Orbit Fit and Astrometric record for 14SS373

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: 14SS373   
# Created Sun Nov 24 02:09:59 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     67 observations of     67
# Arc:  10.02y
# First observation: 2014/09/30
#  Last observation: 2024/10/08
# Chi-squared of fit:    14.11 DOF:    128 RMS:  0.08
# Min/Max residuals:    -0.21    0.30
# Exact a, adot, b, bdot, g, gdot:
  1.671843E-05  2.576367E-02  3.681992E-06  5.639597E-03  2.453612E-02 -5.886113E-03
# Covariance matrix:
  1.1021E-13 -4.5276E-14  6.7197E-16 -6.9797E-15  4.8902E-14 -1.2180E-13
 -4.5276E-14  3.1296E-14 -5.3869E-15  6.1101E-15 -8.7428E-15  1.0073E-13
  6.7197E-16 -5.3869E-15  4.5182E-14 -8.0848E-15 -1.2500E-14 -2.3009E-14
 -6.9797E-15  6.1101E-15 -8.0848E-15  3.4231E-15  6.1560E-16  2.1830E-14
  4.8902E-14 -8.7428E-15 -1.2500E-14  6.1560E-16  8.4004E-14 -4.5239E-15
 -1.2180E-13  1.0073E-13 -2.3009E-14  2.1830E-14 -4.5239E-15  3.5529E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
  -28.133140   11.735131    0.088028   -0.471373   -0.881918  2456930.738618
# Heliocentric elements and errors
Epoch:              2456930.5000  =  2014/09/30
Mean Anomaly:          334.80955 +/-     0.004
Argument of Peri:      344.15044 +/-     0.007
Long of Asc Node:       76.12797 +/-     0.000
Inclination:            29.95361 +/-     0.000
Eccentricity:         0.34795429 +/-    0.0000
Semi-Major Axis:     57.58681095 +/-    0.0045
Time of Perihelion: 2468099.5525 +/-      17.3
Perihelion:          37.54923276 +/-    0.0036
Aphelion:            77.62438913 +/-    0.0064
Period (y)              437.0114 +/-      0.05
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           36.18431649 +/-    0.0004
Ecliptic Y            7.42916261 +/-    0.0001
Ecliptic Z          -19.21736898 +/-    0.0002
Ecliptic XDOT        -0.00086589 +/-    0.0000
Ecliptic YDOT         0.00275266 +/-    0.0000
Ecliptic ZDOT         0.00086475 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.63913293 +/-    0.0004
Geocenter to KBO     40.75644156 +/-    0.0005
# Hcoef:  6.34

The following table shows the complete astrometric record for 14SS373. 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 (14SS373) followed by the observatory code and reference code for the source of the astrometry.

