Orbit Fit and Astrometric record for 14OG392

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: 14OG392   
# Created Fri Nov 16 02:09:40 2018
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting  141 observations of  141
# Arc:   7.13y
# First observation: 2011/07/27
#  Last observation: 2018/09/11
# Chi-squared of fit:   186.48 DOF:  276 RMS:  0.20
# Min/Max residuals:    -0.80    1.25
# Exact a, adot, b, bdot, g, gdot:
  2.709516E-05  1.482919E-01 -3.625093E-06 -1.915249E-02  8.691627E-02 -3.017954E-02
# Covariance matrix:
  3.4559E-14 -8.5833E-15 -1.0079E-15  5.8877E-17  1.3796E-15 -8.3087E-16
 -8.5833E-15  2.6416E-15  3.9639E-17 -1.3317E-17 -2.1018E-16  2.0076E-17
 -1.0079E-15  3.9639E-17  2.9195E-14 -8.5641E-15 -9.7692E-16  1.8151E-16
  5.8877E-17 -1.3317E-17 -8.5641E-15  2.6575E-15  3.6861E-16 -2.4717E-17
  1.3796E-15 -2.1018E-16 -9.7692E-16  3.6861E-16  5.7528E-15 -4.4849E-16
 -8.3087E-16  2.0076E-17  1.8151E-16 -2.4717E-17 -4.4849E-16  1.3346E-16
#      lat0       lon0       xBary       yBary       zBary        JD0
    5.477033  -68.833965   -0.219565    0.094423   -0.985397  2455769.892316
# Heliocentric elements and errors
Epoch:              2455770.5000  =  2011/07/28
Mean Anomaly:          272.49299 +/-     0.000
Argument of Peri:      254.11221 +/-     0.000
Long of Asc Node:      145.90766 +/-     0.000
Inclination:             9.03320 +/-     0.000
Eccentricity:         0.18239748 +/-    0.0000
Semi-Major Axis:     12.18941264 +/-    0.0000
Time of Perihelion: 2459548.9436 +/-       0.0
Perihelion:           9.96609447 +/-    0.0000
Aphelion:            14.41273080 +/-    0.0000
Period (y)               42.5581 +/-      0.00
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X            4.70155814 +/-    0.0000
Ecliptic Y          -11.52339190 +/-    0.0000
Ecliptic Z            1.09815515 +/-    0.0000
Ecliptic XDOT         0.00403231 +/-    0.0000
Ecliptic YDOT         0.00252098 +/-    0.0000
Ecliptic ZDOT        -0.00069123 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   12.49402177 +/-    0.0000
Geocenter to KBO     11.50542594 +/-    0.0000
# Hcoef: 10.56

The following table shows the complete astrometric record for 14OG392. 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 (14OG392) followed by the observatory code and reference code for the source of the astrometry.

2011 07  27.39155  19 27 59.768  -16 21 37.39  20.8G 14OG392   F51  C~2jhX      
2011 07  27.40231  19 27 59.614  -16 21 38.08  20.9G 14OG392   F51  C~2jhX      
2012 08  04.33788  20 02 33.433  -16 06 47.87  20.9G 14OG392   F51  C~2jhX      
2012 11  06.21825  19 57 43.223  -17 05 16.90  21.5G 14OG392   F51  C~2jhX      
2013 07  02.50304  20 48 59.666  -14 41 04.37  21.4G 14OG392   F51  C~2jhX      
2013 07  06.49680  20 48 10.285  -14 44 49.65  21.0G 14OG392   F51  C~2jhX      
2013 07  12.48413  20 46 51.132  -14 50 53.75  21.8w 14OG392   F51  C~1vXe      
2013 07  12.48545  20 46 51.131  -14 50 53.48  21.4w 14OG392   F51  C~1vXe      
2013 07  12.49909  20 46 50.937  -14 50 54.73  21.6w 14OG392   F51  C~1vXe      
2013 07  12.50042  20 46 50.910  -14 50 54.74  21.7w 14OG392   F51  C~1vXe      
