Orbit Fit and Astrometric record for 14OC394

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: 14OC394   
# Created Thu Apr 25 01:15:56 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     79 observations of     79
# Arc:  12.05y
# First observation: 2009/10/15
#  Last observation: 2021/11/01
# Chi-squared of fit:    74.07 DOF:    152 RMS:  0.17
# Min/Max residuals:    -0.84    0.65
# Exact a, adot, b, bdot, g, gdot:
  1.548563E-05  2.398200E-02 -5.477296E-07 -3.341167E-04  2.430181E-02 -1.209153E-03
# Covariance matrix:
  2.2505E-13 -6.0599E-14 -1.5742E-15  6.4552E-16 -3.8853E-14 -1.5681E-13
 -6.0599E-14  2.6090E-14  6.8644E-16 -3.2474E-16 -4.4788E-15  8.1037E-14
 -1.5742E-15  6.8644E-16  1.0785E-13 -1.4531E-14  2.8468E-16  2.3387E-15
  6.4552E-16 -3.2474E-16 -1.4531E-14  2.3467E-15  3.4881E-17 -1.1079E-15
 -3.8853E-14 -4.4788E-15  2.8468E-16  3.4881E-17  8.2106E-14 -1.6015E-14
 -1.5681E-13  8.1037E-14  2.3387E-15 -1.1079E-15 -1.6015E-14  2.7654E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
   -2.376856  -14.402863   -0.591304   -0.033217   -0.799852  2455119.660278
# Heliocentric elements and errors
Epoch:              2455120.5000  =  2009/10/16
Mean Anomaly:          322.13169 +/-     0.033
Argument of Peri:      293.90507 +/-     0.038
Long of Asc Node:       94.48075 +/-     0.003
Inclination:             2.45195 +/-     0.000
Eccentricity:         0.05511749 +/-    0.0000
Semi-Major Axis:     43.80996396 +/-    0.0023
Time of Perihelion: 2466261.6798 +/-      12.3
Perihelion:          41.39526873 +/-    0.0025
Aphelion:            46.22465919 +/-    0.0027
Period (y)              289.9797 +/-      0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           40.74771996 +/-    0.0005
Ecliptic Y           -9.85570276 +/-    0.0001
Ecliptic Z           -1.70654690 +/-    0.0000
Ecliptic XDOT         0.00054235 +/-    0.0000
Ecliptic YDOT         0.00265627 +/-    0.0000
Ecliptic ZDOT        -0.00003204 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.95742805 +/-    0.0005
Geocenter to KBO     41.14926227 +/-    0.0005
# Hcoef:  6.58

The following table shows the complete astrometric record for 14OC394. 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 (14OC394) followed by the observatory code and reference code for the source of the astrometry.

