Orbit Fit and Astrometric record for 14WC509

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: 14WC509   
# Created Sun Dec 22 02:10:11 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     66 observations of     66
# Arc:  14.99y
# First observation: 2009/12/08
#  Last observation: 2024/12/05
# Chi-squared of fit:    24.18 DOF:    126 RMS:  0.11
# Min/Max residuals:    -0.47    0.25
# Exact a, adot, b, bdot, g, gdot:
  1.992041E-05  4.242370E-02 -2.557316E-06 -5.384765E-03  3.401585E-02  5.085574E-03
# Covariance matrix:
  2.6096E-13 -6.2191E-14 -1.7674E-14  6.0229E-15 -5.0801E-14 -7.5817E-14
 -6.2191E-14  1.9275E-14  6.3528E-15 -2.1516E-15  2.3004E-14  2.7068E-14
 -1.7674E-14  6.3528E-15  1.2740E-13 -1.4613E-14  8.0882E-15  9.8867E-15
  6.0229E-15 -2.1516E-15 -1.4613E-14  2.1225E-15 -2.4374E-15 -3.3639E-15
 -5.0801E-14  2.3004E-14  8.0882E-15 -2.4374E-15  1.3740E-13  3.0277E-14
 -7.5817E-14  2.7068E-14  9.8867E-15 -3.3639E-15  3.0277E-14  4.2339E-14
#      lat0       lon0       xBary       yBary       zBary        JD0
    6.075773   85.439951    0.152297    0.103256   -0.969890  2455173.926813
# Heliocentric elements and errors
Epoch:              2455174.5000  =  2009/12/09
Mean Anomaly:           19.40434 +/-     0.003
Argument of Peri:      107.34591 +/-     0.004
Long of Asc Node:      304.21932 +/-     0.000
Inclination:             9.28131 +/-     0.000
Eccentricity:         0.25719504 +/-    0.0000
Semi-Major Axis:     39.51395936 +/-    0.0023
Time of Perihelion: 2450284.3675 +/-       0.8
Perihelion:          29.35116493 +/-    0.0021
Aphelion:            49.67675380 +/-    0.0032
Period (y)              248.3900 +/-      0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X            2.55658329 +/-    0.0000
Ecliptic Y           30.09756278 +/-    0.0003
Ecliptic Z            3.11149995 +/-    0.0000
Ecliptic XDOT        -0.00336455 +/-    0.0000
Ecliptic YDOT         0.00072834 +/-    0.0000
Ecliptic ZDOT        -0.00038772 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   30.36571653 +/-    0.0003
Geocenter to KBO     29.39802818 +/-    0.0003
# Hcoef:  7.05

The following table shows the complete astrometric record for 14WC509. 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 (14WC509) followed by the observatory code and reference code for the source of the astrometry.