2013 07  12.51407  20 46 50.723  -14 50 55.62  21.7w 14OG392   F51  C~1vXe      
2013 07  12.51539  20 46 50.707  -14 50 55.80  21.6w 14OG392   F51  C~1vXe      
2013 07  12.52907  20 46 50.511  -14 50 56.66  21.7w 14OG392   F51  C~1vXe      
2013 07  12.53039  20 46 50.495  -14 50 56.66  21.8w 14OG392   F51  C~1vXe      
2013 08  03.44752  20 41 30.106  -15 16 21.58        14OG392   F51  C~2jhX      
2013 08  23.38260  20 36 43.624  -15 40 38.47  21.4G 14OG392   F51  C~2jhX      
2014 06  05.57079  21 31 39.376  -13 00 33.60  21.3G 14OG392   F51  C~2jhX      
2014 06  21.56403  21 30 31.726  -13 08 14.06  22.0G 14OG392   F51  C~2jhX      
2014 06  21.57534  21 30 31.661  -13 08 14.59  21.8G 14OG392   F51  C~2jhX      
2014 06  21.58664  21 30 31.582  -13 08 15.32  21.5G 14OG392   F51  C~2jhX      
2014 06  21.59792  21 30 31.499  -13 08 15.39  21.6G 14OG392   F51  C~2jhX      
2014 06  29.49076  21 29 30.237  -13 14 28.57  21.7G 14OG392   F51  C~2jhX      
2014 06  29.50305  21 29 30.136  -13 14 29.33  21.4G 14OG392   F51  C~2jhX      
2014 06  29.51532  21 29 30.015  -13 14 29.93  21.5G 14OG392   F51  C~2jhX      
2014 07  07.53551  21 28 10.979  -13 22 16.98  20.8G 14OG392   F51  C~2jhX      
2014 07  07.54732  21 28 10.864  -13 22 17.92  21.6G 14OG392   F51  C~2jhX      
2014 07  07.57097  21 28 10.580  -13 22 19.31  20.4G 14OG392   F51  C~2jhX      
2014 07  09.49929  21 27 49.380  -13 24 23.56  21.6G 14OG392   F51  C~2jhX      
2014 07  28.49510  21 23 43.338  -13 48 03.86  21.4w 14OG392   F51  C@0615      
2014 07  28.50639  21 23 43.180  -13 48 05.03  21.4w 14OG392   F51  C@0615      
2014 07  28.51768  21 23 43.009  -13 48 05.72  21.3w 14OG392   F51  C@0615      
2014 07  29.313162 21 23 31.61   -13 49 12.1   21.3V 14OG392   H21  C~17NO      
2014 07  29.326160 21 23 31.40   -13 49 12.3   20.9V 14OG392   H21  C~17NO      
2014 07  29.339079 21 23 31.25   -13 49 12.9         14OG392   H21  C~17NO      
2014 08  26.38179  21 16 37.385  -14 29 09.28  20.9G 14OG392   F51  C~2jhX      
2014 08  26.39372  21 16 37.210  -14 29 09.84  21.3G 14OG392   F51  C~2jhX      
2014 08  26.40563  21 16 37.035  -14 29 10.83  21.4G 14OG392   F51  C~2jhX      
2014 08  26.41753  21 16 36.875  -14 29 12.06  21.1G 14OG392   F51  C~2jhX      
2014 08  27.38508  21 16 23.216  -14 30 32.32  21.4G 14OG392   F51  C~2jhX      
2014 08  27.39871  21 16 23.022  -14 30 33.68  21.2G 14OG392   F51  C~2jhX      
2014 08  27.41231  21 16 22.838  -14 30 35.16  20.6G 14OG392   F51  C~2jhX      
2014 08  27.42594  21 16 22.643  -14 30 35.89  21.2G 14OG392   F51  C~2jhX      
2014 09  12.33254  21 12 58.935  -14 51 12.31  21.2G 14OG392   F51  C~2jhX      
2014 09  12.34418  21 12 58.801  -14 51 13.31  21.5G 14OG392   F51  C~2jhX      
2014 09  12.35582  21 12 58.664  -14 51 14.27  21.6G 14OG392   F51  C~2jhX      
2014 09  12.36741  21 12 58.525  -14 51 14.93  21.0G 14OG392   F51  C~2jhX      
2014 10  01.31651  21 10 10.251  -15 10 21.92  21.4G 14OG392   F51  C~2jhX      
2015 06  25.55263  22 11 11.900  -11 17 40.95  21.6w 14OG392   F51  C~1vXe      
2015 06  25.56378  22 11 11.850  -11 17 41.29  21.5w 14OG392   F51  C~1vXe      
