23 02.812 -17 29 44.24 20.9w 10LB136 F51 C~7Aj2 2023 09 14.291873 20 23 02.766 -17 29 44.34 20.9w 10LB136 F51 C~7Aj2 2023 09 19.260802 20 22 45.328 -17 31 31.27 20.9w 10LB136 F51 C~7Aj2 2023 09 19.272428 20 22 45.283 -17 31 31.61 21.0w 10LB136 F51 C~7Aj2 2023 09 19.284029 20 22 45.237 -17 31 32.02 20.9w 10LB136 F51 C~7Aj2 2023 11 08.209326 20 22 49.672 -17 39 33.20 20.8w 10LB136 F51 C~7R55 2023 11 08.213906 20 22 49.695 -17 39 33.06 21.0w 10LB136 F51 C~7R55 2023 11 08.218531 20 22 49.709 -17 39 33.30 21.0w 10LB136 F51 C~7R55 2023 11 08.223104 20 22 49.720 -17 39 33.14 20.8w 10LB136 F51 C~7R55
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 -0.09 0.00 0.12
2 0.0000 0.00 -0.13 0.00 0.06
3 0.0055 0.00 0.06 0.00 0.07
4 0.0056 0.00 0.03 0.00 0.04
5 0.1254 0.00 -0.00 0.00 0.09
6 0.1254 0.00 0.06 0.00 0.15
7 0.2457 0.00 0.12 0.00 0.14
8 0.2457 0.00 0.14 0.00 0.16
9 0.9665 0.00 -0.18 0.00 -0.06
10 0.9665 0.00 -0.13 0.00 -0.14
11 0.9830 0.00 0.33 0.00 0.09
12 0.9830 0.00 -0.15 0.00 0.10
13 0.9937 0.00 -0.08 0.00 0.03
14 0.9937 0.00 -0.04 0.00 0.11
15 0.9938 0.00 0.06 0.00 -0.09
16 0.9938 0.00 -0.14 0.00 -0.10
17 2.1789 0.00 -0.03 0.00 -0.12
18 2.1789 0.00 -0.03 0.00 -0.01
19 2.1790 0.00 0.08 0.00 -0.14
20 2.1790 0.00 0.01 0.00 -0.16
21 3.0745 0.00 0.05 0.00 0.00
22 3.0745 0.00 0.05 0.00 0.07
23 3.0825 0.00 0.31 0.00 -0.21
24 5.9494 0.00 -0.07 0.00 -0.02
25 5.9495 0.00 0.02 0.00 -0.03
26 5.9495 0.00 -0.01 0.00 -0.13
27 6.1761 0.00 -0.08 0.00 -0.24
28 6.1762 0.00 -0.05 0.00 -0.12
29 6.1762 0.00 0.00 0.00 -0.03
30 6.1762 0.00 -0.10 0.00 -0.08
31 6.2417 0.00 0.01 0.00 -0.04
32 6.2417 0.00 0.02 0.00 -0.04
33 6.2418 0.00 -0.05 0.00 -0.04
34 6.2418 0.00 -0.00 0.00 -0.11
35 6.9160 0.00 -0.05 0.00 -0.01
36 6.9160 0.00 0.03 0.00 -0.07
37 6.9160 0.00 0.03 0.00 -0.05
38 6.9161 0.00 -0.01 0.00 -0.08
39 7.0473 0.00 0.05 0.00 0.09
40 7.0473 0.00 -0.01 0.00 -0.02
41 7.0473 0.00 -0.04 0.00 0.01
42 7.9619 0.00 0.00 0.00 -0.10
43 7.9619 0.00 -0.02 0.00 -0.03
44 7.9619 0.00 -0.04 0.00 0.01
45 7.9619 0.00 -0.02 0.00 0.00
46 10.1983 0.00 -0.11 0.00 0.21
47 10.1983 0.00 -0.15 0.00 0.09
48 10.1983 0.00 -0.19 0.00 0.06
49 10.9433 0.00 0.02 0.00 0.10
50 10.9434 0.00 -0.02 0.00 0.01
51 10.9434 0.00 0.05 0.00 0.06
52 10.9680 0.00 -0.07 0.00 0.05
53 10.9680 0.00 -0.03 0.00 0.19