2009 12  08.426047 05 39 10.061  +29 25 57.58  21.6G 14WC509   F51  C~400W      
2009 12  08.434789 05 39 09.987  +29 25 57.47  21.8G 14WC509   F51  C~400W      
2011 11  25.555390 06 02 45.978  +28 52 44.72  21.7G 14WC509   F51  C~400W      
2011 11  25.570591 06 02 45.876  +28 52 44.35  21.5G 14WC509   F51  C~400W      
2011 11  25.585914 06 02 45.783  +28 52 44.68  21.8G 14WC509   F51  C~400W      
2011 11  25.600543 06 02 45.695  +28 52 44.69  22.0G 14WC509   F51  C~400W      
2011 11  30.559242 06 02 13.088  +28 52 54.61  21.6G 14WC509   F51  C~400W      
2011 11  30.572314 06 02 13.007  +28 52 54.64  22.0G 14WC509   F51  C~400W      
2011 12  04.573215 06 01 45.520  +28 52 58.53  21.6G 14WC509   F51  C~400W      
2011 12  04.584304 06 01 45.462  +28 52 58.77  21.8G 14WC509   F51  C~400W      
2014 11  17.41935  06 35 01.827  +27 39 15.25  22.1w 14WC509   F51  C~1vXq      
2014 11  17.43252  06 35 01.749  +27 39 15.35  22.1w 14WC509   F51  C~1vXq      
2014 11  17.44561  06 35 01.692  +27 39 15.74  22.1w 14WC509   F51  C~1vXq      
2015 01  14.42414  06 28 36.220  +27 42 40.02  22.0w 14WC509   F51  C~1vXq      
2015 01  14.43707  06 28 36.135  +27 42 39.96  22.0w 14WC509   F51  C~1vXq      
2015 01  14.44996  06 28 36.043  +27 42 39.98  22.0w 14WC509   F51  C~1vXq      
2015 01  14.46281  06 28 35.951  +27 42 39.91  21.9w 14WC509   F51  C~1vXq      
2015 01  16.43271  06 28 22.512  +27 42 36.64  22.1w 14WC509   F51  C~1vXq      
2015 01  16.44434  06 28 22.426  +27 42 36.59  22.0w 14WC509   F51  C~1vXq      
2015 01  16.45600  06 28 22.341  +27 42 36.50  21.9w 14WC509   F51  C~1vXq      
2015 01  16.46754  06 28 22.269  +27 42 36.53  22.2w 14WC509   F51  C~1vXq      
2015 01  23.28299  06 27 37.528  +27 42 19.25  21.9w 14WC509   F51  C~1vXq      
2015 01  23.29699  06 27 37.438  +27 42 19.21  21.9w 14WC509   F51  C~1vXq      
2015 01  23.31095  06 27 37.342  +27 42 19.14  21.9w 14WC509   F51  C~1vXq      
2016 11  10.524911 06 55 18.852  +26 37 31.91  21.8G 14WC509   F51  C~400W      
2016 11  10.536542 06 55 18.809  +26 37 32.01  22.1G 14WC509   F51  C~400W      
2016 11  10.548196 06 55 18.771  +26 37 32.08  22.3G 14WC509   F51  C~400W      
2016 11  10.559900 06 55 18.726  +26 37 32.10  22.1G 14WC509   F51  C~400W      
2017 10  29.538837 07 05 21.393  +26 02 40.81  22.4G 14WC509   F51  C~400W      
2017 10  29.550505 07 05 21.381  +26 02 40.91  22.3G 14WC509   F51  C~400W      
2017 10  29.562190 07 05 21.360  +26 02 40.79  22.4G 14WC509   F51  C~400W      
2017 10  29.573892 07 05 21.340  +26 02 41.02  22.1G 14WC509   F51  C~400W      
2017 12  25.532074 07 00 48.610  +26 10 10.59  21.7G 14WC509   F51  C~400W      