2015 06  25.57493  22 11 11.796  -11 17 41.80  21.6w 14OG392   F51  C~1vXe      
2015 06  25.58612  22 11 11.740  -11 17 42.34  21.4w 14OG392   F51  C~1vXe      
2015 07  12.50026  22 09 15.348  -11 33 30.75  21.5w 14OG392   F51  C~1vXe      
2015 07  12.51139  22 09 15.246  -11 33 31.51  21.5w 14OG392   F51  C~1vXe      
2015 07  12.52254  22 09 15.141  -11 33 32.30  21.6w 14OG392   F51  C~1vXe      
2015 07  12.53369  22 09 15.027  -11 33 33.10  21.5w 14OG392   F51  C~1vXe      
2015 07  14.54315  22 08 55.930  -11 35 55.04  21.4w 14OG392   F51  C~1vXe      
2015 07  14.55458  22 08 55.816  -11 35 56.24  21.4w 14OG392   F51  C~1vXe      
2015 07  14.56593  22 08 55.713  -11 35 56.87  21.4w 14OG392   F51  C~1vXe      
2015 07  14.57721  22 08 55.608  -11 35 57.76  21.4w 14OG392   F51  C~1vXe      
2015 09  05.36937  21 56 58.841  -12 56 39.93  21.2G 14OG392   F51  C~2jhX      
2015 09  05.38033  21 56 58.684  -12 56 41.13  20.5G 14OG392   F51  C~2jhX      
2015 09  05.39155  21 56 58.516  -12 56 42.18  20.8G 14OG392   F51  C~2jhX      
2015 09  05.40262  21 56 58.368  -12 56 43.06  20.8G 14OG392   F51  C~2jhX      
2015 09  06.38096  21 56 44.525  -12 58 13.40  21.2G 14OG392   F51  C~2jhX      
2015 09  06.39219  21 56 44.363  -12 58 14.44  21.0G 14OG392   F51  C~2jhX      
2015 09  06.40339  21 56 44.201  -12 58 15.49  21.3G 14OG392   F51  C~2jhX      
2015 09  06.41459  21 56 44.041  -12 58 16.45  21.2G 14OG392   F51  C~2jhX      
2015 10  09.28711  21 50 42.741  -13 38 42.23  21.8G 14OG392   F51  C~2jhX      
2015 10  09.29876  21 50 42.656  -13 38 42.86  21.3G 14OG392   F51  C~2jhX      
2015 10  09.31241  21 50 42.554  -13 38 43.40  21.7G 14OG392   F51  C~2jhX      
2015 10  09.32408  21 50 42.471  -13 38 44.14  21.7G 14OG392   F51  C~2jhX      
2015 10  10.31402  21 50 35.851  -13 39 33.09  21.4G 14OG392   F51  C~2jhX      
2015 10  10.32499  21 50 35.768  -13 39 33.67  21.3G 14OG392   F51  C~2jhX      
2015 11  07.20156  21 49 43.015  -13 50 31.07  19.5G 14OG392   F51  C~2jhX      
2016 07  07.53556  22 53 00.604  -09 04 53.45  21.4G 14OG392   F51  C~2jhX      
2016 07  07.54681  22 53 00.546  -09 04 54.16  21.2G 14OG392   F51  C~2jhX      
2016 07  07.55802  22 53 00.495  -09 04 54.76  21.0G 14OG392   F51  C~2jhX      
2016 07  07.56922  22 53 00.436  -09 04 55.30  21.0G 14OG392   F51  C~2jhX      
2016 08  03.50968  22 49 13.286  -09 39 48.53  20.7G 14OG392   F51  C~2jhX      
2016 08  03.52071  22 49 13.150  -09 39 49.49  20.8G 14OG392   F51  C~2jhX      
2016 08  03.53177  22 49 13.014  -09 39 50.80  20.8G 14OG392   F51  C~2jhX      
2016 08  03.54282  22 49 12.881  -09 39 51.75  20.9G 14OG392   F51  C~2jhX      
2016 08  28.69002  22 43 28.63   -10 23 47.9   19.6R 14OG392   D29  C~1x8l      
2016 08  28.71830  22 43 28.18   -10 23 50.2   19.7R 14OG392   D29  C~1x8l      
2016 10  06.35940  22 34 43.726  -11 24 55.40  20.2G 14OG392   F51  C~2jhX      
2016 10  06.36069  22 34 43.699  -11 24 55.17  20.7G 14OG392   F51  C~2jhX      
2016 10  06.37126  22 34 43.592  -11 24 55.79  20.5G 14OG392   F51  C~2jhX      
2016 10  06.37255  22 34 43.576  -11 24 55.82  21.1G 14OG392   F51  C~2jhX      
