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: 14QZ510 # Created Fri Nov 22 02:09:58 2024 # Orbit generated by ELGB # -->Covariance matrix from a Bernstein fit # Fitting 83 observations of 83 # Arc: 7.23y # First observation: 2014/08/19 # Last observation: 2021/11/11 # Chi-squared of fit: 28.10 DOF: 160 RMS: 0.10 # Min/Max residuals: -0.39 0.33 # Exact a, adot, b, bdot, g, gdot: 1.824428E-05 3.806551E-02 4.602672E-06 9.918543E-03 3.239616E-02 6.178211E-03 # Covariance matrix: 1.5152E-13 -4.9353E-14 1.3665E-14 -9.2002E-15 6.4166E-14 -1.6371E-13 -4.9353E-14 4.6752E-14 -1.1090E-14 1.1637E-14 9.7785E-15 1.9621E-13 1.3665E-14 -1.1090E-14 5.0978E-14 -1.5776E-14 1.3053E-15 -5.2057E-14 -9.2002E-15 1.1637E-14 -1.5776E-14 8.6719E-15 3.8796E-15 5.5346E-14 6.4166E-14 9.7785E-15 1.3053E-15 3.8796E-15 7.6722E-14 5.6651E-14 -1.6371E-13 1.9621E-13 -5.2057E-14 5.5346E-14 5.6651E-14 9.3201E-13 # lat0 lon0 xBary yBary zBary JD0 -19.761780 20.248392 0.822440 -0.200868 -0.559487 2456888.864778 # Heliocentric elements and errors Epoch: 2456888.5000 = 2014/08/19 Mean Anomaly: 25.15779 +/- 0.004 Argument of Peri: 263.69611 +/- 0.006 Long of Asc Node: 71.86533 +/- 0.000 Inclination: 23.72659 +/- 0.000 Eccentricity: 0.23762919 +/- 0.0000 Semi-Major Axis: 39.32025903 +/- 0.0019 Time of Perihelion: 2450594.9896 +/- 1.0 Perihelion: 29.97661775 +/- 0.0020 Aphelion: 48.66390032 +/- 0.0028 Period (y) 246.5658 +/- 0.02 # Ecliptic coordinates at JD0 (AU and AU/d) Ecliptic X 28.09464458 +/- 0.0002 Ecliptic Y 9.49008115 +/- 0.0001 Ecliptic Z -10.43661085 +/- 0.0001 Ecliptic XDOT -0.00039134 +/- 0.0000 Ecliptic YDOT 0.00328203 +/- 0.0000 Ecliptic ZDOT 0.00061245 +/- 0.0000 # Distances at JD0 (AU) Heliocenter to KBO 31.43705863 +/- 0.0002 Geocenter to KBO 30.86779277 +/- 0.0003 # Hcoef: 7.67
The following table shows the complete astrometric record for 14QZ510. 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 (14QZ510) followed by the observatory code and reference code for the source of the astrometry.
2014 08 19.36400 01 44 33.701 -10 24 27.60 22.7i 14QZ510 W84 C~4yU1 2014 08 19.36400 01 44 33.70 -10 24 27.6 22.8i 14QZ510 W84 C~3cnQ 2014 09 25.25078 01 42 05.799 -10 50 20.03 22.5r 14QZ510 W84 C~4yU1 2014 09 25.25078 01 42 05.80 -10 50 20.0 22.6r 14QZ510 W84 C~3cnQ 2014 10 03.35375 01 41 19.977 -10 55 25.51 22.7r 14QZ510 W84 C~4yU1 2014 10 03.35375 01 41 19.98 -10 55 25.5 22.7r 14QZ510 W84 C~3cnQ 2014 12 13.14243 01 35 05.607 -11 05 04.80 22.6r 14QZ510 W84 C~4yU1 2014 12 13.14243 01 35 05.61 -11 05 04.8 22.6r 14QZ510 W84 C~3cnQ 2014 12 15.14761 01 34 59.933 -11 04 12.63 23.1g 14QZ510 W84 C~4yU1 2014 12 15.14761 01 34 59.93 -11 04 12.6 23.4g 14QZ510 W84 C~3cnQ 2014 12 15.14897 01 34 59.926 -11 04 