2009 10  15.159512 23 10 40.96   -07 52 08.1   22.2V 14OC394   645  C~2sc4      
2009 10  15.160341 23 10 40.96   -07 52 08.2         14OC394   645  C~2sc4      
2009 10  15.162829 23 10 40.95   -07 52 08.4         14OC394   645  C~2sc4      
2010 08  31.48463  23 19 00.393  -07 01 21.70  23.0G 14OC394   F51  C~2r7V      
2010 09  15.44714  23 17 53.795  -07 08 27.87  22.2G 14OC394   F51  C~2r7V      
2010 09  15.45710  23 17 53.740  -07 08 28.40  23.1G 14OC394   F51  C~2r7V      
2010 09  15.47714  23 17 53.669  -07 08 28.87  22.8G 14OC394   F51  C~2r7V      
2011 09  21.36580  23 22 38.785  -06 39 22.64  22.8G 14OC394   F51  C~2r7V      
2011 09  21.37987  23 22 38.725  -06 39 22.79  22.5G 14OC394   F51  C~2r7V      
2011 09  21.39390  23 22 38.662  -06 39 23.32  22.4G 14OC394   F51  C~2r7V      
2011 09  21.40796  23 22 38.601  -06 39 24.05  21.8G 14OC394   F51  C~2r7V      
2013 09  01.43242  23 34 23.869  -05 25 59.38  22.4w 14OC394   F51  C~2r7V      
2013 09  01.44590  23 34 23.795  -05 25 59.61  22.4w 14OC394   F51  C~2r7V      
2013 09  01.45935  23 34 23.746  -05 26 00.17  22.4w 14OC394   F51  C~2r7V      
2013 09  01.47278  23 34 23.682  -05 26 00.45  22.5w 14OC394   F51  C~2r7V      
2014 07  28.54921  23 41 37.041  -04 38 58.89  22.7w 14OC394   F51  C~1vXf      
2014 07  28.56061  23 41 37.012  -04 38 59.18  22.5w 14OC394   F51  C~1vXf      
2014 07  28.57199  23 41 36.992  -04 38 59.00  22.7w 14OC394   F51  C~1vXf      
2014 08  03.52799  23 41 20.544  -04 41 02.89  22.7w 14OC394   F51  C~1vXf      
2014 08  03.53933  23 41 20.514  -04 41 03.01  22.7w 14OC394   F51  C~1vXf      
2014 08  03.56194  23 41 20.448  -04 41 03.56  23.0w 14OC394   F51  C~1vXf      
2014 08  20.48054  23 40 22.317  -04 47 58.87  22.8w 14OC394   F51  C~1vXf      
2014 08  20.49272  23 40 22.269  -04 47 59.11  22.6w 14OC394   F51  C~1vXf      
2014 08  20.50488  23 40 22.221  -04 47 59.48  22.5w 14OC394   F51  C~1vXf      
2014 08  20.51707  23 40 22.165  -04 47 59.80  22.5w 14OC394   F51  C~1vXf      
2014 09  19.33273  23 38 14.532  -05 02 09.92  22.5w 14OC394   F51  C~1vXf      
2014 09  19.35561  23 38 14.433  -05 02 10.49  22.4w 14OC394   F51  C~1vXf      
2014 09  19.36706  23 38 14.378  -05 02 10.97  22.6w 14OC394   F51  C~1vXf      
2015 09  09.41690  23 44 08.392  -04 24 44.23  22.0G 14OC394   F51  C~2r7V      
2015 09  09.42905  23 44 08.326  -04 24 44.71  22.6G 14OC394   F51  C~2r7V      
2015 09  09.44122  23 44 08.267  -04 24 45.07  22.4G 14OC394   F51  C~2r7V      
2015 09  09.45342  23 44 08.224  -04 24 45.49  22.8G 14OC394   F51  C~2r7V      
2015 09  10.39285  23 44 04.083  -04 25 12.92  23.1G 14OC394   F51  C~2r7V      
2015 09  12.39454  23 43 55.218  -04 26 11.14  22.5G 14OC394   F51  C~2r7V      
2015 09  12.40629  23 43 55.166  -04 26 11.33  22.5G 14OC394   F51  C~2r7V      
2015 09  12.41804  23 43 55.111  -04 26 11.90  22.5G 14OC394   F51  C~2r7V      
2015 09  12.42981  23 43 55.061  -04 26 12.19  22.4G 14OC394   F51  C~2r7V      
2015 11  02.28409  23 40 31.105  -04 47 04.84  22.4G 14OC394   F51  C~2r7V      
2015 11  17.23545  23 39 55.611  -04 50 06.62  23.4G 14OC394   F51  C~2r7V      
2015 12  09.21300  23 39 36.958  -04 50 46.44  22.7G 14OC394   F51  C~2r7V      