2016 10  06.38316  22 34 43.451  -11 24 56.61  20.8G 14OG392   F51  C~2jhX      
2016 10  06.38446  22 34 43.444  -11 24 56.86  21.9G 14OG392   F51  C~2jhX      
2016 10  06.39509  22 34 43.312  -11 24 57.45  20.6G 14OG392   F51  C~2jhX      
2016 10  06.39639  22 34 43.313  -11 24 57.55  22.3G 14OG392   F51  C~2jhX      
2016 10  25.26533  22 32 16.027  -11 41 40.18  20.5G 14OG392   F51  C~2jhX      
2016 10  25.27648  22 32 15.966  -11 41 40.38  20.4G 14OG392   F51  C~2jhX      
2016 10  25.28767  22 32 15.904  -11 41 40.73  20.9G 14OG392   F51  C~2jhX      
2016 11  15.21061  22 31 48.118  -11 45 53.06  19.2G 14OG392   F51  C~2jhX      
2016 11  15.22422  22 31 48.133  -11 45 52.58  19.2G 14OG392   F51  C~2jhX      
2016 11  15.23783  22 31 48.160  -11 45 52.61  19.3G 14OG392   F51  C~2jhX      
2016 11  15.25140  22 31 48.191  -11 45 52.48  19.2G 14OG392   F51  C~2jhX      
2017 07  08.59061  23 37 17.096  -06 14 34.99  21.0G 14OG392   F51  C~2jhX      
2017 07  22.57659  23 36 34.308  -06 27 56.49  20.5G 14OG392   F51  C~2jhX      
2017 07  30.49397  23 35 42.772  -06 38 13.86  20.4G 14OG392   F51  C~2jhX      
2017 07  30.50601  23 35 42.665  -06 38 15.04  21.0G 14OG392   F51  C~2jhX      
2017 07  30.51796  23 35 42.568  -06 38 16.03  20.7G 14OG392   F51  C~2jhX      
2017 07  30.52986  23 35 42.472  -06 38 16.88  20.9G 14OG392   F51  C~2jhX      
2017 08  03.53094  23 35 09.450  -06 44 08.66  21.1G 14OG392   F51  C~2jhX      
2017 08  03.54171  23 35 09.355  -06 44 09.70  21.0G 14OG392   F51  C~2jhX      
2017 08  03.55248  23 35 09.259  -06 44 10.81  20.7G 14OG392   F51  C~2jhX      
2017 08  03.56324  23 35 09.150  -06 44 11.71  20.5G 14OG392   F51  C~2jhX      
2017 08  17.47679  23 32 42.541  -07 07 23.24  21.1G 14OG392   F51  C~2jhX      
2017 08  17.48785  23 32 42.404  -07 07 24.38  21.0G 14OG392   F51  C~2jhX      
2017 08  17.49891  23 32 42.264  -07 07 25.54  21.2G 14OG392   F51  C~2jhX      
2017 08  17.50997  23 32 42.124  -07 07 26.83  21.0G 14OG392   F51  C~2jhX      
2017 09  15.40527  23 25 55.626  -08 02 13.82  21.1w 14OG392   F51  C~2KWy      
2017 09  15.41638  23 25 55.460  -08 02 14.99  21.1w 14OG392   F51  C~2KWy      
2017 09  15.42757  23 25 55.285  -08 02 16.21  21.2w 14OG392   F51  C~2KWy      
2017 09  15.43867  23 25 55.130  -08 02 17.54  21.6w 14OG392   F51  C~2KWy      
2017 09  22.37594  23 24 11.826  -08 15 00.44  20.8G 14OG392   F51  C~2jhX      
2017 09  22.38697  23 24 11.666  -08 15 01.65  20.6G 14OG392   F51  C~2jhX      
2017 09  22.39801  23 24 11.495  -08 15 02.87  20.5G 14OG392   F51  C~2jhX      
2017 09  22.40904  23 24 11.330  -08 15 03.89  20.6G 14OG392   F51  C~2jhX      
2017 09  23.39024  23 23 56.931  -08 16 48.39  20.8G 14OG392   F51  C~2jhX      
2017 10  11.36275  23 19 53.59   -08 45 04.3   17.9o 14OG392   T08  C~2Ma9      
2017 10  11.36997  23 19 53.52   -08 45 05.4   17.9o 14OG392   T08  C~2Ma9      
2017 10  11.37700  23 19 53.43   -08 45 05.8   17.9o 14OG392   T08  C~2Ma9      
2017 10  11.38426  23 19 53.32   -08 45 06.2   17.9o 14OG392   T08  C~2Ma9      
2017 11  07.30265  23 16 03.281  -09 08 55.22  19.5G 14OG392   F51  C~2jhX      