54 10.9680 0.00 -0.00 0.00 0.21
55 10.9680 0.00 -0.03 0.00 0.11
56 10.9707 0.00 0.06 0.00 0.14
57 10.9707 0.00 -0.05 0.00 -0.07
58 10.9708 0.00 0.03 0.00 0.07
59 10.9708 0.00 -0.00 0.00 0.01
60 10.9980 0.00 0.05 0.00 0.09
61 10.9980 0.00 0.01 0.00 -0.08
62 10.9981 0.00 -0.05 0.00 -0.05
63 10.9981 0.00 -0.10 0.00 -0.02
64 11.0036 0.00 -0.00 0.00 0.01
65 11.0036 0.00 0.00 0.00 0.01
66 11.0037 0.00 -0.04 0.00 0.06
67 11.0037 0.00 0.04 0.00 -0.09
68 11.0199 0.00 -0.39 0.00 -0.05
69 11.0199 0.00 0.42 0.00 0.15
70 11.0199 0.00 -0.35 0.00 -0.12
71 11.0389 0.00 -0.02 0.00 0.01
72 11.0390 0.00 0.01 0.00 -0.02
73 11.0390 0.00 0.04 0.00 -0.01
74 11.0960 0.00 0.03 0.00 0.03
75 11.0961 0.00 -0.00 0.00 -0.09
76 11.1646 0.00 0.12 0.00 0.07
77 11.1646 0.00 0.03 0.00 -0.02
78 11.1646 0.00 -0.03 0.00 -0.02
79 11.1647 0.00 -0.02 0.00 0.01
80 11.1838 0.00 0.04 0.00 -0.09
81 11.1838 0.00 0.06 0.00 0.07
82 11.1839 0.00 -0.02 0.00 0.01
83 11.1839 0.00 -0.04 0.00 -0.03
84 11.2520 0.00 0.08 0.00 0.03
85 11.2521 0.00 0.03 0.00 0.23
86 11.2521 0.00 0.07 0.00 0.20
87 11.2521 0.00 -0.22 0.00 -0.17
88 11.2629 0.00 0.08 0.00 -0.03
89 11.2629 0.00 0.05 0.00 0.01
90 11.2630 0.00 0.07 0.00 -0.01
91 11.2630 0.00 -0.02 0.00 0.07
92 11.9727 0.00 -0.02 0.00 -0.02
93 11.9727 0.00 0.00 0.00 -0.06
94 11.9727 0.00 0.08 0.00 -0.01
95 11.9727 0.00 0.06 0.00 -0.10
96 11.9727 0.00 -0.06 0.00 0.02
97 11.9727 0.00 0.05 0.00 -0.03
98 11.9728 0.00 -0.17 0.00 0.02
99 11.9728 0.00 -0.04 0.00 -0.01
100 11.9891 0.00 0.01 0.00 0.05
101 11.9891 0.00 -0.02 0.00 0.03
102 11.9892 0.00 -0.01 0.00 0.04
103 11.9892 0.00 -0.03 0.00 0.08
104 12.1284 0.00 0.14 0.00 0.02
105 12.1284 0.00 -0.14 0.00 -0.01
106 12.1285 0.00 0.14 0.00 -0.03
107 12.1285 0.00 0.02 0.00 0.16
108 12.1584 0.00 0.07 0.00 0.03
109 12.1585 0.00 -0.02 0.00 -0.00
110 12.1585 0.00 0.03 0.00 -0.01
111 12.1585 0.00 0.02 0.00 0.03
112 12.2430 0.00 0.05 0.00 -0.02
113 12.2430 0.00 0.05 0.00 -0.09
114 12.2430 0.00 0.08 0.00 -0.10
115 12.2431 0.00 0.07 0.00 0.09
116 12.2813 0.00 0.06 0.00 0.00
117 12.2813 0.00 0.08 0.00 0.06
118 12.2814 0.00 -0.03 0.00 0.09
119 12.2814 0.00 0.08 0.00 0.06
120 12.3087 0.00 0.07 0.00 -0.04
121 12.3087 0.00 0.09 0.00 -0.03
122 12.3087 0.00 -0.00 0.00 0.02
123 12.3088 0.00 0.08 0.00 -0.02
