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: 11HK103
# Created Sun Nov 24 02:09:10 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 81 observations of 81
# Arc: 6.23y
# First observation: 2011/04/28
# Last observation: 2017/07/21
# Chi-squared of fit: 34.57 DOF: 156 RMS: 0.12
# Min/Max residuals: -0.32 0.41
# Exact a, adot, b, bdot, g, gdot:
1.538616E-05 2.250106E-02 -1.393581E-06 -2.303545E-03 2.285083E-02 -5.747916E-03
# Covariance matrix:
1.0633E-13 -2.6254E-14 -3.4876E-15 2.5180E-15 6.3918E-14 -1.6731E-13
-2.6254E-14 4.4607E-14 3.5304E-15 -4.4878E-15 3.8058E-14 3.0131E-13
-3.4876E-15 3.5304E-15 4.6592E-14 -1.1379E-14 2.1751E-16 2.8398E-14
2.5180E-15 -4.4878E-15 -1.1379E-14 4.6432E-15 -3.0363E-15 -3.4217E-14
6.3918E-14 3.8058E-14 2.1751E-16 -3.0363E-15 1.4860E-13 2.0636E-13
-1.6731E-13 3.0131E-13 2.8398E-14 -3.4217E-14 2.0636E-13 2.2955E-12
# lat0 lon0 xBary yBary zBary JD0
2.721341 -82.448396 0.876434 0.023800 -0.501227 2455679.768846
# Heliocentric elements and errors
Epoch: 2455680.5000 = 2011/04/29
Mean Anomaly: 317.94932 +/- 0.007
Argument of Peri: 229.15266 +/- 0.009
Long of Asc Node: 121.11988 +/- 0.001
Inclination: 6.41549 +/- 0.000
Eccentricity: 0.31358260 +/- 0.0001
Semi-Major Axis: 53.34798060 +/- 0.0051
Time of Perihelion: 2472304.8984 +/- 18.1
Perihelion: 36.61898209 +/- 0.0054
Aphelion: 70.07697912 +/- 0.0078
Period (y) 389.6594 +/- 0.06
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X 4.94648531 +/- 0.0001
Ecliptic Y -43.94614277 +/- 0.0007
Ecliptic Z 2.07770806 +/- 0.0000
Ecliptic XDOT 0.00258198 +/- 0.0000
Ecliptic YDOT 0.00102919 +/- 0.0000
Ecliptic ZDOT -0.00030835 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 44.27261832 +/- 0.0007
Geocenter to KBO 43.76228346 +/- 0.0007
# Hcoef: 7.55
The following table shows the complete astrometric record for 11HK103. 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 (11HK103) followed by the observatory code and reference code for the source of the astrometry.
2011 04 28.26808 18 32 13.60 -20 30 25.2 11HK103 268 C~11qb 2011 04 28.36805 18 32 13.40 -20 30 25.2 11HK103 268 C~11qb 2011 04 30.27063 18 32 09.65 -20 30 24.2 11HK103 268 C~11qb 2011 04 30.39635 18 32 09.38 -20 30 24.3 11HK103 268 C~11qb 2011 05 06.36890 18 31 55.57 -20 30 23.9 11HK103 268 C~11qb 2011 05 31.43696 18 30 29.87 -20 30 59.5 11HK103 268 C~11qb 2011 05 31.48809 18 30 29.68 -20 30 59.8 11HK103 266 C~11qb 2011 05 31.56672 18 30 29.35 -20 30 59.9 11HK103 266 C~11qb 2011 06 01.59657 18 30 25.04 -20 31 02.7 11HK103 266 C~11qb 2011 06 04.14568 18 30 