Orbit Fit and Astrometric record for 16GA371

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: 16GA371   
# Created Wed Nov 27 02:10:38 2024
# Orbit generated from Bernstein formalism
# Fitting     18 observations of     18
# Arc:  34.95d
# First observation: 2016/03/07
#  Last observation: 2016/04/11
Preliminary a, adot, b, bdot, g, gdot:
   0.000001   0.031920  -0.000002   0.004031   0.027762   0.000000
# Chi-squared of fit:     6.73 DOF:     30 RMS:  0.11
# Min/Max residuals:    -0.20    0.25
# Exact a, adot, b, bdot, g, gdot:
  1.689239E-05  2.889162E-02  3.482150E-06  4.287301E-03  2.706922E-02 -1.946386E-04
# Covariance matrix:
  3.7034E-13  6.4228E-11 -7.0037E-14 -5.3921E-12  1.6155E-11  1.9986E-09
  6.4228E-11  1.8752E-07 -1.3773E-10 -1.7623E-08  3.7986E-08  2.2739E-06
 -7.0037E-14 -1.3773E-10  3.6404E-13  9.7950E-12 -2.8504E-11 -1.9481E-09
 -5.3921E-12 -1.7623E-08  9.7950E-12  1.7150E-09 -3.5443E-09 -2.0140E-07
  1.6155E-11  3.7986E-08 -2.8504E-11 -3.5443E-09  7.7704E-09  4.9490E-07
  1.9986E-09  2.2739E-06 -1.9481E-09 -2.0140E-07  4.9490E-07  4.3462E-05
#      lat0       lon0       xBary       yBary       zBary        JD0
   12.801151 -150.717573    0.664587    0.162514   -0.714600  2457455.103509
# Heliocentric elements and errors
Epoch:              2457450.5000  =  2016/03/03
Mean Anomaly:          349.85279 +/-    95.085
Argument of Peri:       68.90605 +/-   121.329
Long of Asc Node:      153.19270 +/-     0.591
Inclination:            15.19483 +/-     0.105
Eccentricity:         0.11767800 +/-    0.0339
Semi-Major Axis:     42.57762336 +/-    0.8036
Time of Perihelion: 2460310.8207 +/-   26802.8
Perihelion:          37.56717392 +/-    1.6071
Aphelion:            47.58807281 +/-    1.6991
Period (y)              277.8308 +/-      7.87
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -32.38863875 +/-    0.1023
Ecliptic Y          -17.40111404 +/-    0.0574
Ecliptic Z            8.18538672 +/-    0.0267
Ecliptic XDOT         0.00152969 +/-    0.0006
Ecliptic YDOT        -0.00249937 +/-    0.0003
Ecliptic ZDOT         0.00041850 +/-    0.0001
# Distances at JD0 (AU)
Heliocenter to KBO   37.66727021 +/-    0.0921
Geocenter to KBO     36.94232792 +/-    0.1203
# Hcoef:  8.65

The following table shows the complete astrometric record for 16GA371. 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 (16GA371) followed by the observatory code and reference code for the source of the astrometry.

2016 03  07.60272  14 06 53.04   +00 46 37.4   25.1g 16GA371   T09  C~8DkA      
2016 03  07.61343  14 06 53.01   +00 46 37.9   25.1g 16GA371   T09  C~8DkA      
2016 03  07.63334  14 06 52.95   +00 46 38.8   24.9g 16GA371   T09  C~8DkA      
2016 03  07.64836  14 06 52.91   +00 46 39.3   25.0g 16GA371   T09  C~8DkA      
2016 03  16.48011  14 06 23.34   +00 51 51.9   24.2z 16GA371   T09  C~8DkA      
2016 03  16.55457  14 06 23.03   +00 51 54.4   24.7z 16GA371   T09  C~8DkA      
2016 03  16.57907  14 06 22.94   +00 51 55.4   23.9z 16GA371   T09  C~8DkA      
2016 04  08.53825  14 04 44.63   +01 05 21.9   23.6r 16GA371   T09  C~8DkA      
2016 04  08.54109  14 04 44.63   +01 05 22.1   24.4r 16GA371   T09  C~8DkA      
2016 04  08.54958  14 04 44.59   +01 05 22.4   24.1r 16GA371   T09  C~8DkA      
2016 04  08.56247  14 04 44.53   +01 05 22.9   24.4r 16GA371   T09  C~8DkA      
2016 04  11.44440  14 04 30.74   +01 06 58.3   23.7i 16GA371   T09  C~8DkA      
2016 04  11.46760  14 04 30.62   +01 06 58.9   24.6i 16GA371   T09  C~8DkA      
2016 04  11.48411  14 04 30.53   +01 06 59.4   24.4i 16GA371   T09  C~8DkA      
2016 04  11.49226  14 04 30.51   +01 06 59.6   23.9i 16GA371   T09  C~8DkA      
2016 04  11.51385  14 04 30.39   +01 07 00.5   23.9i 16GA371   T09  C~8DkB      
2016 04  11.53541  14 04 30.29   +01 07 01.1   24.4i 16GA371   T09  C~8DkB      
2016 04  11.55443  14 04 30.20   +01 07 01.6   24.0i 16GA371   T09  C~8DkB      

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    -0.00       0.00    -0.20
     2   0.0000     -0.60    -0.00       0.31    -0.07
     3   0.0001     -1.75    -0.05       0.84     0.14
     4   0.0001     -2.49     0.05       1.11     0.15
     5   0.0243   -526.90     0.25     140.41     0.15
     6   0.0245   -532.13    -0.12     141.14    -0.16
     7   0.0246   -533.74    -0.14     141.61    -0.03
     8   0.0874  -2196.48    -0.12     386.56    -0.13
     9   0.0874  -2196.55     0.04     386.75     0.04
    10   0.0875  -2197.21     0.05     386.82     0.06
    11   0.0875  -2198.23     0.06     386.98     0.13
    12   0.0954  -2425.32    -0.01     404.73     0.16
    13   0.0955  -2427.22    -0.04     404.67    -0.02
    14   0.0955  -2428.66    -0.15     404.67    -0.10
    15   0.0955  -2429.01     0.16     404.76    -0.06
    16   0.0956  -2431.01    -0.10     404.98     0.05
    17   0.0956  -2432.63     0.01     405.02    -0.01
    18   0.0957  -2434.06     0.10     405.02    -0.11

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.