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: 14UE228
# Created Fri Nov 22 02:10:06 2024
# Orbit generated from Bernstein formalism
# Fitting 31 observations of 31
# Arc: 4.06y
# First observation: 2013/08/09
# Last observation: 2017/08/30
Preliminary a, adot, b, bdot, g, gdot:
-0.000706 0.028573 0.000092 -0.003943 0.025286 0.000000
# Chi-squared of fit: 18.60 DOF: 56 RMS: 0.14
# Min/Max residuals: -0.76 0.38
# Exact a, adot, b, bdot, g, gdot:
1.735078E-05 2.742747E-02 -1.599495E-06 -3.776869E-03 2.517231E-02 -7.126466E-03
# Covariance matrix:
2.8846E-13 -1.9530E-13 -1.3259E-14 1.9333E-14 7.4638E-14 -1.2282E-12
-1.9530E-13 2.7578E-13 2.1919E-14 -3.5598E-14 3.4400E-14 2.2060E-12
-1.3259E-14 2.1919E-14 1.0826E-13 -4.8650E-14 3.4793E-15 2.0058E-13
1.9333E-14 -3.5598E-14 -4.8650E-14 3.9413E-14 -8.0175E-15 -3.2921E-13
7.4638E-14 3.4400E-14 3.4793E-15 -8.0175E-15 1.0812E-13 4.6444E-13
-1.2282E-12 2.2060E-12 2.0058E-13 -3.2921E-13 4.6444E-13 2.0354E-11
# lat0 lon0 xBary yBary zBary JD0
4.114506 26.544292 0.952951 0.025228 -0.350260 2456513.995978
# Heliocentric elements and errors
Epoch: 2456510.5000 = 2013/08/06
Mean Anomaly: 335.15371 +/- 0.007
Argument of Peri: 210.40882 +/- 0.020
Long of Asc Node: 232.65208 +/- 0.001
Inclination: 8.78454 +/- 0.000
Eccentricity: 0.40649096 +/- 0.0002
Semi-Major Axis: 58.32373396 +/- 0.0086
Time of Perihelion: 2467739.0959 +/- 2.2
Perihelion: 34.61566308 +/- 0.0102
Aphelion: 82.03180483 +/- 0.0149
Period (y) 445.4266 +/- 0.10
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X 36.18664070 +/- 0.0005
Ecliptic Y 17.01501707 +/- 0.0002
Ecliptic Z 2.85033090 +/- 0.0000
Ecliptic XDOT -0.00200460 +/- 0.0000
Ecliptic YDOT 0.00233547 +/- 0.0000
Ecliptic ZDOT -0.00046520 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 40.08875350 +/- 0.0004
Geocenter to KBO 39.72619278 +/- 0.0005
# Hcoef: 8.41
The following table shows the complete astrometric record for 14UE228. 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 (14UE228) followed by the observatory code and reference code for the source of the astrometry.
2013 08 09.49520 01 32 21.714 +14 04 17.62 24.2r 14UE228 568 C~2SDe 2013 08 09.53863 01 32 21.655 +14 04 17.78 24.7r 14UE228 568 C~2SDe 2013 11 01.48519 01 27 12.271 +13 35 21.58 23.7r 14UE228 568 C~2SDe 2013 12 29.24308 01 24 26.893 +13 12 37.73 24.3r 14UE228 568 C~2SDe 2013 12 30.33421 01 24 26.401 +13 12 25.13 24.6r 14UE228 568 C~2SDe 2014 01 02.22987 01 24 25.709 +13 11 55.35 24.5r 14UE228 568 C~2SDe 2014 01 02.27696 01 24 25.696 +13 11 54.91 24.4r 14UE228 568 C~2SDe 2014 01 02.35718 01 24 25.690 +13 11 54.59 24.5r 14UE228 568 C~2SDe 2014 01 03.23668 01 24 25.655 +13 11 46.13 24.5r 14UE228 568 C~2SDe 2014 07 26.50994 01 38 50.780 +14 26 08.92 24.5r 14UE228 568 C~2SDe 2014 07 26.55326 01 38 50.788 +14 26 09.05 24.4r 14UE228 568 C~2SDe 2014 07 26.59650 01 38 50.801 +14 26 09.41 24.6r 14UE228 568 C~2SDe 2014 08 24.44612 01 38 22.831 +14 25 17.83 24.4r 14UE228 568 C~2SDe 2014 08 24.52005 01 38 22.674 +14 25 17.09 24.4r 14UE228 568 C~2SDe 