2017 12  25.544176 07 00 48.528  +26 10 10.76  21.8G 14WC509   F51  C~400W      
2017 12  25.556315 07 00 48.456  +26 10 10.73  21.5G 14WC509   F51  C~400W      
2017 12  25.568406 07 00 48.326  +26 10 11.02  21.9G 14WC509   F51  C~400W      
2018 12  17.579050 07 11 12.422  +25 34 02.20  22.0G 14WC509   F51  C~400W      
2018 12  17.591345 07 11 12.355  +25 34 02.36  22.2G 14WC509   F51  C~400W      
2018 12  17.603691 07 11 12.266  +25 34 02.40  22.2G 14WC509   F51  C~400W      
2019 01  02.523824 07 09 24.796  +25 36 26.68  21.6G 14WC509   F51  C~400W      
2019 01  02.534873 07 09 24.705  +25 36 26.80  22.1G 14WC509   F51  C~400W      
2019 01  02.545917 07 09 24.623  +25 36 26.98  22.2G 14WC509   F51  C~400W      
2019 01  02.556900 07 09 24.558  +25 36 26.93  22.1G 14WC509   F51  C~400W      
2019 01  09.355731 07 08 37.040  +25 37 21.16  22.0G 14WC509   F51  C~400W      
2019 01  09.367605 07 08 36.945  +25 37 21.35  22.0G 14WC509   F51  C~400W      
2019 01  09.379563 07 08 36.862  +25 37 21.37  22.1G 14WC509   F51  C~400W      
2019 01  09.391528 07 08 36.780  +25 37 21.38  22.0G 14WC509   F51  C~400W      
2019 01  25.469797 07 06 47.420  +25 39 00.85  22.4G 14WC509   F51  C~400W      
2019 01  25.483448 07 06 47.335  +25 39 00.80  21.8G 14WC509   F51  C~400W      
2019 01  25.497017 07 06 47.238  +25 39 00.65  22.0G 14WC509   F51  C~400W      
2019 01  25.510670 07 06 47.155  +25 39 00.97  21.8G 14WC509   F51  C~400W      
2019 02  04.252050 07 05 46.763  +25 39 36.71  22.2G 14WC509   F51  C~400W      
2019 02  04.265076 07 05 46.665  +25 39 37.01  22.2G 14WC509   F51  C~400W      
2019 12  08.578563 07 21 21.417  +24 55 40.94  22.5G 14WC509   F52  C~400W      
2019 12  08.590542 07 21 21.342  +24 55 41.19  21.9G 14WC509   F52  C~400W      
2019 12  08.602433 07 21 21.280  +24 55 41.11  21.6G 14WC509   F52  C~400W      
2020 01  20.462152 07 16 40.028  +25 02 38.48  21.8G 14WC509   F51  C~400W      
2020 01  20.475604 07 16 39.941  +25 02 38.34  21.7G 14WC509   F51  C~400W      
2020 01  20.489070 07 16 39.838  +25 02 38.44  21.7G 14WC509   F51  C~400W      
2020 01  20.502613 07 16 39.758  +25 02 38.60  22.1G 14WC509   F51  C~400W      
2022 01  07.343110 07 36 01.423  +23 43 39.80  21.7w 14WC509   F52  C~5Lip      
2022 01  07.355149 07 36 01.332  +23 43 40.28  21.8w 14WC509   F52  C~5Lip      
2022 01  07.367201 07 36 01.250  +23 43 40.18  21.9w 14WC509   F52  C~5Lip      
2024 12  05.440017 08 04 17.514  +21 31 22.77  22.1w 14WC509   F52  C~8ST9      
2024 12  05.452709 08 04 17.460  +21 31 22.84  21.9w 14WC509   F52  C~8ST9      
2024 12  05.478203 08 04 17.349  +21 31 23.03  22.0w 14WC509   F52  C~8ST9      