124 12.3196 0.00 0.07 0.00 0.01
125 12.3197 0.00 -0.06 0.00 0.08
126 12.3197 0.00 -0.10 0.00 -0.03
127 12.3197 0.00 -0.02 0.00 0.12
128 13.0269 0.00 0.05 0.00 0.04
129 13.0269 0.00 -0.11 0.00 -0.06
130 13.0269 0.00 0.03 0.00 -0.09
131 13.0270 0.00 -0.15 0.00 0.03
132 13.0377 0.00 0.34 0.00 0.04
133 13.0377 0.00 0.42 0.00 0.14
134 13.0378 0.00 -0.40 0.00 -0.18
135 13.0512 0.00 0.07 0.00 -0.25
136 13.0513 0.00 0.10 0.00 -0.23
137 13.0513 0.00 -0.08 0.00 0.09
138 13.0513 0.00 0.15 0.00 0.14
139 13.0623 0.00 0.08 0.00 -0.09
140 13.0623 0.00 0.01 0.00 0.01
141 13.0623 0.00 -0.01 0.00 -0.03
142 13.0624 0.00 -0.08 0.00 0.08
143 13.1140 0.00 -0.09 0.00 -0.02
144 13.1140 0.00 0.03 0.00 0.09
145 13.1141 0.00 -0.13 0.00 0.21
146 13.2041 0.00 0.01 0.00 -0.07
147 13.2041 0.00 -0.07 0.00 -0.01
148 13.2042 0.00 0.02 0.00 0.01
149 13.2042 0.00 0.04 0.00 0.01
150 13.2124 0.00 0.07 0.00 -0.01
151 13.2124 0.00 0.10 0.00 0.02
152 13.2124 0.00 -0.05 0.00 -0.01
153 13.2125 0.00 0.03 0.00 0.00
154 13.2478 0.00 0.15 0.00 0.04
155 13.2478 0.00 0.07 0.00 -0.03
156 13.2478 0.00 0.15 0.00 0.03
157 13.2478 0.00 0.01 0.00 0.04
158 13.2603 0.00 -0.74 0.00 -0.38
159 13.2605 0.00 -0.41 0.00 0.34
160 13.2607 0.00 -0.78 0.00 -0.42
161 13.2779 0.00 0.14 0.00 -0.01
162 13.2779 0.00 -0.03 0.00 0.02
163 13.2780 0.00 0.08 0.00 -0.08
164 13.2780 0.00 0.00 0.00 0.06
165 13.2916 0.00 0.13 0.00 0.04
166 13.2916 0.00 0.04 0.00 -0.06
167 13.2917 0.00 -0.07 0.00 -0.23
168 13.4284 0.00 -0.04 0.00 -0.08
169 13.4284 0.00 0.07 0.00 0.05
170 13.4284 0.00 0.04 0.00 -0.20
171 13.4284 0.00 -0.03 0.00 -0.06
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.
10LB136 quality flag:3 Type: 3:2E 3:2E 3:2E axisobj 39.084 39.084 39.084 ecceobj 0.260 0.260 0.260 incobj 14.081 14.081 14.081 qmin 27.797 27.821 27.839 qmax 51.764 51.842 51.728 amean 39.455 39.455 39.455 amin 38.951 38.951 38.957 amax 40.053 40.087 40.027 emean 0.271 0.271 0.271 emin 0.251 0.251 0.251 emax 0.295 0.295 0.294 imean 12.286 12.276 12.284 imin 11.222 11.191 11.164 imax 13.052 13.067 13.077 excite_mean 0.345 0.345 0.345 fracstop 1.000 1.000 1.000 cjmean 2.916 2.916 2.916 libcent 0 180.5 179.5 179.4 libamp 0 102.3 102.0 101.1 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 203.0 201.8 199.8 kozaiamp 180.0 180.0 180.0