Orbit Fit and Astrometric record for 19GJ186

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: 19GJ186   
# Created Wed Jul 17 01:11:39 2024
# Orbit generated from Bernstein formalism
# Fitting     13 observations of     13
# Arc:  83.97d
# First observation: 2019/01/11
#  Last observation: 2019/04/05
Preliminary a, adot, b, bdot, g, gdot:
  -0.000000   0.028318  -0.000000  -0.009662   0.027613   0.000000
# WARNING Fitting with energy constraint
# Chi-squared of fit:     5.65 DOF:     21 RMS:  0.12
# Min/Max residuals:    -0.27    0.21
# Exact a, adot, b, bdot, g, gdot:
  1.297382E-05  2.172417E-02 -6.451598E-06 -9.784164E-03  2.630237E-02  9.087547E-03
# Covariance matrix:
  4.1293E-12  6.6941E-09  1.9395E-13  2.1576E-10  1.1339E-09 -8.9220E-09
  6.6941E-09  1.1914E-05  3.4542E-10  3.8488E-07  2.0154E-06 -1.6289E-05
  1.9395E-13  3.4542E-10  3.7569E-13  9.7304E-12  5.8062E-11 -5.4474E-10
  2.1576E-10  3.8488E-07  9.7304E-12  1.2964E-08  6.3988E-08 -7.4507E-07
  1.1339E-09  2.0154E-06  5.8062E-11  6.3988E-08  3.4335E-07 -2.2839E-06
 -8.9220E-09 -1.6289E-05 -5.4474E-10 -7.4507E-07 -2.2839E-06  1.1440E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
   -6.633558  166.034664    0.815435   -0.064914   -0.558939  2458495.042281
# Heliocentric elements and errors
Epoch:              2458490.5000  =  2019/01/07
Mean Anomaly:           84.81203 +/-    59.382
Argument of Peri:       72.85940 +/-    32.268
Long of Asc Node:      330.65186 +/-     2.260
Inclination:            25.07437 +/-     3.402
Eccentricity:         0.34410920 +/-    0.3380
Semi-Major Axis:     35.62551595 +/-    7.8260
Time of Perihelion: 2440192.8579 +/-   11303.8
Perihelion:          23.36644828 +/-   13.0897
Aphelion:            47.88458362 +/-   15.9888
Period (y)              212.6424 +/-     70.07
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -36.99713016 +/-    0.8164
Ecliptic Y           10.03317269 +/-    0.2031
Ecliptic Z           -4.39223725 +/-    0.0979
Ecliptic XDOT        -0.00133547 +/-    0.0010
Ecliptic YDOT        -0.00199798 +/-    0.0005
Ecliptic ZDOT        -0.00112111 +/-    0.0001
# Distances at JD0 (AU)
Heliocenter to KBO   38.58424474 +/-    0.7847
Geocenter to KBO     38.01939405 +/-    0.8470
# Hcoef:  9.83

The following table shows the complete astrometric record for 19GJ186. 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 (19GJ186) followed by the observatory code and reference code for the source of the astrometry.

2019 01  11.54148  10 58 19.04   -00 36 33.0   25.3z 19GJ186   T09  C~870l      
2019 01  11.57352  10 58 18.93   -00 36 33.0   25.2z 19GJ186   T09  C~870l      
2019 01  11.58707  10 58 18.90   -00 36 33.0   25.2z 19GJ186   T09  C~870l      
2019 01  11.61693  10 58 18.81   -00 36 33.0   25.2z 19GJ186   T09  C~870l      
2019 04  04.38985  10 51 55.66   -00 08 26.7   26.2g 19GJ186   T09  C~870l      
2019 04  04.41725  10 51 55.53   -00 08 26.0   25.9g 19GJ186   T09  C~870l      
2019 04  04.42780  10 51 55.50   -00 08 25.8   26.0g 19GJ186   T09  C~870l      
2019 04  05.38960  10 51 51.36   -00 08 00.3   26.2r 19GJ186   T09  C~870l      
2019 04  05.42197  10 51 51.23   -00 07 59.3   26.4r 19GJ186   T09  C~870l      
2019 04  05.43532  10 51 51.18   -00 07 58.9   25.6r 19GJ186   T09  C~870l      
2019 04  05.46680  10 51 51.05   -00 07 58.3   25.8r 19GJ186   T09  C~870l      
2019 04  05.50116  10 51 50.91   -00 07 57.3   25.6r 19GJ186   T09  C~870l      
2019 04  05.51163  10 51 50.84   -00 07 57.3   26.0r 19GJ186   T09  C~870l      

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     0.12
     2   0.0001     -1.52    -0.13      -0.64    -0.04
     3   0.0001     -1.94     0.04      -0.81    -0.01
     4   0.0002     -3.18     0.07      -1.33    -0.08
     5   0.2268  -5957.37     0.02    -665.22     0.05
     6   0.2269  -5959.44    -0.11    -665.33    -0.03
     7   0.2269  -5959.93     0.15    -665.31    -0.01
     8   0.2296  -6027.12    -0.22    -665.78    -0.11
     9   0.2297  -6029.31    -0.13    -665.61     0.08
    10   0.2297  -6030.15    -0.04    -665.53     0.17
    11   0.2298  -6032.19     0.14    -665.73    -0.01
    12   0.2299  -6034.51     0.21    -665.62     0.13
    13   0.2299  -6035.48    -0.03    -666.03    -0.27

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.