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    -0.05       0.00     0.01
     2   0.0000      0.00    -0.17       0.00    -0.06
     3   1.9634      0.00    -0.04       0.00     0.15
     4   1.9634      0.00    -0.08       0.00    -0.26
     5   1.9635      0.00     0.02       0.00     0.04
     6   1.9635      0.00     0.13       0.00     0.02
     7   1.9771      0.00    -0.06       0.00     0.11
     8   1.9771      0.00     0.07       0.00     0.12
     9   1.9881      0.00    -0.16       0.00    -0.27
    10   1.9881      0.00     0.15       0.00    -0.03
    11   4.9418      0.00     0.17       0.00    -0.05
    12   4.9418      0.00    -0.02       0.00    -0.05
    13   4.9419      0.00     0.09       0.00     0.25
    14   5.1006      0.00    -0.09       0.00     0.05
    15   5.1006      0.00    -0.00       0.00     0.01
    16   5.1007      0.00    -0.03       0.00     0.05
    17   5.1007      0.00    -0.06       0.00     0.00
    18   5.1061      0.00     0.09       0.00    -0.04
    19   5.1061      0.00     0.01       0.00    -0.07
    20   5.1062      0.00    -0.06       0.00    -0.13
    21   5.1062      0.00     0.05       0.00    -0.08
    22   5.1249      0.00     0.18       0.00     0.06
    23   5.1249      0.00     0.19       0.00     0.06
    24   5.1249      0.00     0.10       0.00     0.03
    25   6.9243      0.00    -0.08       0.00     0.10
    26   6.9243      0.00    -0.09       0.00     0.11
    27   6.9244      0.00    -0.02       0.00     0.09
    28   6.9244      0.00    -0.06       0.00     0.02
    29   7.8908      0.00    -0.04       0.00    -0.05
    30   7.8908      0.00     0.08       0.00    -0.02
    31   7.8909      0.00     0.06       0.00    -0.21
    32   7.8909      0.00     0.06       0.00    -0.04
    33   8.0468      0.00    -0.05       0.00    -0.01
    34   8.0469      0.00    -0.00       0.00     0.07
    35   8.0469      0.00     0.20       0.00    -0.05
    36   8.0469      0.00    -0.47       0.00     0.15
    37   9.0244      0.00    -0.20       0.00    -0.02
    38   9.0244      0.00    -0.00       0.00     0.03
    39   9.0244      0.00    -0.13       0.00    -0.04
    40   9.0680      0.00     0.20       0.00    -0.08
    41   9.0681      0.00     0.00       0.00    -0.05
    42   9.0681      0.00    -0.05       0.00     0.04
    43   9.0681      0.00     0.14       0.00    -0.09
    44   9.0867      0.00     0.11       0.00    -0.00
    45   9.0868      0.00    -0.06       0.00     0.09
    46   9.0868      0.00    -0.03       0.00     0.02
    47   9.0868      0.00     0.02       0.00    -0.06
    48   9.1309      0.00    -0.01       0.00     0.11
    49   9.1309      0.00     0.06       0.00    -0.00
    50   9.1309      0.00    -0.05       0.00    -0.21
    51   9.1310      0.00     0.05       0.00     0.05
    52   9.1576      0.00     0.18       0.00    -0.07
    53   9.1577      0.00    -0.12       0.00     0.19
    54   9.9990      0.00     0.06       0.00    -0.03
    55   9.9991      0.00    -0.05       0.00     0.10
    56   9.9991      0.00     0.03       0.00    -0.10
    57  10.1165      0.00    -0.09       0.00     0.18
    58  10.1165      0.00    -0.01       0.00    -0.06
    59  10.1165      0.00    -0.18       0.00    -0.06
    60  10.1166      0.00     0.01       0.00     0.00
    61  12.0819      0.00     0.18       0.00    -0.13
    62  12.0819      0.00     0.04       0.00     0.20
    63  12.0820      0.00     0.04       0.00    -0.05
    64  14.9925      0.00     0.02       0.00     0.04
    65  14.9925      0.00     0.02       0.00    -0.02
    66  14.9926      0.00    -0.03       0.00    -0.11

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.

14WC509    quality flag:3

Type:           3:2E      3:2E      3:2E

axisobj        39.938    39.938    39.938
ecceobj         0.264     0.264     0.264
incobj          9.265     9.265     9.265
qmin           28.501    28.499    28.502
qmax           51.027    51.019    51.035
amean          39.455    39.455    39.455
amin           38.987    38.986    38.988
amax           39.977    39.975    39.978
emean           0.241     0.241     0.241
emin            0.206     0.206     0.206
emax            0.277     0.277     0.277
imean          11.156    11.157    11.156
imin            9.201     9.202     9.201
imax           13.045    13.045    13.044
excite_mean     0.310     0.310     0.310
fracstop        1.000     1.000     1.000
cjmean          2.941     2.941     2.941

libcent 0       180.2     179.8     180.1
libamp  0        84.7      84.9      84.9
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        87.7      87.7      87.7
kozaiamp         42.5      42.5      42.5