2015 12  09.22525  23 39 36.936  -04 50 46.99  22.6G 14OC394   F51  C~2r7V      
2015 12  09.23755  23 39 36.967  -04 50 46.30  22.5G 14OC394   F51  C~2r7V      
2015 12  09.24991  23 39 36.960  -04 50 46.34  23.3G 14OC394   F51  C~2r7V      
2017 07  30.50923  23 56 48.911  -03 02 14.83  22.3G 14OC394   F51  C~2r7V      
2017 07  30.53307  23 56 48.867  -03 02 15.42  22.5G 14OC394   F51  C~2r7V      
2017 08  01.53329  23 56 43.877  -03 02 53.84  22.5G 14OC394   F51  C~2r7V      
2017 08  01.54515  23 56 43.849  -03 02 54.13  22.8G 14OC394   F51  C~2r7V      
2017 08  01.55704  23 56 43.826  -03 02 54.19  23.1G 14OC394   F51  C~2r7V      
2017 08  01.56895  23 56 43.784  -03 02 54.61  22.8G 14OC394   F51  C~2r7V      
2017 08  03.52437  23 56 38.641  -03 03 33.71  23.1G 14OC394   F51  C~2r7V      
2017 08  03.54593  23 56 38.607  -03 03 34.27  23.7G 14OC394   F51  C~2r7V      
2017 08  03.55668  23 56 38.565  -03 03 34.48  22.8G 14OC394   F51  C~2r7V      
2017 08  17.47873  23 55 55.051  -03 08 55.05  23.0G 14OC394   F51  C~2r7V      
2017 08  17.48978  23 55 55.031  -03 08 55.18  22.3G 14OC394   F51  C~2r7V      
2017 08  17.49043  23 55 54.975  -03 08 54.61  22.9G 14OC394   F51  C~2r7V      
2017 08  17.50149  23 55 54.947  -03 08 54.59  23.2G 14OC394   F51  C~2r7V      
2017 08  17.51191  23 55 54.911  -03 08 54.90  23.1G 14OC394   F51  C~2r7V      
2017 08  20.53329  23 55 43.990  -03 10 12.52  23.7G 14OC394   F51  C~2r7V      
2017 09  14.41532  23 54 01.055  -03 21 53.30  22.4G 14OC394   F51  C~2r7V      
2017 09  14.42731  23 54 01.020  -03 21 53.57  22.5G 14OC394   F51  C~2r7V      
2017 09  14.43923  23 54 00.944  -03 21 53.66  22.6G 14OC394   F51  C~2r7V      
2017 09  14.45116  23 54 00.894  -03 21 54.09  22.3G 14OC394   F51  C~2r7V      
2017 09  17.38477  23 53 47.851  -03 23 20.11  22.7G 14OC394   F51  C~2r7V      
2017 09  17.39647  23 53 47.792  -03 23 20.46  22.9G 14OC394   F51  C~2r7V      
2017 09  17.40819  23 53 47.734  -03 23 20.77  23.4G 14OC394   F51  C~2r7V      
2017 09  17.41994  23 53 47.696  -03 23 21.00  23.4G 14OC394   F51  C~2r7V      
2017 09  22.41421  23 53 25.330  -03 25 46.35  22.5G 14OC394   F51  C~2r7V      
2017 09  23.32104  23 53 21.26   -03 26 12.6   22.5R 14OC394   G37  C~2r7V      
2017 09  23.40445  23 53 20.87   -03 26 15.0         14OC394   G37  C~2r7V      
2017 09  25.38210  23 53 12.073  -03 27 11.53  22.7G 14OC394   F51  C~2r7V      
2017 09  25.39270  23 53 12.006  -03 27 12.15  23.0G 14OC394   F51  C~2r7V      
2017 09  25.40332  23 53 11.977  -03 27 12.27  22.5G 14OC394   F51  C~2r7V      
2017 09  25.41391  23 53 11.909  -03 27 12.74  22.9G 14OC394   F51  C~2r7V      
2020 09  16.40949  00 09 19.248  -01 43 26.91  22.6w 14OC394   F51  C~48DM      
2020 09  16.42733  00 09 19.158  -01 43 27.08  22.8w 14OC394   F51  C~48DM      
2020 09  16.46291  00 09 18.996  -01 43 28.41  22.5w 14OC394   F51  C~48DM      
2021 11  01.287333 00 11 17.613  -01 30 00.85  22.6w 14OC394   F51  C~5BTf      
2021 11  01.299294 00 11 17.552  -01 30 01.37  22.7w 14OC394   F51  C~5BTf      
2021 11  01.311148 00 11 17.525  -01 30 01.40  22.3w 14OC394   F51  C~5BTf      