14.18 -20 31 09.5 11HK103 268 C~11qb 2011 06 04.29530 18 30 13.52 -20 31 10.2 11HK103 268 C~11qb 2011 06 04.39266 18 30 13.11 -20 31 10.4 11HK103 268 C~11qb 2011 07 01.35670 18 28 07.08 -20 32 55.7 11HK103 269 C~11qb 2011 07 02.03941 18 28 03.81 -20 32 58.7 11HK103 269 C~11qb 2011 07 02.14714 18 28 03.28 -20 32 59.4 11HK103 269 C~11qb 2011 07 02.14771 18 28 03.28 -20 32 59.4 11HK103 269 C~11qb 2011 07 02.25740 18 28 02.74 -20 33 00.0 11HK103 269 C~11qb 2011 07 02.25798 18 28 02.74 -20 32 59.9 11HK103 269 C~11qb 2011 07 02.28855 18 28 02.60 -20 33 00.4 11HK103 266 C~11qb 2011 07 02.53920 18 28 01.37 -20 33 01.7 11HK103 266 C~11qb 2013 06 03.21749 18 41 32.61 -20 37 35.3 11HK103 268 C~11qb 2013 06 03.27688 18 41 32.35 -20 37 35.5 11HK103 268 C~11qb 2013 06 04.21140 18 41 28.39 -20 37 39.3 11HK103 268 C~11qb 2013 06 04.28988 18 41 28.05 -20 37 39.6 11HK103 268 C~11qb 2013 06 04.36359 18 41 27.74 -20 37 39.9 11HK103 268 C~11qb 2013 06 08.17983 18 41 11.14 -20 37 56.3 11HK103 268 C~11qb 2013 06 08.22941 18 41 10.91 -20 37 56.5 11HK103 268 C~11qb 2013 06 08.26997 18 41 10.73 -20 37 56.7 11HK103 268 C~11qb 2013 06 11.21626 18 40 57.52 -20 38 10.3 11HK103 268 C~11qb 2013 06 11.27933 18 40 57.22 -20 38 10.5 11HK103 268 C~11qb 2013 06 13.21699 18 40 48.37 -20 38 19.7 11HK103 268 C~11qb 2013 06 13.27759 18 40 48.08 -20 38 20.0 11HK103 268 C~11qb 2013 06 13.35667 18 40 47.71 -20 38 20.5 11HK103 268 C~11qb 2013 06 13.37736 18 40 47.62 -20 38 20.6 11HK103 268 C~11qb 2013 07 02.16685 18 39 17.63 -20 40 04.5 11HK103 268 C~11qb 2013 07 03.16722 18 39 12.74 -20 40 10.6 24.7R 11HK103 268 C~11qb 2013 07 03.21583 18 39 12.51 -20 40 10.8 24.4R 11HK103 268 C~11qb 2013 07 03.29283 18 39 12.13 -20 40 11.3 24.1R 11HK103 268 C~11qb 2013 07 04.19617 18 39 07.74 -20 40 16.9 11HK103 268 C~11qb 2013 07 04.22277 18 39 07.60 -20 40 17.0 11HK103 268 C~11qb 2013 07 04.26659 18 39 07.37 -20 40 17.3 11HK103 268 C~11qb 2013 07 04.28468 18 39 07.29 -20 40 17.5 11HK103 268 C~11qb 2013 07 04.32105 18 39 07.16 -20 40 18.1 11HK103 266 C~11qb 2013 07 04.49429 18 39 06.31 -20 40 19.2 11HK103 266 C~11qb 2013 07 05.40444 18 39 01.89 -20 40 24.9 11HK103 266 C~11qb 2013 07 05.48836 18 39 01.46 -20 40 25.4 11HK103 266 C~11qb 2013 07 06.31422 18 38 57.43 -20 40 30.5 11HK103 266 C~11qb 2013 07 06.40236 18 38 57.00 -20 40 31.0 11HK103 266 C~11qb 2013 07 06.48552 18 38 56.60 -20 40 31.5 11HK103 266 C~11qb 2013 08 28.07314 18 35 33.69 -20 46 17.8 11HK103 268 C~11qb 2013 08 30.06766 18 35 29.45 -20 46 30.0 11HK103 268 C~11qb 2013 09 01.05156 18 35 25.57 -20 46 