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: 11UF411
# Created Fri Nov 22 02:09:14 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 39 observations of 39
# Arc: 9.28y
# First observation: 2011/08/30
# Last observation: 2020/12/09
# Chi-squared of fit: 23.17 DOF: 72 RMS: 0.14
# Min/Max residuals: -0.48 0.30
# Exact a, adot, b, bdot, g, gdot:
1.635741E-05 2.995170E-02 -1.184311E-06 -1.915705E-03 2.726684E-02 -7.846903E-03
# Covariance matrix:
1.7840E-13 -7.9349E-14 -3.9240E-15 5.6360E-15 1.3362E-13 -3.0160E-13
-7.9349E-14 2.9295E-13 5.7419E-15 -2.0331E-14 2.4611E-14 1.1023E-12
-3.9240E-15 5.7419E-15 4.5136E-14 -6.7995E-15 -2.5154E-15 2.2440E-14
5.6360E-15 -2.0331E-14 -6.7995E-15 6.0934E-15 -1.1391E-15 -7.7831E-14
1.3362E-13 2.4611E-14 -2.5154E-15 -1.1391E-15 1.7222E-13 6.6582E-14
-3.0160E-13 1.1023E-12 2.2440E-14 -7.7831E-14 6.6582E-14 4.2189E-12
# lat0 lon0 xBary yBary zBary JD0
4.718311 30.880231 0.818325 0.048197 -0.584338 2455803.999576
# Heliocentric elements and errors
Epoch: 2455804.5000 = 2011/08/31
Mean Anomaly: 325.67442 +/- 0.006
Argument of Peri: 194.93617 +/- 0.013
Long of Asc Node: 261.83447 +/- 0.001
Inclination: 5.86640 +/- 0.000
Eccentricity: 0.34985773 +/- 0.0001
Semi-Major Axis: 48.20390723 +/- 0.0041
Time of Perihelion: 2467460.1681 +/- 14.3
Perihelion: 31.33939783 +/- 0.0040
Aphelion: 65.06841663 +/- 0.0063
Period (y) 334.6814 +/- 0.04
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X 32.29560014 +/- 0.0005
Ecliptic Y 18.35909082 +/- 0.0003
Ecliptic Z 3.01672206 +/- 0.0000
Ecliptic XDOT -0.00220705 +/- 0.0000
Ecliptic YDOT 0.00219161 +/- 0.0000
Ecliptic ZDOT -0.00025645 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 37.27165204 +/- 0.0004
Geocenter to KBO 36.67477162 +/- 0.0006
# Hcoef: 8.36
The following table shows the complete astrometric record for 11UF411. 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 (11UF411) followed by the observatory code and reference code for the source of the astrometry.
2011 08 30.49881 01 48 09.738 +16 11 47.88 24.3r 11UF411 568 C~1C6N 2011 08 30.54538 01 48 09.603 +16 11 47.29 23.8r 11UF411 568 C~1C6N 2011 08 30.59180 01 48 09.460 +16 11 46.88 23.9r 11UF411 568 C~1C6N 2011 09 05.59321 01 47 51.522 +16 10 40.68 11UF411 568 C~1C6N 2011 10 25.33804 01 44 03.067 +15 51 22.66 11UF411 568 C~1C6N 2011 10 25.33804 01 44 03.03 +15 51 22.9 23.7r 11UF411 568 C~3j8g 2011 10 25.38684 01 44 02.808 +15 51 21.25 24.1r 11UF411 568 C~1C6N 2011 10 25.38684 01 44 02.78 +15 51 21.4 24.5r 11UF411 568 C~3j8g 2011 10 25.43648 01 44 02.541 +15 51 19.76 24.0r 11UF411 568 C~1C6N 2011 10 25.44205 01 44 02.517 +15 51 19.50 23.6r 11UF411 568 C~1C6N 2011 10 25.44723 01 44 02.478 +15 51 19.44 11UF411 568 C~1C6N 2011 10 25.45234 01 44 02.458 +15 51 19.27 24.0r 11UF411 568 C~1C6N 2011 10 25.45781 01 44 02.422 +15 51 19.03 23.8r 11UF411 568 C~1C6N 2011 10 25.45781 01 44 02.40 +15 51 19.2 23.6r 11UF411 568 C~3j8g 2011 10 26.28698 01 43 58.114 +15 50 53.51 24.1r 11UF411 568 C~1C6N 2011 10 26.33962 01 43 57.839 +15 50 52.04 11UF411 568 C~1C6N 2011 10 26.33962 01 43 57.81 +15 50 52.2 23.6r 11UF411 568 C~3j8g 2011 10 26.38266 01 43 57.604 +15 50 50.89 11UF411 568 C~1C6N 2011 10 26.39884 01 43 57.522 +15 50 50.39 24.0r 11UF411 568 C~1C6N 2011 10 