2014 09  30.23784  01 28 44.764  -21 10 41.18  23.7g 14SS373   W84  C~4yUX      
2014 09  30.23784  01 28 44.76   -21 10 41.2   23.7g 14SS373   W84  C~3cnr      
2014 12  17.14421  01 23 26.707  -21 09 14.27  23.7g 14SS373   W84  C~4yUX      
2014 12  23.09313  01 23 17.479  -21 05 36.09  22.8r 14SS373   W84  C~4yUX      
2014 12  23.09313  01 23 17.48   -21 05 36.1   23.2r 14SS373   W84  C~3cnr      
2014 12  23.09451  01 23 17.466  -21 05 36.03  23.9g 14SS373   W84  C~4yUX      
2014 12  23.09451  01 23 17.46   -21 05 36.1   24.3g 14SS373   W84  C~3cnr      
2014 12  23.09586  01 23 17.474  -21 05 35.90  22.1i 14SS373   W84  C~4yUX      
2014 12  23.09586  01 23 17.47   -21 05 35.9   22.5i 14SS373   W84  C~3cnr      
2015 01  12.05566  01 23 11.593  -20 50 34.43  22.2i 14SS373   W84  C~4yUX      
2015 01  12.05566  01 23 11.59   -20 50 34.4   22.3i 14SS373   W84  C~3cnr      
2015 08  17.40599  01 36 27.666  -19 47 28.04  22.8r 14SS373   W84  C~4yUX      
2015 08  24.38299  01 36 12.528  -19 52 17.31  22.3i 14SS373   W84  C~4yUX      
2015 08  24.38435  01 36 12.523  -19 52 17.35  22.6r 14SS373   W84  C~4yUX      
2015 09  04.35407  01 35 40.894  -19 59 48.13  21.9z 14SS373   W84  C~4yUX      
2015 09  04.35407  01 35 40.89   -19 59 48.1   21.9z 14SS373   W84  C~3cnr      
2015 10  07.23199  01 33 22.660  -20 18 46.51  22.2i 14SS373   W84  C~4yUX      
2015 10  07.23338  01 33 22.642  -20 18 46.58  22.6r 14SS373   W84  C~4yUX      
2015 10  07.23338  01 33 22.64   -20 18 46.6   22.6r 14SS373   W84  C~3cnr      
2015 10  18.24488  01 32 28.385  -20 22 54.16  23.1g 14SS373   W84  C~4yUX      
2015 10  18.24625  01 32 28.370  -20 22 54.45  22.3r 14SS373   W84  C~4yUX      
2015 11  06.13290  01 30 56.504  -20 26 18.09  22.3i 14SS373   W84  C~4yUX      
2015 11  06.13290  01 30 56.50   -20 26 18.1   22.2i 14SS373   W84  C~3cnr      
2015 11  06.13428  01 30 56.508  -20 26 18.03  23.1g 14SS373   W84  C~4yUX      
2015 11  07.14852  01 30 51.794  -20 26 20.42  22.5r 14SS373   W84  C~4yUX      
2015 11  07.14852  01 30 51.79   -20 26 20.4   22.5r 14SS373   W84  C~3cnr      
2015 11  08.18350  01 30 47.030  -20 26 21.66  23.8g 14SS373   W84  C~4yUX      
2015 11  14.17776  01 30 20.302  -20 26 10.97  21.3z 14SS373   W84  C~4yUX      
2015 11  14.17776  01 30 20.30   -20 26 11.0   21.5z 14SS373   W84  C~3cnr      
2015 11  14.17912  01 30 20.30   -20 26 11.1   21.8i 14SS373   W84  C~3cnr      
2015 11  14.18051  01 30 20.292  -20 26 10.97  22.5r 14SS373   W84  C~4yUX      
2015 11  14.18051  01 30 20.29   -20 26 11.0   22.4r 14SS373   W84  C~3cnr      
2015 11  14.18190  01 30 20.275  -20 26 10.84  24.3g 14SS373   W84  C~4yUX      
2015 11  18.15278  01 30 03.514  -20 25 45.80  22.0z 14SS373   W84  C~4yUX      
2015 11  18.15278  01 30 03.51   -20 25 45.8   22.1z 14SS373   W84  C~3cnr      
2016 10  05.26710  01 38 38.305  -19 21 58.71  22.2i 14SS373   W84  C~4yUX      
2016 10  05.26710  01 38 38.30   -19 21 58.7   22.2i 14SS373   W84  C~3cnr      
2016 10  05.26847  01 38 38.299  -19 21 58.76  22.5r 14SS373   W84  C~4yUX      
2016 10  05.26847  01 38 38.30   -19 21 58.7   22.7r 14SS373   W84  C~3cnr      
2016 10  05.26985  01 38 38.300  -19 21 58.76  23.5g 14SS373   W84  C~4yUX      
2016 10  05.26985  01 38 38.30   -19 21 58.7   23.5g 14SS373   W84  C~3cnr      
2017 10  03.22722  01 43 58.800  -18 23 24.32  21.6z 14SS373   W84  C~4yUX      
2017 11  10.14149  01 40 53.881  -18 33 41.86  22.6r 14SS373   W84  C~4yUX      
2017 11  10.14286  01 40 53.885  -18 33 41.70  22.0i 14SS373   W84  C~4yUX      
2017 11  10.14422  01 40 53.873  -18 33 41.85  23.0g 14SS373   W84  C~4yUX      
2017 11  24.10370  01 39 53.949  -18 32 28.76  21.7z 14SS373   W84  C~4yUX      
2017 11  27.06623  01 39 42.600  -18 31 50.67  22.1i 14SS373   W84  C~4yUX      
2017 12  08.06381  01 39 05.762  -18 28 21.86  22.6r 14SS373   W84  C~4yUX      
2017 12  08.06519  01 39 05.755  -18 28 21.68  23.8g 14SS373   W84  C~4yUX      
2018 10  01.29096  01 49 18.646  -17 23 35.51  21.7z 14SS373   W84  C~4yUX      
2018 10  21.14700  01 47 42.234  -17 31 56.51  22.2Y 14SS373   W84  C~4yUX      
2018 10  21.17169  01 47 42.103  -17 31 56.97  21.7z 14SS373   W84  C~4yUX      
2018 11  16.23330  01 45 36.473  -17 35 28.04  22.2i 14SS373   W84  C~4yUX      
2021 08  08.540453 02 07 11.532  -13 48 06.63  22.8w 14SS373   F51  C~4xS9      
2021 08  08.552784 02 07 11.538  -13 48 07.29  22.5w 14SS373   F51  C~4xS9      
2021 08  08.565240 02 07 11.554  -13 48 07.52  22.6w 14SS373   F51  C~4xS9      
2021 08  08.577760 02 07 11.526  -13 48 08.14  22.5w 14SS373   F51  C~4xS9      
2021 08  09.525045 02 07 11.117  -13 48 40.45  22.4w 14SS373   F51  C~4xS9      
2021 08  09.534486 02 07 11.112  -13 48 40.76  22.2w 14SS373   F51  C~4xS9      
2021 08  09.543906 02 07 11.110  -13 48 41.09  22.2w 14SS373   F51  C~4xS9      
2024 09  08.550847 02 21 47.872  -10 55 23.08  21.9w 14SS373   F52  C~8Df9      
2024 09  08.563345 02 21 47.835  -10 55 23.40  22.0w 14SS373   F52  C~8Df9      
2024 09  08.588330 02 21 47.759  -10 55 24.24  22.2w 14SS373   F52  C~8Df9      
2024 10  08.435914 02 19 53.226  -11 11 56.40  22.2w 14SS373   F51  C~8H3s      
2024 10  08.449847 02 19 53.157  -11 11 56.92  22.2w 14SS373   F51  C~8H3s      
2024 10  08.463816 02 19 53.089  -11 11 57.24  22.4w 14SS373   F51  C~8H3s      
2024 10  08.478025 02 19 53.039  -11 11 57.76  22.3w 14SS373   F51  C~8H3s      