41.9 11HK103 268 C~11qb 2013 09 03.04605 18 35 22.02 -20 46 53.7 11HK103 268 C~11qb 2013 09 04.04833 18 35 20.37 -20 46 59.6 11HK103 268 C~11qb 2013 09 06.04337 18 35 17.35 -20 47 11.0 11HK103 268 C~11qb 2014 06 25.36079 18 45 37.028 -20 41 50.51 11HK103 266 C~2Gt6 2014 06 25.41554 18 45 36.754 -20 41 50.94 11HK103 266 C~2Gt6 2014 06 25.42936 18 45 36.687 -20 41 50.92 11HK103 266 C~2Gt6 2014 06 25.43035 18 45 36.685 -20 41 50.88 11HK103 266 C~2Gt6 2014 06 25.52625 18 45 36.214 -20 41 51.60 11HK103 266 C~2Gt6 2014 06 25.54714 18 45 36.107 -20 41 51.67 11HK103 266 C~2Gt6 2014 06 27.36374 18 45 27.281 -20 42 03.37 11HK103 266 C~2Gt7 2014 06 27.37057 18 45 27.247 -20 42 03.37 11HK103 266 C~2Gt7 2016 06 05.44847 18 58 49.839 -20 42 24.07 23.6r 11HK103 266 C~7ued 2016 06 05.52553 18 58 49.510 -20 42 24.54 23.6r 11HK103 266 C~7ued 2016 06 05.60261 18 58 49.181 -20 42 24.99 23.6r 11HK103 266 C~7ued 2016 06 30.28405 18 56 54.725 -20 45 20.46 23.9r 11HK103 266 C~7ued 2016 06 30.36862 18 56 54.303 -20 45 21.17 23.9r 11HK103 266 C~7ued 2016 06 30.42261 18 56 54.033 -20 45 21.61 23.9r 11HK103 266 C~7ued 2017 07 20.25325 19 01 17.167 -20 48 38.19 23.4r 11HK103 266 C~7ued 2017 07 20.27714 19 01 17.052 -20 48 38.43 23.5r 11HK103 266 C~7ued 2017 07 20.39364 19 01 16.484 -20 48 39.51 23.4r 11HK103 266 C~7ued 2017 07 20.41604 19 01 16.375 -20 48 39.73 23.5r 11HK103 266 C~7ued 2017 07 20.53088 19 01 15.816 -20 48 40.75 23.4r 11HK103 266 C~7ued 2017 07 20.55184 19 01 15.715 -20 48 40.95 23.5r 11HK103 266 C~7ued 2017 07 21.24888 19 01 12.405 -20 48 47.47 23.6r 11HK103 266 C~7ued 2017 07 21.26989 19 01 12.306 -20 48 47.57 23.6r 11HK103 266 C~7ued 2017 07 21.39163 19 01 11.716 -20 48 48.71 23.6r 11HK103 266 C~7ued 2017 07 21.41126 19 01 11.618 -20 48 49.00 23.6r 11HK103 266 C~7ued 2017 07 21.50353 19 01 11.171 -20 48 49.83 23.6r 11HK103 266 C~7ued 2017 07 21.52175 19 01 11.085 -20 48 49.89 23.6r 11HK103 266 C~7ued
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 0.04 0.00 -0.04
2 0.0003 0.00 -0.02 0.00 -0.08
3 0.0055 0.00 -0.02 0.00 0.02
4 0.0058 0.00 -0.05 0.00 -0.11
5 0.0222 0.00 0.06 0.00 -0.08
6 0.0908 0.00 -0.04 0.00 -0.01
7 0.0910 0.00 0.11 0.00 0.01
8 0.0912 0.00 0.16 0.00 0.11
9 0.0940 0.00 0.14 0.00 0.02
10 0.1010 0.00 -0.08 0.00 0.15
11 0.1014 0.00 -0.12 0.00 -0.11
12 0.1016 0.00 0.14 0.00 -0.04
13 0.1755 0.00 0.02 0.00 -0.07
14 0.1773 0.00 0.04 0.00 0.21
15 0.1776 0.00 -0.01 0.00 0.05
16 0.1776 0.00 0.03 0.00 0.05
17 0.1779 0.00 -0.01 0.00 -0.02
18 0.1779 0.00 0.03 0.00 0.08
19 0.1780 0.00 -0.09 0.00 -0.13
