Orbit Fit and Astrometric record for 16GV368

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: 16GV368   
# Created Wed Nov 27 02:10:37 2024
# Orbit generated from Bernstein formalism
# Fitting     18 observations of     18
# Arc:  63.93d
# First observation: 2016/04/02
#  Last observation: 2016/06/05
Preliminary a, adot, b, bdot, g, gdot:
  -0.000001   0.021990   0.000002   0.000037   0.021767   0.000000
# WARNING Fitting with energy constraint
# Chi-squared of fit:     5.53 DOF:     31 RMS:  0.10
# Min/Max residuals:    -0.36    0.17
# Exact a, adot, b, bdot, g, gdot:
  1.323846E-05  1.842052E-02  1.730371E-06 -7.225486E-06  2.122342E-02 -3.741862E-03
# Covariance matrix:
  6.8034E-13  4.9006E-10 -8.6581E-15  5.9197E-12  8.5700E-11 -6.7945E-09
  4.9006E-10  7.6629E-07 -1.4488E-11  9.4216E-09  1.1690E-07 -1.6135E-05
 -8.6581E-15 -1.4488E-11  1.8824E-13 -1.2798E-12 -2.1721E-12  3.1761E-10
  5.9197E-12  9.4216E-09 -1.2798E-12  1.2745E-10  1.4301E-09 -2.0076E-07
  8.5700E-11  1.1690E-07 -2.1721E-12  1.4301E-09  1.8487E-08 -2.2463E-06
 -6.7945E-09 -1.6135E-05  3.1761E-10 -2.0076E-07 -2.2463E-06  4.1062E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
    0.842927 -174.895855   -0.133272    0.014653   -0.986552  2457480.909989
# Heliocentric elements and errors
Epoch:              2457480.5000  =  2016/04/02
Mean Anomaly:          269.96468 +/-   188.726
Argument of Peri:      204.24330 +/-   131.184
Long of Asc Node:       93.30864 +/-     1.492
Inclination:             0.82618 +/-     0.001
Eccentricity:         0.19921113 +/-    0.9159
Semi-Major Axis:     46.31182036 +/-   20.9409
Time of Perihelion: 2486270.8280 +/-   57101.7
Perihelion:          37.08599027 +/-   45.6124
Aphelion:            55.53765045 +/-   49.2943
Period (y)              315.1708 +/-    213.77
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -47.90045156 +/-    0.3006
Ecliptic Y           -4.41463220 +/-    0.0268
Ecliptic Z            0.69327041 +/-    0.0044
Ecliptic XDOT         0.00069224 +/-    0.0026
Ecliptic YDOT        -0.00233089 +/-    0.0001
Ecliptic ZDOT        -0.00000803 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   48.10844896 +/-    0.2993
Geocenter to KBO     47.11776473 +/-    0.3019
# Hcoef:  7.76

The following table shows the complete astrometric record for 16GV368. 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 (16GV368) followed by the observatory code and reference code for the source of the astrometry.

2016 04  02.40920  12 20 04.60   -01 15 15.0   24.0i 16GV368   T09  C~89Td      
2016 04  02.48554  12 20 04.30   -01 15 12.6   24.5i 16GV368   T09  C~89Td      
2016 04  02.49093  12 20 04.27   -01 15 12.6   24.3i 16GV368   T09  C~89Td      
2016 04  02.50710  12 20 04.21   -01 15 12.1   23.9i 16GV368   T09  C~89Td      
2016 04  04.33742  12 19 57.02   -01 14 25.9   25.4g 16GV368   T09  C~89Td      
2016 04  04.34027  12 19 57.01   -01 14 25.6   25.9g 16GV368   T09  C~89Td      
2016 04  04.36164  12 19 56.93   -01 14 25.1   25.4g 16GV368   T09  C~89Td      
2016 04  04.38302  12 19 56.84   -01 14 24.7   25.1g 16GV368   T09  C~89Td      
2016 06  04.24853  12 17 08.71   -00 56 59.2   24.0z 16GV368   T09  C~89Td      
2016 06  04.26496  12 17 08.68   -00 56 59.0   24.5z 16GV368   T09  C~89Td      
2016 06  04.26765  12 17 08.68   -00 56 59.0   24.4z 16GV368   T09  C~89Td      
2016 06  04.28388  12 17 08.66   -00 56 58.8   24.3z 16GV368   T09  C~89Td      
2016 06  04.30006  12 17 08.65   -00 56 58.8   24.1z 16GV368   T09  C~89Td      
2016 06  04.32166  12 17 08.63   -00 56 58.8   24.0z 16GV368   T09  C~89Td      
2016 06  04.33517  12 17 08.62   -00 56 58.7   24.3z 16GV368   T09  C~89Td      
2016 06  05.30579  12 17 07.68   -00 56 53.6   24.5r 16GV368   T09  C~89Td      
2016 06  05.32218  12 17 07.67   -00 56 53.6   24.6r 16GV368   T09  C~89Td      
2016 06  05.33492  12 17 07.64   -00 56 53.5   24.7r 16GV368   T09  C~89Td      

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     0.10       0.00    -0.36
     2   0.0002     -5.08     0.01       0.42     0.11
     3   0.0002     -5.49    -0.05       0.24    -0.07
     4   0.0003     -6.52    -0.02       0.34     0.04
     5   0.0053   -123.82     0.00       0.03    -0.05
     6   0.0053   -124.08    -0.07       0.25     0.17
     7   0.0053   -125.38     0.02       0.23     0.16
     8   0.0054   -126.78     0.01       0.06     0.01
     9   0.1720  -2856.32     0.12     -39.66    -0.05
    10   0.1721  -2856.81    -0.10     -39.65    -0.02
    11   0.1721  -2856.81    -0.05     -39.65    -0.01
    12   0.1721  -2857.16    -0.13     -39.59     0.07
    13   0.1722  -2857.30     0.00     -39.65     0.04
    14   0.1722  -2857.58     0.09     -39.77    -0.05
    15   0.1723  -2857.75     0.14     -39.74    -0.00
    16   0.1749  -2872.72    -0.02     -40.64     0.05
    17   0.1750  -2872.86     0.10     -40.70     0.01
    18   0.1750  -2873.31    -0.15     -40.79    -0.06

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.