2017 11  07.31513  23 16 03.194  -09 08 54.78  21.1G 14OG392   F51  C~2jhX      
2017 11  07.32632  23 16 03.139  -09 08 55.03  20.8G 14OG392   F51  C~2jhX      
2017 11  07.33749  23 16 03.092  -09 08 55.39  20.3G 14OG392   F51  C~2jhX      
2017 11  13.27453  23 15 42.571  -09 10 30.35  20.7G 14OG392   F51  C~2jhX      
2017 11  13.28647  23 15 42.520  -09 10 30.67  20.6G 14OG392   F51  C~2jhX      
2017 11  13.29848  23 15 42.497  -09 10 30.43  20.5G 14OG392   F51  C~2jhX      
2017 11  13.31051  23 15 42.468  -09 10 30.75  20.5G 14OG392   F51  C~2jhX      
2018 01  05.21582  23 21 46.315  -08 25 30.14  19.8G 14OG392   F51  C~2jhX      
2018 01  05.22034  23 21 46.367  -08 25 30.40  22.3G 14OG392   F51  C~2jhX      
2018 01  05.22487  23 21 46.436  -08 25 30.07  22.5G 14OG392   F51  C~2jhX      
2018 01  05.22937  23 21 46.505  -08 25 29.46  20.8G 14OG392   F51  C~2jhX      
2018 09  11.69311  00 15 32.46   -04 32 24.8   19.9R 14OG392   D29  C~2kQQ      
2018 09  11.71281  00 15 32.13   -04 32 27.7   19.9R 14OG392   D29  C~2kQQ      
2018 09  11.73251  00 15 31.83   -04 32 28.0   19.9R 14OG392   D29  C~2kQQ      

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    -0.03       0.00     0.03
  2   0.0000      0.00     0.03       0.00    -0.14
  3   1.0238      0.00    -0.02       0.00     0.00
  4   1.2808      0.00     0.03       0.00     0.03
  5   1.9332      0.00     0.05       0.00     0.05
  6   1.9442      0.00     0.16       0.00    -0.22
  7   1.9606      0.00    -0.10       0.00     0.06
  8   1.9606      0.00     0.16       0.00     0.41
  9   1.9606      0.00     0.12       0.00     0.03
 10   1.9606      0.00    -0.01       0.00     0.10
 11   1.9606      0.00     0.05       0.00     0.08
 12   1.9606      0.00     0.09       0.00    -0.01
 13   1.9607      0.00     0.02       0.00    -0.01
 14   1.9607      0.00     0.06       0.00     0.07
 15   2.0207      0.00     0.17       0.00    -0.21
 16   2.0753      0.00    -0.00       0.00     0.01
 17   2.8588      0.00     0.17       0.00    -0.13
 18   2.9026      0.00    -0.26       0.00     0.07
 19   2.9026      0.00    -0.05       0.00     0.01
 20   2.9027      0.00    -0.06       0.00    -0.25
 21   2.9027      0.00    -0.12       0.00     0.15
 22   2.9243      0.00    -0.05       0.00     0.06
 23   2.9243      0.00     0.12       0.00    -0.04
 24   2.9244      0.00    -0.01       0.00     0.01
 25   2.9463      0.00    -0.14       0.00     0.08
 26   2.9464      0.00     0.10       0.00    -0.11
 27   2.9464      0.00    -0.20       0.00    -0.01
 28   2.9517      0.00     0.33       0.00     0.02
 29   3.0037      0.00    -0.08       0.00     0.15
 30   3.0037      0.00     0.03       0.00    -0.10
 31   3.0038      0.00    -0.06       0.00     0.14
 32   3.0059      0.00     0.10       0.00    -0.50
 33   3.0060      0.00    -0.19       0.00     0.37
 34   3.0060      0.00     0.40       0.00     0.83
 35   3.0828      0.00    -0.02       0.00    -0.43
 36   3.0828      0.00    -0.05       0.00     0.01
 37   3.0829      0.00    -0.09       0.00     0.01
 38   3.0829      0.00     0.10       0.00    -0.23
