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: 14RT86 # Created Sun Nov 24 02:09:57 2024 # Orbit generated from Bernstein formalism # Fitting 12 observations of 12 # Arc: 3.37y # First observation: 2014/09/04 # Last observation: 2018/01/17 Preliminary a, adot, b, bdot, g, gdot: 0.000106 0.031163 -0.000087 0.004884 0.027525 0.000000 # Chi-squared of fit: 4.99 DOF: 18 RMS: 0.11 # Min/Max residuals: -0.24 0.26 # Exact a, adot, b, bdot, g, gdot: 1.796757E-05 3.117456E-02 2.836363E-06 4.837773E-03 2.770286E-02 -2.982150E-03 # Covariance matrix: 1.2172E-12 -6.9557E-14 -1.6405E-13 3.2455E-14 7.2195E-13 7.6660E-14 -6.9557E-14 6.9583E-13 -1.1912E-13 1.8894E-13 3.2354E-13 9.2538E-12 -1.6405E-13 -1.1912E-13 3.9699E-13 -1.7100E-13 -1.8363E-13 -1.6320E-12 3.2455E-14 1.8894E-13 -1.7100E-13 1.3579E-13 1.0952E-13 2.8159E-12 7.2195E-13 3.2354E-13 -1.8363E-13 1.0952E-13 7.1932E-13 4.1567E-12 7.6660E-14 9.2538E-12 -1.6320E-12 2.8159E-12 4.1567E-12 1.3942E-10 # lat0 lon0 xBary yBary zBary JD0 -30.366597 22.655316 0.665644 -0.384677 -0.656833 2456904.828548 # Heliocentric elements and errors Epoch: 2456900.5000 = 2014/08/31 Mean Anomaly: 339.47915 +/- 0.052 Argument of Peri: 318.00465 +/- 0.093 Long of Asc Node: 95.17336 +/- 0.001 Inclination: 30.78479 +/- 0.000 Eccentricity: 0.24275008 +/- 0.0002 Semi-Major Axis: 46.93222943 +/- 0.0086 Time of Perihelion: 2463594.6893 +/- 16.7 Perihelion: 35.53942683 +/- 0.0131 Aphelion: 58.32503204 +/- 0.0156 Period (y) 321.5252 +/- 0.09 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 29.69823566 +/- 0.0009 Ecliptic Y 11.67763835 +/- 0.0003 Ecliptic Z -18.24825759 +/- 0.0006 Ecliptic XDOT -0.00120315 +/- 0.0000 Ecliptic YDOT 0.00283395 +/- 0.0000 Ecliptic ZDOT 0.00056163 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 36.76073101 +/- 0.0008 Geocenter to KBO 36.09735106 +/- 0.0011 # Hcoef: 7.70
The following table shows the complete astrometric record for 14RT86. 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 (14RT86) followed by the observatory code and reference code for the source of the astrometry.
2014 09 04.32777 02 09 44.635 -19 22 01.10 23.4r 14RT86 W84 C~52Tx 2014 12 22.12341 02 01 29.541 -19 45 31.65 22.9r 14RT86 W84 C~52Tx 2014 12 24.15363 02 01 24.733 -19 44 12.24 23.4i 14RT86 W84 C~52Tx 2015 01 09.05044 02 01 02.146 -19 31 55.40 23.0i 14RT86 W84 C~52Tx 2015 01 28.06351 02 01 11.833 -19 13 39.36 23.1z 14RT86 W84 C~52Tx 2016 11 25.22626 02 16 08.051 -18 02 23.22 23.6r 14RT86 W84 C~52Tx 2016 11 25.22762 02 16 08.045 -18 02 23.37 24.2g 14RT86 W84 C~52Tx 2016 11 26.20792 02 16 03.304 -18 02 14.08 22.9i 14RT86 W84 C~52Tx 2016 12 31.12454 02 14 02.782 -17 46 20.76 22.3i 14RT86 W84 C~52Tx 2017 11 23.13798 02 22 48.328 -17 03 36.42 23.5r 14RT86 W84 C~52Tx 2017 11 23.13935 02 22 48.323 -17 03 36.47 23.6i 14RT86 W84 C~52Tx 2018 01 17.09602 02 20 07.648 -16 34 48.10 23.7r 14RT86 W84 C~52Tx
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 -0.02
2 0.2979 -7006.27 0.03 1381.93 -0.18
3 0.3034 -7039.16 -0.01 1481.17 0.01
4 0.3469 -7056.52 0.09 2284.49 0.26
5 0.3990 -6515.34 -0.10 3248.23 -0.06
6 2.2256 6890.25 0.14 2251.53 0.01
7 2.2256 6890.11 0.08 2251.43 -0.14
8 2.2283 6831.68 -0.24 2286.83 0.14
9 2.3239 5628.52 0.10 3844.12 -0.02
10 3.2192 13566.95 -0.04 3187.20 -0.06
11 3.2192 13566.86 -0.03 3187.18 -0.12
12 3.3697 12149.78 0.02 5704.92 0.17
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.
14RT86 quality flag:3 Type: SCATNEAR SCATNEAR SCATNEAR axisobj 47.397 47.418 47.376 ecceobj 0.248 0.249 0.248 incobj 30.798 30.798 30.798 qmin 34.388 34.409 34.388 qmax 60.129 60.208 60.127 amean 46.988 47.014 46.974 amin 46.557 46.570 46.552 amax 47.556 47.525 47.511 emean 0.246 0.247 0.246 emin 0.227 0.227 0.226 emax 0.266 0.267 0.266 imean 29.062 29.062 29.059 imin 28.492 28.496 28.486 imax 29.560 29.550 29.543 excite_mean 0.545 0.545 0.545 fracstop 1.000 1.000 1.000 cjmean 2.758 2.758 2.758 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 180.1 179.6 180.1 kozaiamp 180.0 180.0 180.0