12.48 22.6r 14QZ510 W84 C~4yU1 2014 12 15.14897 01 34 59.93 -11 04 12.5 22.7r 14QZ510 W84 C~3cnQ 2014 12 26.05664 01 34 37.022 -10 58 23.03 22.1z 14QZ510 W84 C~4yU1 2015 08 18.41190 01 51 51.091 -09 02 48.03 23.3g 14QZ510 W84 C~4yU1 2015 08 19.39839 01 51 49.169 -09 03 26.12 22.9i 14QZ510 W84 C~4yU1 2015 08 24.41215 01 51 37.727 -09 06 44.03 22.5i 14QZ510 W84 C~4yU1 2015 09 13.31447 01 50 27.270 -09 20 26.06 22.7r 14QZ510 W84 C~4yU1 2015 09 13.31447 01 50 27.27 -09 20 26.1 22.7r 14QZ510 W84 C~3cnQ 2015 09 23.25357 01 49 39.286 -09 27 09.65 22.6z 14QZ510 W84 C~4yU1 2015 11 01.21545 01 45 49.995 -09 46 44.75 22.1z 14QZ510 W84 C~4yU1 2015 11 01.21545 01 45 49.99 -09 46 44.8 22.3z 14QZ510 W84 C~3cnQ 2015 11 02.17299 01 45 44.243 -09 47 00.80 23.4g 14QZ510 W84 C~4yU1 2015 11 06.20466 01 45 20.286 -09 47 59.91 22.2i 14QZ510 W84 C~4yU1 2015 11 06.20466 01 45 20.29 -09 47 59.9 22.2i 14QZ510 W84 C~3cnQ 2015 11 07.19885 01 45 14.456 -09 48 12.33 22.5z 14QZ510 W84 C~4yU1 2015 11 07.19885 01 45 14.46 -09 48 12.3 22.7z 14QZ510 W84 C~3cnQ 2015 11 07.23740 01 45 14.228 -09 48 12.96 21.8i 14QZ510 W84 C~4yU1 2015 11 07.23740 01 45 14.23 -09 48 12.8 22.3i 14QZ510 W84 C~3cnQ 2015 11 08.20295 01 45 08.605 -09 48 23.96 22.2z 14QZ510 W84 C~4yU1 2015 11 08.20295 01 45 08.60 -09 48 24.0 22.2z 14QZ510 W84 C~3cnQ 2015 11 15.13681 01 44 29.459 -09 49 19.34 22.6i 14QZ510 W84 C~4yU1 2015 11 15.13681 01 44 29.46 -09 49 19.3 22.6i 14QZ510 W84 C~3cnQ 2015 11 15.13819 01 44 29.457 -09 49 19.35 22.7r 14QZ510 W84 C~4yU1 2015 11 15.13819 01 44 29.46 -09 49 19.4 22.7r 14QZ510 W84 C~3cnQ 2015 11 15.13957 01 44 29.453 -09 49 19.17 23.0g 14QZ510 W84 C~4yU1 2015 11 15.13957 01 44 29.45 -09 49 19.2 23.2g 14QZ510 W84 C~3cnQ 2016 10 03.24871 01 55 54.479 -08 12 33.91 22.5r 14QZ510 W84 C~4yU1 2016 10 03.24871 01 55 54.48 -08 12 33.9 22.6r 14QZ510 W84 C~3cnQ 2016 10 03.25008 01 55 54.476 -08 12 34.01 22.2i 14QZ510 W84 C~4yU1 2016 10 03.25008 01 55 54.48 -08 12 34.0 22.2i 14QZ510 W84 C~3cnQ 2016 10 03.25145 01 55 54.463 -08 12 34.10 23.4g 14QZ510 W84 C~4yU1 2016 10 03.25145 01 55 54.46 -08 12 34.1 23.5g 14QZ510 W84 C~3cnQ 2016 10 03.26110 01 55 54.401 -08 12 34.40 22.4i 14QZ510 W84 C~4yU1 2016 10 03.26110 01 55 54.40 -08 12 34.4 22.5i 14QZ510 W84 C~3cnQ 2016 10 03.26248 01 55 54.397 -08 12 34.36 22.6r 14QZ510 W84 C~4yU1 2016 10 03.26248 01 55 54.40 -08 12 34.3 22.8r 14QZ510 W84 C~3cnQ 2016 10 03.26385 01 55 54.389 -08 12 34.36 23.3g 14QZ510 W84 C~4yU1 2016 10 03.26385 01 55 54.39 -08 12 34.3 23.3g 14QZ510 W84 C~3cnQ 2016 10 03.26523 01 55 54.378 -08 12 34.52 22.3z 14QZ510 W84 C~4yU1 2016 10 22.28291 01 54 01.288 -08 22 17.58 22.0i 14QZ510 W84 C~4yU1 2016 10 22.28291 01 54 01.29 -08 22 17.6 22.1i 14QZ510 W84 C~3cnQ 2016 