 39   3.0855      0.00    -0.12       0.00     0.14
 40   3.0856      0.00    -0.09       0.00    -0.09
 41   3.0856      0.00     0.09       0.00    -0.44
 42   3.0857      0.00     0.11       0.00    -0.04
 43   3.1292      0.00    -0.04       0.00     0.10
 44   3.1292      0.00    -0.02       0.00    -0.07
 45   3.1293      0.00    -0.04       0.00    -0.20
 46   3.1293      0.00    -0.10       0.00    -0.04
 47   3.1812      0.00    -0.03       0.00     0.04
 48   3.9128      0.00     0.01       0.00     0.06
 49   3.9129      0.00     0.05       0.00     0.19
 50   3.9129      0.00     0.03       0.00     0.15
 51   3.9129      0.00    -0.02       0.00     0.08
 52   3.9592      0.00    -0.18       0.00     0.10
 53   3.9593      0.00    -0.12       0.00     0.11
 54   3.9593      0.00    -0.09       0.00     0.10
 55   3.9593      0.00    -0.20       0.00     0.07
 56   3.9648      0.00    -0.27       0.00     0.23
 57   3.9649      0.00    -0.24       0.00    -0.14
 58   3.9649      0.00    -0.07       0.00     0.04
 59   3.9649      0.00     0.06       0.00    -0.04
 60   4.1095      0.00    -0.02       0.00     0.07
 61   4.1095      0.00     0.02       0.00    -0.12
 62   4.1095      0.00    -0.06       0.00    -0.13
 63   4.1095      0.00     0.14       0.00     0.02
 64   4.1122      0.00    -0.09       0.00     0.03
 65   4.1123      0.00    -0.08       0.00     0.02
 66   4.1123      0.00    -0.09       0.00    -0.00
 67   4.1123      0.00    -0.07       0.00     0.07
 68   4.2023      0.00    -0.10       0.00     0.01
 69   4.2023      0.00    -0.12       0.00    -0.03
 70   4.2024      0.00    -0.18       0.00     0.11
 71   4.2024      0.00    -0.16       0.00    -0.04
 72   4.2051      0.00    -0.04       0.00     0.08
 73   4.2052      0.00    -0.16       0.00     0.03
 74   4.2815      0.00     0.74       0.00     0.24
 75   4.9477      0.00    -0.00       0.00     0.04
 76   4.9477      0.00    -0.04       0.00    -0.04
 77   4.9478      0.00     0.03       0.00    -0.02
 78   4.9478      0.00    -0.02       0.00     0.07
 79   5.0215      0.00     0.06       0.00    -0.03
 80   5.0216      0.00     0.03       0.00     0.07
 81   5.0216      0.00    -0.00       0.00    -0.18
 82   5.0216      0.00     0.02       0.00    -0.06
 83   5.0905      0.00     0.91       0.00    -0.80
 84   5.0906      0.00     0.61       0.00    -0.03
 85   5.1964      0.00     0.16       0.00    -0.42
 86   5.1964      0.00    -0.03       0.00    -0.10
 87   5.1964      0.00     0.07       0.00     0.02
 88   5.1964      0.00     0.04       0.00     0.08
 89   5.1964      0.00    -0.12       0.00     0.04
 90   5.1964      0.00    -0.01       0.00    -0.12
 91   5.1965      0.00    -0.28       0.00     0.04
 92   5.1965      0.00    -0.05       0.00     0.03
 93   5.2481      0.00     0.07       0.00    -0.17
 94   5.2481      0.00     0.04       0.00     0.01
 95   5.2482      0.00    -0.00       0.00     0.05
 96   5.3055      0.00     0.16       0.00    -0.15
 97   5.3055      0.00    -0.03       0.00     0.19
 98   5.3055      0.00    -0.04       0.00     0.01
 99   5.3056      0.00     0.01       0.00    -0.00