20 0.1787 0.00 -0.13 0.00 -0.21
21 2.0998 0.00 0.03 0.00 0.01
22 2.1000 0.00 -0.04 0.00 0.05
23 2.1025 0.00 -0.07 0.00 0.03
24 2.1027 0.00 -0.05 0.00 0.06
25 2.1029 0.00 0.10 0.00 0.05
26 2.1134 0.00 -0.01 0.00 -0.01
27 2.1135 0.00 -0.11 0.00 0.02
28 2.1136 0.00 -0.07 0.00 -0.00
29 2.1217 0.00 0.05 0.00 -0.10
30 2.1219 0.00 -0.08 0.00 0.00
31 2.1272 0.00 0.02 0.00 0.08
32 2.1273 0.00 -0.07 0.00 0.08
33 2.1276 0.00 -0.07 0.00 -0.05
34 2.1276 0.00 0.03 0.00 -0.05
35 2.1791 0.00 -0.01 0.00 -0.04
36 2.1818 0.00 -0.21 0.00 -0.02
37 2.1819 0.00 -0.05 0.00 0.08
38 2.1821 0.00 -0.04 0.00 0.04
39 2.1846 0.00 0.01 0.00 0.02
40 2.1847 0.00 -0.12 0.00 0.08
41 2.1848 0.00 -0.32 0.00 0.05
42 2.1849 0.00 -0.18 0.00 -0.04
43 2.1849 0.00 0.29 0.00 -0.26
44 2.1854 0.00 0.41 0.00 -0.28
45 2.1879 0.00 0.40 0.00 -0.31
46 2.1881 0.00 0.18 0.00 -0.29
47 2.1904 0.00 -0.31 0.00 -0.22
48 2.1906 0.00 -0.24 0.00 -0.16
49 2.1909 0.00 -0.08 0.00 -0.14
50 2.3349 0.00 0.09 0.00 0.17
51 2.3403 0.00 0.03 0.00 0.14
52 2.3457 0.00 -0.03 0.00 0.16
53 2.3512 0.00 -0.02 0.00 0.14
54 2.3540 0.00 0.01 0.00 0.08
55 2.3594 0.00 -0.04 0.00 0.13
56 3.1597 0.00 0.14 0.00 0.13
57 3.1599 0.00 0.08 0.00 0.06
58 3.1599 0.00 0.10 0.00 0.17
59 3.1599 0.00 0.15 0.00 0.22
60 3.1602 0.00 0.19 0.00 0.10
61 3.1602 0.00 0.13 0.00 0.16
62 3.1652 0.00 0.09 0.00 0.13
63 3.1652 0.00 0.09 0.00 0.17
64 5.1066 0.00 -0.04 0.00 -0.01
65 5.1068 0.00 -0.03 0.00 -0.02
66 5.1070 0.00 -0.03 0.00 -0.01
67 5.1746 0.00 -0.06 0.00 -0.01
68 5.1748 0.00 -0.07 0.00 -0.01
69 5.1750 0.00 -0.07 0.00 -0.01
70 6.2286 0.00 0.01 0.00 -0.01
71 6.2286 0.00 0.02 0.00 -0.02
72 6.2290 0.00 0.02 0.00 -0.01
73 6.2290 0.00 0.02 0.00 -0.02
74 6.2293 0.00 0.02 0.00 -0.00
75 6.2294 0.00 0.02 0.00 -0.02
76 6.2313 0.00 -0.02 0.00 -0.10
77 6.2314 0.00 0.01 0.00 0.01
78 6.2317 0.00 0.01 0.00 0.01
79 6.2317 0.00 -0.03 0.00 -0.10
80 6.2320 0.00 -0.03 0.00 -0.09
81 6.2320 0.00 0.00 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.
11HK103 quality flag:3 Type: SCATNEAR SCATNEAR SCATNEAR axisobj 53.099 53.099 53.100 ecceobj 0.313 0.313 0.313 incobj 6.419 6.419 6.419 qmin 35.678 35.721 35.348 qmax 71.609 71.548 71.812 amean 53.241 53.013 53.192 amin 52.622 52.158 52.193 amax 53.966 53.984 53.938 emean 0.313 0.308 0.313 emin 0.299 0.288 0.297 emax 0.328 0.326 0.332 imean 5.299 5.308 5.348 imin 4.427 4.415 4.421 imax 6.397 6.334 6.623 excite_mean 0.327 0.322 0.327 fracstop 1.000 1.000 1.000 cjmean 3.080 3.081 3.079 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 182.8 182.9 183.7 kozaiamp 179.9 180.0 179.9