10 23.20414 01 53 55.665 -08 22 40.40 22.6r 14QZ510 W84 C~4yU1 2016 10 23.20414 01 53 55.66 -08 22 40.4 22.7r 14QZ510 W84 C~3cnQ 2016 10 23.20551 01 53 55.655 -08 22 40.21 23.5g 14QZ510 W84 C~4yU1 2016 10 23.20551 01 53 55.65 -08 22 40.2 23.5g 14QZ510 W84 C~3cnQ 2016 12 04.05703 01 50 07.582 -08 27 43.73 22.2z 14QZ510 W84 C~4yU1 2016 12 04.05703 01 50 07.58 -08 27 43.7 22.1z 14QZ510 W84 C~3cnQ 2017 10 30.14413 02 00 22.341 -07 04 22.80 22.2i 14QZ510 W84 C~4yU1 2017 10 30.14550 02 00 22.335 -07 04 22.72 22.3z 14QZ510 W84 C~4yU1 2017 11 27.14226 01 57 45.282 -07 08 42.06 21.9z 14QZ510 W84 C~4yU1 2017 11 27.15056 01 57 45.231 -07 08 42.00 22.3i 14QZ510 W84 C~4yU1 2017 11 27.19433 01 57 45.017 -07 08 41.77 22.2i 14QZ510 W84 C~4yU1 2017 12 07.15681 01 57 00.527 -07 07 27.16 22.5Y 14QZ510 W84 C~4yU1 2017 12 22.11777 01 56 10.943 -07 02 45.06 22.8r 14QZ510 W84 C~4yU1 2017 12 22.11915 01 56 10.937 -07 02 45.10 23.8g 14QZ510 W84 C~4yU1 2017 12 25.11530 01 56 03.858 -07 01 24.54 22.8z 14QZ510 W84 C~4yU1 2018 09 10.40795 02 11 47.502 -05 17 10.98 22.3z 14QZ510 W84 C~4yU1 2019 09 29.43478 02 17 14.93 -04 09 10.2 22.9r 14QZ510 T09 C~7znH 2019 09 29.45729 02 17 14.81 -04 09 10.9 23.1r 14QZ510 T09 C~7znH 2019 09 29.49462 02 17 14.60 -04 09 12.2 22.8i 14QZ510 T09 C~7znH 2019 09 29.49845 02 17 14.60 -04 09 12.4 23.0i 14QZ510 T09 C~7znH 2019 09 29.53122 02 17 14.42 -04 09 13.8 22.9i 14QZ510 T09 C~7znH 2019 09 29.53505 02 17 14.39 -04 09 13.8 23.0i 14QZ510 T09 C~7znH 2019 09 29.55335 02 17 14.32 -04 09 14.4 22.9i 14QZ510 T09 C~7znH 2019 09 29.59096 02 17 14.10 -04 09 15.8 22.4z 14QZ510 T09 C~7znH 2019 09 29.59862 02 17 14.06 -04 09 16.4 22.0z 14QZ510 T09 C~7znH 2019 10 04.61764 02 16 47.95 -04 12 07.3 23.0z 14QZ510 T09 C~83CO 2019 10 04.62530 02 16 47.92 -04 12 07.6 22.8z 14QZ510 T09 C~83CO 2019 10 04.62913 02 16 47.89 -04 12 07.6 22.8z 14QZ510 T09 C~83CO 2019 10 04.63679 02 16 47.85 -04 12 07.8 22.5z 14QZ510 T09 C~83CO 2021 11 11.354216 02 26 33.700 -01 51 12.99 22.9w 14QZ510 F51 C~5BU6 2021 11 11.379714 02 26 33.553 -01 51 13.40 23.0w 14QZ510 F51 C~5BU6 2021 11 11.392429 02 26 33.484 -01 51 13.34 22.8w 14QZ510 F51 C~5BU6
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 0.05 0.00 0.07
2 0.0000 0.00 0.03 0.00 0.07
3 0.1010 0.00 0.02 0.00 0.01
4 0.1010 0.00 0.04 0.00 0.04
5 0.1232 0.00 -0.03 0.00 -0.00
6 0.1232 0.00 0.01 0.00 0.01
7 0.3170 0.00 -0.06 0.00 -0.04
8 0.3170 0.00 -0.02 0.00 -0.04
9 0.3225 0.00 0.06 0.00 -0.05
10 0.3225 0.00 0.11 0.00 -0.08
11 0.3225 0.00 0.12 0.00 0.01
12 0.3225 0.00 0.06 0.00 0.03
13 0.3523 0.00 0.07 0.00 0.01
14 0.9967 0.00 -0.03 0.00 0.04
15 0.9994 0.00 0.01 0.00 0.05
16 1.0131 0.00 0.02 0.00 0.03
17 1.0676 0.00 -0.08 0.00 -0.02
18 1.0676 0.00 -0.08 0.00 0.02