100   5.9499      0.00     0.17       0.00    -0.02
101   5.9882      0.00     0.15       0.00    -0.13
102   6.0099      0.00     0.25       0.00     0.13
103   6.0099      0.00     0.09       0.00    -0.03
104   6.0099      0.00     0.07       0.00    -0.01
105   6.0100      0.00     0.07       0.00     0.15
106   6.0209      0.00     0.00       0.00     0.13
107   6.0209      0.00     0.06       0.00     0.07
108   6.0210      0.00     0.10       0.00    -0.06
109   6.0210      0.00    -0.06       0.00     0.02
110   6.0591      0.00     0.03       0.00     0.05
111   6.0591      0.00     0.04       0.00     0.11
112   6.0592      0.00     0.01       0.00     0.14
113   6.0592      0.00    -0.02       0.00     0.04
114   6.1383      0.00    -0.00       0.00     0.12
115   6.1383      0.00     0.07       0.00     0.20
116   6.1384      0.00     0.02       0.00     0.24
117   6.1384      0.00     0.25       0.00     0.16
118   6.1574      0.00    -0.08       0.00    -0.01
119   6.1574      0.00     0.02       0.00    -0.04
120   6.1574      0.00    -0.05       0.00    -0.08
121   6.1575      0.00    -0.03       0.00     0.08
122   6.1602      0.00    -0.02       0.00     0.07
123   6.2094      0.00    -0.32       0.00     0.14
124   6.2094      0.00    -0.03       0.00    -0.38
125   6.2094      0.00    -0.07       0.00    -0.22
126   6.2094      0.00    -0.37       0.00    -0.03
127   6.2831      0.00     0.35       0.00    -0.68
128   6.2832      0.00    -0.05       0.00     0.05
129   6.2832      0.00    -0.07       0.00     0.05
130   6.2832      0.00     0.03       0.00    -0.05
131   6.2995      0.00     0.15       0.00    -0.07
132   6.2995      0.00    -0.12       0.00    -0.28
133   6.2995      0.00     0.03       0.00     0.06
134   6.2996      0.00     0.10       0.00    -0.15
135   6.4444      0.00     0.20       0.00     0.78
136   6.4444      0.00    -0.06       0.00     0.05
137   6.4444      0.00    -0.06       0.00    -0.10
138   6.4445      0.00    -0.05       0.00     0.04
139   7.1275      0.00     0.25       0.00    -0.24
140   7.1275      0.00    -0.38       0.00    -0.80
141   7.1276      0.00    -0.56       0.00     1.25

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.

14OG392    quality flag:3

Type:       CENTAURR  CENTAURR  CENTAURR

axisobj        12.134    12.134    12.134
ecceobj         0.185     0.185     0.185
incobj          9.042     9.042     9.042
qmin            9.739     9.740     9.661
qmax           16.277    21.240    33.713
amean          12.303    14.036    16.703
amin           11.373    12.134    12.134
amax           13.050    15.619    21.868
emean           0.201     0.292     0.397
emin            0.144     0.185     0.185
emax            0.247     0.360     0.543
imean           7.490     8.384     7.595
imin            7.261     7.252     5.673
imax            7.864     9.286     8.817
excite_mean     0.240     0.327     0.421
fracstop        0.000     0.002     0.002
cjmean          3.696     3.440     3.186

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       290.1     159.8     162.3
kozaiamp         34.1     169.2     168.0