2014 08 30.42440 01 38 07.986 +14 24 11.08 24.2r 14UE228 568 C~2SDe 2014 08 30.53271 01 38 07.693 +14 24 09.86 24.8r 14UE228 568 C~2SDe 2014 09 18.45130 01 37 03.677 +14 18 44.12 24.2r 14UE228 568 C~2SDe 2014 09 18.49406 01 37 03.506 +14 18 43.28 24.8r 14UE228 568 C~2SDe 2014 10 22.27410 01 34 29.710 +14 03 44.18 24.4r 14UE228 568 C~2SDe 2014 10 22.31909 01 34 29.504 +14 03 42.70 24.3r 14UE228 568 C~2SDe 2014 10 22.36391 01 34 29.277 +14 03 41.42 24.0r 14UE228 568 C~2SDe 2014 10 23.45625 01 34 24.028 +14 03 08.36 24.0r 14UE228 568 C~2SDe 2014 10 25.47218 01 34 14.371 +14 02 07.33 24.3r 14UE228 568 C~2SDe 2014 11 20.34387 01 32 20.104 +13 49 16.05 24.7r 14UE228 568 C~2SDe 2014 11 21.24351 01 32 16.668 +13 48 50.82 24.1r 14UE228 568 C~2SDe 2014 11 21.40974 01 32 16.010 +13 48 46.03 24.3r 14UE228 568 C~2SDe 2016 11 04.38287 01 46 42.352 +14 41 57.66 24.5w 14UE228 568 C~2SDe 2016 11 04.43686 01 46 42.090 +14 41 56.06 24.4w 14UE228 568 C~2SDe 2017 08 25.59703 01 58 21.321 +15 30 21.21 24.7w 14UE228 568 C~2SDe 2017 08 30.60899 01 58 10.375 +15 29 33.28 14UE228 568 C~2SDe 2017 08 30.61830 01 58 10.356 +15 29 33.24 24.6w 14UE228 568 C~2SDe
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 -0.03 0.00 -0.16
2 0.0001 -0.74 -0.03 0.46 0.12
3 0.2300 -4830.45 0.10 51.52 -0.76
4 0.3881 -7580.73 -0.02 -313.58 -0.04
5 0.3911 -7592.13 -0.11 -322.58 -0.13
6 0.3990 -7612.68 -0.01 -346.42 -0.04
7 0.3991 -7613.02 -0.06 -346.76 -0.00
8 0.3993 -7613.22 0.20 -347.03 0.38
9 0.4018 -7616.87 -0.03 -354.68 0.06
10 0.9610 5747.44 0.11 -835.48 0.05
11 0.9611 5747.60 -0.02 -835.40 -0.05
12 0.9613 5747.91 0.02 -835.13 0.03
13 1.0402 5350.03 -0.17 -736.66 0.16
14 1.0405 5347.63 0.01 -736.53 0.05
15 1.0566 5124.66 -0.03 -721.05 -0.03
16 1.0569 5120.25 0.16 -720.65 0.05
17 1.1087 4134.66 -0.02 -687.89 -0.04
18 1.1088 4132.03 0.04 -687.77 0.01
19 1.2013 1721.10 -0.06 -712.40 0.20
20 1.2014 1717.77 0.07 -712.68 0.00
21 1.2016 1714.23 -0.01 -712.67 0.10
22 1.2045 1631.05 0.01 -715.59 -0.04
23 1.2101 1477.93 -0.02 -721.13 -0.03
24 1.2809 -352.56 -0.03 -830.11 0.19
25 1.2834 -408.38 0.04 -835.22 0.12
26 1.2838 -419.05 -0.16 -836.16 0.03
27 3.2386 12496.48 0.07 -2391.71 -0.03
28 3.2387 12492.35 0.07 -2391.87 -0.00
29 4.0441 23079.81 0.01 -3180.36 -0.17
30 4.0578 22912.64 -0.09 -3171.47 -0.03
31 4.0578 22912.36 -0.01 -3171.41 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.
14UE228 quality flag:3 Type: 8:3EEEEE 8:3EEEEE 8:3EEEEE axisobj 58.672 58.693 58.651 ecceobj 0.408 0.408 0.407 incobj 8.777 8.777 8.777 qmin 34.059 34.069 34.020 qmax 82.962 83.149 83.127 amean 57.901 57.900 57.900 amin 57.102 57.152 57.178 amax 58.867 58.883 58.866 emean 0.397 0.398 0.397 emin 0.383 0.385 0.383 emax 0.411 0.412 0.413 imean 10.371 10.312 10.297 imin 9.638 9.748 9.483 imax 11.186 10.797 11.214 excite_mean 0.436 0.436 0.436 fracstop 1.000 1.000 1.000 cjmean 3.024 3.024 3.024 libcent 0 179.5 180.4 179.6 libamp 0 89.9 105.3 85.9 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 223.3 196.6 235.7 kozaiamp 180.0 180.0 180.0