19 1.0948 0.00 -0.11 0.00 0.16
20 1.2015 0.00 0.01 0.00 0.05
21 1.2015 0.00 0.08 0.00 0.10
22 1.2041 0.00 0.06 0.00 0.09
23 1.2152 0.00 0.09 0.00 0.00
24 1.2152 0.00 0.03 0.00 -0.01
25 1.2179 0.00 0.02 0.00 -0.00
26 1.2179 0.00 -0.04 0.00 -0.03
27 1.2180 0.00 -0.00 0.00 -0.04
28 1.2180 0.00 -0.03 0.00 -0.20
29 1.2206 0.00 -0.18 0.00 -0.07
30 1.2206 0.00 -0.11 0.00 -0.03
31 1.2396 0.00 -0.15 0.00 -0.04
32 1.2396 0.00 -0.13 0.00 -0.00
33 1.2396 0.00 -0.02 0.00 -0.10
34 1.2396 0.00 -0.06 0.00 -0.05
35 1.2396 0.00 -0.05 0.00 0.11
36 1.2396 0.00 -0.01 0.00 0.14
37 2.1243 0.00 0.08 0.00 0.01
38 2.1243 0.00 0.07 0.00 -0.00
39 2.1243 0.00 0.20 0.00 -0.04
40 2.1243 0.00 0.14 0.00 -0.05
41 2.1243 0.00 0.02 0.00 -0.10
42 2.1243 0.00 0.07 0.00 -0.10
43 2.1243 0.00 -0.05 0.00 -0.05
44 2.1243 0.00 -0.03 0.00 -0.05
45 2.1243 0.00 0.07 0.00 0.09
46 2.1243 0.00 0.03 0.00 0.03
47 2.1243 0.00 0.04 0.00 0.14
48 2.1243 0.00 0.03 0.00 0.08
49 2.1243 0.00 -0.02 0.00 -0.03
50 2.1764 0.00 -0.01 0.00 -0.10
51 2.1764 0.00 -0.04 0.00 -0.08
52 2.1789 0.00 -0.09 0.00 -0.09
53 2.1789 0.00 -0.02 0.00 -0.09
54 2.1789 0.00 -0.12 0.00 0.14
55 2.1789 0.00 -0.04 0.00 0.13
56 2.2935 0.00 0.10 0.00 0.14
57 2.2935 0.00 0.13 0.00 0.11
58 3.1972 0.00 0.04 0.00 -0.12
59 3.1972 0.00 0.08 0.00 -0.01
60 3.2739 0.00 0.19 0.00 -0.13
61 3.2739 0.00 0.04 0.00 -0.09
62 3.2740 0.00 0.09 0.00 0.01
63 3.3013 0.00 -0.05 0.00 -0.05
64 3.3422 0.00 0.02 0.00 -0.07
65 3.3422 0.00 -0.02 0.00 -0.15
66 3.3504 0.00 0.01 0.00 -0.06
67 4.0604 0.00 -0.07 0.00 -0.15
68 5.1118 0.00 0.20 0.00 0.12
69 5.1118 0.00 0.13 0.00 0.21
70 5.1119 0.00 -0.13 0.00 0.20
71 5.1119 0.00 0.16 0.00 0.14
72 5.1120 0.00 -0.00 0.00 -0.13
73 5.1120 0.00 -0.16 0.00 0.01
74 5.1121 0.00 0.21 0.00 0.04
75 5.1122 0.00 -0.19 0.00 -0.05
76 5.1122 0.00 -0.20 0.00 -0.39
77 5.1260 0.00 -0.13 0.00 0.18
78 5.1260 0.00 0.04 0.00 0.14
79 5.1260 0.00 -0.10 0.00 0.27
80 5.1260 0.00 -0.08 0.00 0.33
81 7.2306 0.00 -0.06 0.00 -0.21
82 7.2307 0.00 0.03 0.00 -0.23
83 7.2307 0.00 0.14 0.00 0.03
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.
14QZ510 quality flag:3 Type: 3:2E 3:2E 3:2E axisobj 39.676 39.676 39.676 ecceobj 0.245 0.245 0.245 incobj 23.732 23.732 23.732 qmin 28.905 28.912 28.902 qmax 50.754 50.824 50.701 amean 39.455 39.455 39.455 amin 38.946 38.946 38.946 amax 40.033 40.042 40.033 emean 0.241 0.241 0.241 emin 0.217 0.217 0.217 emax 0.269 0.269 0.268 imean 22.234 22.234 22.234 imin 21.773 21.768 21.777 imax 22.684 22.684 22.684 excite_mean 0.449 0.449 0.449 fracstop 1.000 1.000 1.000 cjmean 2.820 2.820 2.820 libcent 0 179.9 179.7 179.7 libamp 0 110.2 110.0 110.0 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 268.2 268.2 268.2 kozaiamp 20.0 20.0 20.0