26.40555 01 43 57.486 +15 50 50.09 24.0r 11UF411 568 C~1C6N 2011 10 31.28562 01 43 32.171 +15 48 19.43 23.0r 11UF411 568 C~1C6N 2011 10 31.38837 01 43 31.631 +15 48 16.45 24.1r 11UF411 568 C~1C6N 2011 10 31.41441 01 43 31.495 +15 48 15.57 23.8r 11UF411 568 C~1C6N 2011 10 31.44399 01 43 31.339 +15 48 14.52 23.8r 11UF411 568 C~1C6N 2011 11 24.23661 01 41 38.898 +15 36 08.50 23.9r 11UF411 568 C~1C6N 2011 11 26.45630 01 41 29.873 +15 35 04.81 24.3r 11UF411 568 C~1C6N 2012 01 25.29229 01 40 15.192 +15 19 37.78 24.6r 11UF411 568 C~1C6N 2012 01 26.27710 01 40 17.096 +15 19 39.55 24.6r 11UF411 568 C~1C6N 2012 02 28.22088 01 42 15.664 +15 26 01.48 11UF411 568 C~1C6N 2012 08 23.57113 01 55 19.848 +16 42 49.83 24.0r 11UF411 568 C~1C6N 2012 08 24.45714 01 55 18.037 +16 42 45.49 11UF411 568 C~1C6N 2012 10 21.33604 01 51 17.973 +16 24 04.60 23.6r 11UF411 568 C~1C6N 2012 10 21.36172 01 51 17.835 +16 24 03.85 23.7r 11UF411 568 C~1C6N 2012 10 21.38781 01 51 17.697 +16 24 03.06 24.0r 11UF411 568 C~1C6N 2013 02 03.29696 01 47 19.719 +15 50 33.48 24.0r 11UF411 568 C~1C6N 2019 10 26.415970 02 44 04.263 +19 44 40.16 23.5G 11UF411 G37 C~3chz 2019 10 26.501140 02 44 03.769 +19 44 38.01 11UF411 G37 C~3chz 2020 12 09.116710 02 48 13.593 +19 50 36.74 24.1G 11UF411 G37 C~4U7j 2020 12 09.171370 02 48 13.338 +19 50 35.47 11UF411 G37 C~4U7j
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 0.20 0.00 0.09
2 0.0001 0.00 0.15 0.00 -0.07
3 0.0003 0.00 -0.02 0.00 -0.05
4 0.0167 0.00 0.25 0.00 -0.01
5 0.1529 0.00 -0.48 0.00 0.17
6 0.1529 0.00 0.08 0.00 -0.07
7 0.1530 0.00 0.09 0.00 0.00
8 0.1530 0.00 -0.33 0.00 0.15
9 0.1531 0.00 0.05 0.00 0.03
10 0.1532 0.00 0.13 0.00 -0.06
11 0.1532 0.00 -0.04 0.00 0.04
12 0.1532 0.00 0.07 0.00 0.02
13 0.1532 0.00 -0.36 0.00 0.12
14 0.1532 0.00 -0.03 0.00 -0.05
15 0.1555 0.00 0.08 0.00 -0.21
16 0.1556 0.00 -0.30 0.00 0.08
17 0.1556 0.00 0.14 0.00 -0.08
18 0.1557 0.00 0.05 0.00 0.08
19 0.1558 0.00 0.11 0.00 0.07
20 0.1558 0.00 0.10 0.00 -0.02
21 0.1692 0.00 -0.01 0.00 -0.14
22 0.1694 0.00 -0.03 0.00 0.06
23 0.1695 0.00 -0.02 0.00 -0.01
24 0.1696 0.00 -0.04 0.00 -0.14
25 0.2347 0.00 -0.19 0.00 0.06
26 0.2408 0.00 -0.13 0.00 -0.01
27 0.4046 0.00 0.18 0.00 -0.09
28 0.4073 0.00 0.30 0.00 0.27
29 0.4975 0.00 -0.15 0.00 -0.14
30 0.9831 0.00 -0.18 0.00 -0.20
31 0.9855 0.00 0.05 0.00 0.03
32 1.1440 0.00 -0.02 0.00 0.00
33 1.1440 0.00 -0.02 0.00 0.01
34 1.1441 0.00 0.02 0.00 -0.01
35 1.4313 0.00 0.09 0.00 0.03
36 8.1558 0.00 0.09 0.00 -0.12
37 8.1561 0.00 -0.01 0.00 -0.07
38 9.2775 0.00 -0.07 0.00 0.03
39 9.2777 0.00 0.02 0.00 0.16
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.
11UF411 quality flag:3 Type: 2:1E 2:1E 2:1E axisobj 48.314 48.314 48.314 ecceobj 0.350 0.350 0.350 incobj 5.866 5.866 5.866 qmin 30.571 30.592 30.540 qmax 65.833 65.735 65.961 amean 47.797 47.797 47.797 amin 47.263 47.280 47.258 amax 48.483 48.442 48.480 emean 0.337 0.337 0.338 emin 0.318 0.318 0.318 emax 0.359 0.359 0.361 imean 8.098 8.095 8.071 imin 6.326 6.377 6.258 imax 9.266 9.272 9.264 excite_mean 0.366 0.366 0.366 fracstop 1.000 1.000 1.000 cjmean 2.978 2.978 2.978 libcent 0 70.7 70.1 70.4 libamp 0 21.6 19.3 20.3 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 154.6 156.9 151.1 kozaiamp 179.9 180.0 180.0