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: 14UT277 # Created Sun Nov 24 02:10:06 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 13 observations of 13 # Arc: 7.09y # First observation: 2014/10/29 # Last observation: 2021/12/01 # Chi-squared of fit: 9.34 DOF: 20 RMS: 0.15 # Min/Max residuals: -0.26 0.35 # Exact a, adot, b, bdot, g, gdot: 1.425472E-05 2.026890E-02 1.319002E-06 1.543625E-03 2.251438E-02 6.886984E-05 # Covariance matrix: 5.2829E-13 -5.0501E-13 2.8286E-14 -4.1131E-14 1.5484E-13 -3.3234E-12 -5.0501E-13 6.9338E-13 -4.1083E-14 5.9804E-14 -2.2975E-13 4.8317E-12 2.8286E-14 -4.1083E-14 2.1008E-13 -4.2584E-14 1.1367E-14 -2.9199E-13 -4.1131E-14 5.9804E-14 -4.2584E-14 2.1433E-14 -2.3763E-14 4.2815E-13 1.5484E-13 -2.2975E-13 1.1367E-14 -2.3763E-14 6.0173E-13 -1.8647E-12 -3.3234E-12 4.8317E-12 -2.9199E-13 4.2815E-13 -1.8647E-12 3.4568E-11 # lat0 lon0 xBary yBary zBary JD0 -3.873317 18.675126 -0.285809 -0.064185 -0.950742 2456959.728228 # Heliocentric elements and errors Epoch: 2456960.5000 = 2014/10/30 Mean Anomaly: 173.05125 +/- 0.248 Argument of Peri: 145.13978 +/- 0.244 Long of Asc Node: 59.86030 +/- 0.002 Inclination: 5.78981 +/- 0.000 Eccentricity: 0.06605943 +/- 0.0001 Semi-Major Axis: 42.57163855 +/- 0.0070 Time of Perihelion: 2408190.6742 +/- 71.0 Perihelion: 39.75938023 +/- 0.0082 Aphelion: 45.38389687 +/- 0.0090 Period (y) 277.7722 +/- 0.07 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 42.78986135 +/- 0.0014 Ecliptic Y 14.76727571 +/- 0.0005 Ecliptic Z -3.00032993 +/- 0.0001 Ecliptic XDOT -0.00077372 +/- 0.0000 Ecliptic YDOT 0.00233692 +/- 0.0000 Ecliptic ZDOT 0.00018682 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 45.36569425 +/- 0.0014 Geocenter to KBO 44.41609410 +/- 0.0015 # Hcoef: 6.55
The following table shows the complete astrometric record for 14UT277. 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 (14UT277) followed by the observatory code and reference code for the source of the astrometry.
2014 10 29.22745 01 14 48.663 +03 43 57.65 22.6i 14UT277 W84 C~55Sh 2014 11 18.12715 01 13 33.823 +03 37 33.00 22.0z 14UT277 W84 C~55Sh 2014 11 21.11003 01 13 24.116 +03 36 47.63 22.4z 14UT277 W84 C~55Sh 2015 11 07.11459 01 18 24.291 +04 12 01.56 22.7i 14UT277 W84 C~55Sh 2015 11 07.11595 01 18 24.280 +04 12 01.36 23.3r 14UT277 W84 C~55Sh 2015 11 07.11732 01 18 24.269 +04 12 01.47 24.4g 14UT277 W84 C~55Sh 2015 12 18.07071 01 16 29.620 +04 03 47.24 22.8z 14UT277 W84 C~55Sh 2016 08 26.33786 01 27 09.546 +05 10 34.37 23.2i 14UT277 W84 C~55Sh 2016 08 26.33924 01 27 09.557 +05 10 34.36 23.2r 14UT277 W84 C~55Sh 2016 10 29.19725 01 23 07.371 +04 45 56.85 23.7g 14UT277 W84 C~55Sh 2021 12 01.070050 01 42 02.622 +07 09 26.30 23.3G 14UT277 G37 C~5J6X 2021 12 01.121880 01 42 02.421 +07 09 25.26 14UT277 G37 C~5J6X 2021 12 01.173620 01 42 02.265 +07 09 24.74 14UT277 G37 C~5J6X
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 0.01 0.00 -0.05
2 0.0545 0.00 -0.03 0.00 -0.01
3 0.0626 0.00 0.03 0.00 0.21
4 1.0236 0.00 0.04 0.00 0.05
5 1.0237 0.00 -0.05 0.00 -0.13
6 1.0237 0.00 -0.13 0.00 0.01
7 1.1358 0.00 0.14 0.00 -0.26
8 1.8264 0.00 -0.07 0.00 -0.06
9 1.8265 0.00 0.15 0.00 -0.05
10 2.0013 0.00 -0.04 0.00 0.31
11 7.0906 0.00 0.35 0.00 0.18
12 7.0907 0.00 -0.23 0.00 -0.18
13 7.0909 0.00 -0.14 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.
14UT277 quality flag:3 Type: CLASSICAL CLASSICAL CLASSICAL axisobj 42.916 42.916 42.916 ecceobj 0.058 0.058 0.058 incobj 5.781 5.781 5.781 qmin 39.033 39.031 39.031 qmax 46.478 46.477 46.493 amean 42.674 42.674 42.674 amin 42.340 42.335 42.335 amax 43.019 43.016 43.020 emean 0.058 0.058 0.058 emin 0.036 0.036 0.036 emax 0.081 0.081 0.081 imean 3.846 3.846 3.846 imin 2.787 2.788 2.788 imax 5.062 5.062 5.064 excite_mean 0.089 0.089 0.089 fracstop 1.000 1.000 1.000 cjmean 3.076 3.076 3.076 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 188.6 188.6 188.4 kozaiamp 180.0 180.0 180.0