Orbit Fit and Astrometric record for 10TG192

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: 10TG192   
# Created Fri Apr 19 01:13:36 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     23 observations of     23
# Arc:  18.19y
# First observation: 2004/09/21
#  Last observation: 2022/12/01
# Chi-squared of fit:    13.97 DOF:     40 RMS:  0.14
# Min/Max residuals:    -0.30    0.27
# Exact a, adot, b, bdot, g, gdot:
  1.579895E-05  2.402372E-02  8.523194E-07  1.580588E-04  2.422566E-02  1.277264E-03
# Covariance matrix:
  4.6522E-13 -9.4706E-14  2.1163E-15 -5.1982E-16 -7.5722E-14 -1.5198E-13
 -9.4706E-14  3.6072E-14 -1.1578E-15  1.6816E-16  1.3222E-13  5.6209E-14
  2.1163E-15 -1.1578E-15  2.1283E-13 -1.7851E-14 -5.9370E-15 -1.7567E-15
 -5.1982E-16  1.6816E-16 -1.7851E-14  2.1011E-15  2.5802E-16  3.2225E-16
 -7.5722E-14  1.3222E-13 -5.9370E-15  2.5802E-16  1.1502E-12  1.4820E-13
 -1.5198E-13  5.6209E-14 -1.7567E-15  3.2225E-16  1.4820E-13  1.0083E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
    1.278863   47.906875    0.764924    0.014728   -0.656447  2453269.817659
# Heliocentric elements and errors
Epoch:              2453270.5000  =  2004/09/22
Mean Anomaly:           34.24590 +/-     0.072
Argument of Peri:       34.08710 +/-     0.082
Long of Asc Node:      334.75266 +/-     0.005
Inclination:             1.32267 +/-     0.000
Eccentricity:         0.05543980 +/-    0.0001
Semi-Major Axis:     43.90623202 +/-    0.0078
Time of Perihelion: 2443161.8368 +/-      21.6
Perihelion:          41.47207921 +/-    0.0086
Aphelion:            46.34038482 +/-    0.0093
Period (y)              290.9360 +/-      0.08
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           28.66677350 +/-    0.0012
Ecliptic Y           30.59932928 +/-    0.0014
Ecliptic Z            0.92133168 +/-    0.0000
Ecliptic XDOT        -0.00191987 +/-    0.0000
Ecliptic YDOT         0.00191971 +/-    0.0000
Ecliptic ZDOT         0.00002118 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.93983711 +/-    0.0013
Geocenter to KBO     41.27854226 +/-    0.0018
# Hcoef:  6.53

The following table shows the complete astrometric record for 10TG192. 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 (10TG192) followed by the observatory code and reference code for the source of the astrometry.

2004 09  21.316916 03 00 16.45   +18 23 44.2         10TG192   645  C~2POO      
2004 09  21.317746 03 00 16.45   +18 23 44.2         10TG192   645  C~2POO      
2004 09  21.320233 03 00 16.44   +18 23 44.2         10TG192   645  C~2POO      
2010 10  09.42936  03 32 54.648  +20 31 02.85  23.3w 10TG192   F51  C~1w3k      
2010 10  09.44545  03 32 54.585  +20 31 02.93  23.0w 10TG192   F51  C~1w3k      
2010 10  09.46161  03 32 54.531  +20 31 02.87  23.5w 10TG192   F51  C~1w3k      
2010 11  07.48051  03 30 45.152  +20 23 59.90  23.1w 10TG192   F51  C~1w3k      
2010 11  07.49400  03 30 45.069  +20 23 59.52  23.2w 10TG192   F51  C~1w3k      
2010 11  07.50872  03 30 45.017  +20 23 59.40  23.2w 10TG192   F51  C~1w3k      
2010 11  07.52219  03 30 44.935  +20 23 58.90  23.4w 10TG192   F51  C~1w3k      
2011 10  24.55843  03 37 34.405  +20 47 25.10  23.6w 10TG192   F51  C~1w3k      
2011 11  30.30447  03 34 32.921  +20 37 23.69  22.0i 10TG192   F51  C~1w3k      
2012 10  22.54508  03 43 22.121  +21 06 36.01  22.6w 10TG192   F51  C~1w3k      
2012 10  22.55961  03 43 22.066  +21 06 36.01  23.0w 10TG192   F51  C~1w3k      
2012 10  22.57409  03 43 22.000  +21 06 35.80  23.0w 10TG192   F51  C~1w3k      
2012 10  22.58856  03 43 21.939  +21 06 35.64  22.9w 10TG192   F51  C~1w3k      
2013 12  03.29208  03 45 40.677  +21 14 21.66  22.4w 10TG192   F51  C~1w3k      
2013 12  03.32034  03 45 40.506  +21 14 21.37  22.7w 10TG192   F51  C~1w3k      
2013 12  03.33452  03 45 40.424  +21 14 20.95  22.9w 10TG192   F51  C~1w3k      
2022 12  01.478119 04 37 33.238  +23 26 36.45  22.8w 10TG192   F52  C~671d      
2022 12  01.490309 04 37 33.168  +23 26 36.23  22.9w 10TG192   F52  C~671d      
2022 12  01.502582 04 37 33.128  +23 26 36.21  22.7w 10TG192   F52  C~671d      
2022 12  01.514828 04 37 33.055  +23 26 36.07  22.6w 10TG192   F52  C~671d      

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    -0.16
     2   0.0000      0.00     0.06       0.00    -0.15
     3   0.0000      0.00     0.02       0.00    -0.12
     4   6.0482      0.00     0.06       0.00    -0.15
     5   6.0483      0.00     0.02       0.00     0.11
     6   6.0483      0.00     0.13       0.00     0.24
     7   6.1278      0.00    -0.02       0.00     0.14
     8   6.1278      0.00    -0.24       0.00    -0.01
     9   6.1278      0.00     0.10       0.00     0.12
    10   6.1279      0.00    -0.11       0.00    -0.15
    11   7.0890      0.00     0.15       0.00    -0.11
    12   7.1896      0.00     0.21       0.00     0.19
    13   8.0855      0.00    -0.21       0.00    -0.12
    14   8.0855      0.00    -0.06       0.00     0.07
    15   8.0856      0.00    -0.08       0.00     0.05
    16   8.0856      0.00    -0.03       0.00     0.08
    17   9.1991      0.00     0.27       0.00     0.03
    18   9.1992      0.00    -0.15       0.00     0.19
    19   9.1992      0.00    -0.30       0.00    -0.00
    20  18.1935      0.00    -0.09       0.00    -0.06
    21  18.1935      0.00    -0.17       0.00    -0.15
    22  18.1935      0.00     0.22       0.00    -0.04
    23  18.1936      0.00     0.10       0.00    -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.

10TG192    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.394    44.394    44.394
ecceobj         0.066     0.066     0.066
incobj          1.320     1.320     1.320
qmin           40.504    40.502    40.507
qmax           47.780    47.787    47.781
amean          44.040    44.040    44.040
amin           43.693    43.694    43.694
amax           44.398    44.398    44.400
emean           0.061     0.061     0.061
emin            0.044     0.044     0.044
emax            0.077     0.077     0.077
imean           2.567     2.567     2.567
imin            1.810     1.811     1.810
imax            3.236     3.236     3.235
excite_mean     0.076     0.076     0.076
fracstop        1.000     1.000     1.000
cjmean          3.095     3.095     3.095

libcent 0      -180.0    -180.0    -180.0
libamp  0      -180.0    -180.0    -180.0
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       184.0     184.0     183.9
kozaiamp        180.0     180.0     179.9