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     0.07
     2   0.0000      0.00     0.04       0.00    -0.01
     3   0.0000      0.00     0.02       0.00    -0.16
     4   0.8770      0.00     0.04       0.00    -0.07
     5   0.9180      0.00    -0.04       0.00     0.16
     6   0.9180      0.00    -0.18       0.00    -0.09
     7   0.9180      0.00     0.12       0.00     0.00
     8   1.9335      0.00    -0.02       0.00    -0.09
     9   1.9335      0.00     0.03       0.00     0.15
    10   1.9336      0.00     0.03       0.00     0.01
    11   1.9336      0.00     0.07       0.00    -0.33
    12   3.8803      0.00     0.11       0.00     0.07
    13   3.8803      0.00    -0.11       0.00     0.23
    14   3.8804      0.00     0.04       0.00     0.06
    15   3.8804      0.00    -0.04       0.00     0.16
    16   4.7841      0.00     0.02       0.00    -0.09
    17   4.7841      0.00     0.04       0.00    -0.16
    18   4.7842      0.00     0.19       0.00     0.25
    19   4.8005      0.00     0.01       0.00     0.04
    20   4.8005      0.00     0.07       0.00     0.17
    21   4.8006      0.00     0.11       0.00     0.11
    22   4.8469      0.00    -0.10       0.00    -0.02
    23   4.8469      0.00    -0.10       0.00     0.07
    24   4.8469      0.00    -0.10       0.00     0.02
    25   4.8470      0.00    -0.22       0.00     0.03
    26   4.9286      0.00    -0.15       0.00    -0.13
    27   4.9287      0.00    -0.08       0.00    -0.05
    28   4.9287      0.00    -0.12       0.00    -0.20
    29   5.9008      0.00     0.08       0.00     0.17
    30   5.9008      0.00    -0.09       0.00     0.04
    31   5.9008      0.00    -0.16       0.00     0.04
    32   5.9009      0.00     0.02       0.00    -0.03
    33   5.9034      0.00    -0.04       0.00    -0.08
    34   5.9089      0.00    -0.01       0.00     0.09
    35   5.9090      0.00     0.01       0.00     0.24
    36   5.9090      0.00    -0.02       0.00     0.01
    37   5.9090      0.00     0.03       0.00     0.07
    38   6.0483      0.00    -0.00       0.00     0.17
    39   6.0892      0.00     0.08       0.00     0.48
    40   6.1494      0.00     0.04       0.00     0.02
    41   6.1494      0.00    -0.30       0.00    -0.59
    42   6.1494      0.00     0.15       0.00     0.05
    43   6.1495      0.00     0.04       0.00    -0.05
    44   7.7901      0.00    -0.08       0.00     0.07
    45   7.7902      0.00     0.15       0.00    -0.07
    46   7.7957      0.00    -0.09       0.00     0.05
    47   7.7957      0.00    -0.04       0.00    -0.00
    48   7.7957      0.00     0.08       0.00     0.17
    49   7.7958      0.00    -0.07       0.00    -0.01
    50   7.8011      0.00    -0.27       0.00     0.16
    51   7.8012      0.00     0.12       0.00     0.04
    52   7.8012      0.00    -0.06       0.00     0.05
    53   7.8393      0.00     0.36       0.00    -0.84
    54   7.8394      0.00     0.65       0.00    -0.69
    55   7.8394      0.00    -0.15       0.00    -0.11
    56   7.8394      0.00     0.03       0.00     0.19
    57   7.8394      0.00     0.05       0.00     0.14
    58   7.8477      0.00    -0.17       0.00    -0.07
    59   7.9158      0.00    -0.10       0.00    -0.18
    60   7.9159      0.00     0.19       0.00    -0.10
    61   7.9159      0.00    -0.14       0.00     0.16
    62   7.9159      0.00    -0.09       0.00     0.08
    63   7.9240      0.00     0.18       0.00    -0.13
    64   7.9240      0.00     0.09       0.00    -0.14
    65   7.9240      0.00     0.02       0.00    -0.11
    66   7.9241      0.00     0.26       0.00     0.01
    67   7.9377      0.00     0.06       0.00     0.00
    68   7.9402      0.00    -0.06       0.00    -0.00
    69   7.9404      0.00    -0.23       0.00     0.00
    70   7.9459      0.00     0.25       0.00     0.27
    71   7.9459      0.00    -0.03       0.00    -0.05
    72   7.9459      0.00     0.26       0.00     0.13
    73   7.9459      0.00    -0.04       0.00    -0.03
    74  10.9220      0.00    -0.03       0.00    -0.17
    75  10.9220      0.00    -0.18       0.00     0.19
    76  10.9221      0.00    -0.20       0.00    -0.10
    77  12.0469      0.00     0.13       0.00     0.23
    78  12.0469      0.00    -0.15       0.00    -0.05
    79  12.0470      0.00     0.07       0.00     0.16

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.

14OC394    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        43.771    43.771    43.771
ecceobj         0.056     0.056     0.057
incobj          2.454     2.454     2.454
qmin           39.940    39.926    39.946
qmax           47.490    47.514    47.501
amean          43.599    43.599    43.600
amin           43.244    43.242    43.259
amax           43.964    43.955    43.956
emean           0.063     0.063     0.063
emin            0.042     0.042     0.042
emax            0.081     0.081     0.081
imean           1.095     1.095     1.095
imin            0.000     0.000     0.000
imax            1.817     1.817     1.816
excite_mean     0.067     0.067     0.067
fracstop        1.000     1.000     1.000
cjmean          3.091     3.091     3.091

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       171.5     171.5     171.5
kozaiamp        180.0     180.0     180.0