Orbit Fit and Astrometric record for 16GK370

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: 16GK370   
# Created Wed Nov 27 02:10:38 2024
# Orbit generated from Bernstein formalism
# Fitting     18 observations of     18
# Arc:  63.95d
# First observation: 2016/04/02
#  Last observation: 2016/06/05
Preliminary a, adot, b, bdot, g, gdot:
  -0.000001   0.038348  -0.000000   0.000547   0.030564   0.000000
# WARNING Fitting with energy constraint
# Chi-squared of fit:     8.11 DOF:     31 RMS:  0.12
# Min/Max residuals:    -0.24    0.23
# Exact a, adot, b, bdot, g, gdot:
  1.642591E-05  3.071555E-02  3.055183E-07  3.083654E-04  2.941753E-02  1.772400E-02
# Covariance matrix:
  3.8997E-13  2.5142E-10 -7.5275E-15  7.6623E-12  4.7504E-11 -1.8535E-09
  2.5142E-10  4.1406E-07 -1.3363E-11  1.2806E-08  6.8192E-08 -5.4902E-06
 -7.5275E-15 -1.3363E-11  1.6642E-13 -1.3842E-12 -2.1485E-12  1.9034E-10
  7.6623E-12  1.2806E-08 -1.3842E-12  4.0778E-10  2.0970E-09 -1.7288E-07
  4.7504E-11  6.8192E-08 -2.1485E-12  2.0970E-09  1.1733E-08 -7.7782E-07
 -1.8535E-09 -5.4902E-06  1.9034E-10 -1.7288E-07 -7.7782E-07  1.0459E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
    2.160648 -175.050035   -0.135594    0.037326   -0.985631  2457480.890769
# Heliocentric elements and errors
Epoch:              2457480.5000  =  2016/04/02
Mean Anomaly:           31.11377 +/-    24.355
Argument of Peri:      340.59783 +/-     1.587
Long of Asc Node:      111.17540 +/-     0.358
Inclination:             2.18406 +/-     0.004
Eccentricity:         0.56255827 +/-    0.3166
Semi-Major Axis:     49.46589883 +/-   24.4334
Time of Perihelion: 2446497.8435 +/-    2774.0
Perihelion:          21.63844833 +/-   18.9597
Aphelion:            77.29334934 +/-   41.2655
Period (y)              347.9101 +/-    257.77
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -34.81715545 +/-    0.1246
Ecliptic Y           -3.15385176 +/-    0.0108
Ecliptic Z            1.28163248 +/-    0.0047
Ecliptic XDOT        -0.00139438 +/-    0.0010
Ecliptic YDOT        -0.00299711 +/-    0.0000
Ecliptic ZDOT         0.00009088 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   34.98319134 +/-    0.1240
Geocenter to KBO     33.99333253 +/-    0.1252
# Hcoef: 10.10

The following table shows the complete astrometric record for 16GK370. 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 (16GK370) followed by the observatory code and reference code for the source of the astrometry.

2016 04  02.38998  12 21 35.97   +00 01 00.3   25.1i 16GK370   T09  C~8AhT      
2016 04  02.41732  12 21 35.83   +00 01 01.3   25.2i 16GK370   T09  C~8AhT      
2016 04  02.44189  12 21 35.69   +00 01 02.2   24.8i 16GK370   T09  C~8AhT      
2016 04  02.50172  12 21 35.36   +00 01 04.0   25.4i 16GK370   T09  C~8AhT      
2016 04  02.51521  12 21 35.31   +00 01 04.5   25.4i 16GK370   T09  C~8AhT      
2016 04  02.52328  12 21 35.24   +00 01 04.7   24.7i 16GK370   T09  C~8AhT      
2016 04  04.40648  12 21 25.33   +00 02 08.4   26.3g 16GK370   T09  C~8AhT      
2016 04  04.41295  12 21 25.29   +00 02 08.7   26.6g 16GK370   T09  C~8AhT      
2016 04  04.41948  12 21 25.27   +00 02 08.9   26.3g 16GK370   T09  C~8AhT      
2016 06  04.26227  12 17 43.85   +00 23 42.1   25.3z 16GK370   T09  C~8AhT      
2016 06  04.27037  12 17 43.84   +00 23 42.1   25.2z 16GK370   T09  C~8AhT      
2016 06  04.28656  12 17 43.82   +00 23 42.2   25.0z 16GK370   T09  C~8AhT      
2016 06  04.28926  12 17 43.80   +00 23 42.1   24.7z 16GK370   T09  C~8AhT      
2016 06  04.32707  12 17 43.77   +00 23 42.6   25.4z 16GK370   T09  C~8AhT      
2016 06  04.34327  12 17 43.75   +00 23 42.6   25.2z 16GK370   T09  C~8AhT      
2016 06  05.31720  12 17 42.63   +00 23 46.4   25.5r 16GK370   T09  C~8AhT      
2016 06  05.33917  12 17 42.61   +00 23 46.4   26.2r 16GK370   T09  C~8AhT      
2016 06  05.34340  12 17 42.59   +00 23 46.1   26.4r 16GK370   T09  C~8AhT      

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     0.02       0.00    -0.03
     2   0.0001     -2.32     0.09       0.09     0.08
     3   0.0001     -4.61    -0.04       0.08     0.10
     4   0.0003     -9.87    -0.06      -0.23    -0.16
     5   0.0003    -10.75     0.23      -0.07     0.02
     6   0.0004    -11.80    -0.10      -0.30    -0.21
     7   0.0055   -173.52    -0.05      -0.72     0.02
     8   0.0055   -174.19    -0.16      -0.69     0.06
     9   0.0056   -174.54     0.06      -0.62     0.13
    10   0.1721  -3736.78     0.06    -129.44    -0.05
    11   0.1722  -3736.92     0.08    -129.50    -0.07
    12   0.1722  -3737.23     0.08    -129.52    -0.04
    13   0.1722  -3737.47    -0.10    -129.74    -0.24
    14   0.1723  -3738.08     0.02    -129.45     0.19
    15   0.1724  -3738.36     0.05    -129.57     0.13
    16   0.1750  -3755.29    -0.11    -132.74     0.17
    17   0.1751  -3755.57     0.00    -132.86     0.14
    18   0.1751  -3755.73    -0.08    -133.26    -0.24

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.