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    -0.02
     2   0.0000      0.00     0.04       0.00     0.00
     3   0.2133      0.00     0.17       0.00    -0.01
     4   0.2296      0.00     0.06       0.00    -0.02
     5   0.2296      0.00     0.05       0.00    -0.01
     6   0.2296      0.00    -0.21       0.00    -0.08
     7   0.2296      0.00    -0.12       0.00    -0.01
     8   0.2296      0.00    -0.03       0.00     0.07
     9   0.2296      0.00     0.03       0.00     0.07
    10   0.2842      0.00    -0.01       0.00     0.00
    11   0.2842      0.00    -0.05       0.00     0.03
    12   0.8793      0.00    -0.08       0.00     0.08
    13   0.8984      0.00    -0.01       0.00    -0.01
    14   0.8984      0.00    -0.04       0.00     0.01
    15   0.9284      0.00    -0.05       0.00    -0.02
    16   0.9284      0.00    -0.11       0.00     0.01
    17   1.0185      0.00     0.21       0.00     0.06
    18   1.0185      0.00     0.01       0.00     0.01
    19   1.0185      0.00     0.04       0.00     0.03
    20   1.0486      0.00     0.19       0.00     0.23
    21   1.0486      0.00     0.07       0.00    -0.04
    22   1.1003      0.00    -0.05       0.00    -0.02
    23   1.1003      0.00     0.01       0.00    -0.01
    24   1.1003      0.00     0.17       0.00     0.06
    25   1.1031      0.00    -0.04       0.00    -0.01
    26   1.1031      0.00     0.02       0.00    -0.03
    27   1.1059      0.00     0.03       0.00     0.14
    28   1.1224      0.00    -0.03       0.00    -0.05
    29   1.1224      0.00     0.00       0.00    -0.02
    30   1.1224      0.00     0.06       0.00    -0.16
    31   1.1224      0.00     0.03       0.00    -0.03
    32   1.1224      0.00     0.00       0.00    -0.06
    33   1.1224      0.00    -0.13       0.00     0.09
    34   1.1332      0.00    -0.03       0.00    -0.04
    35   1.1332      0.00     0.03       0.00    -0.04
    36   2.0151      0.00    -0.12       0.00     0.01
    37   2.0151      0.00    -0.05       0.00     0.00
    38   2.0151      0.00    -0.02       0.00     0.05
    39   2.0151      0.00    -0.04       0.00    -0.01
    40   2.0151      0.00     0.08       0.00     0.09
    41   2.0151      0.00     0.08       0.00     0.03
    42   3.0089      0.00    -0.08       0.00    -0.07
    43   3.1127      0.00    -0.07       0.00    -0.07
    44   3.1127      0.00     0.09       0.00     0.09
    45   3.1127      0.00     0.01       0.00    -0.06
    46   3.1509      0.00     0.12       0.00    -0.08
    47   3.1590      0.00    -0.01       0.00    -0.04
    48   3.1891      0.00     0.05       0.00    -0.04
    49   3.1891      0.00     0.01       0.00     0.11
    50   4.0029      0.00     0.06       0.00    -0.04
    51   4.0572      0.00     0.07       0.00    -0.08
    52   4.0573      0.00    -0.01       0.00    -0.08
    53   4.1287      0.00     0.05       0.00    -0.09
    54   6.8564      0.00    -0.20       0.00     0.17
    55   6.8564      0.00    -0.02       0.00    -0.07
    56   6.8565      0.00     0.30       0.00     0.13
    57   6.8565      0.00    -0.03       0.00    -0.06
    58   6.8591      0.00    -0.12       0.00     0.05
    59   6.8591      0.00    -0.11       0.00     0.06
    60   6.8592      0.00    -0.07       0.00     0.06
    61   9.9420      0.00     0.03       0.00    -0.12
    62   9.9420      0.00     0.02       0.00     0.00
    63   9.9421      0.00    -0.03       0.00     0.06
    64  10.0238      0.00    -0.02       0.00     0.06
    65  10.0239      0.00    -0.07       0.00    -0.06
    66  10.0239      0.00    -0.09       0.00     0.02
    67  10.0239      0.00     0.17       0.00    -0.09

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.

14SS373    quality flag:3

Type:       SCATNEAR  SCATNEAR  SCATNEAR

axisobj        58.274    58.274    58.275
ecceobj         0.353     0.353     0.353
incobj         29.957    29.957    29.957
qmin           35.725    35.742    35.751
qmax           80.597    80.705    80.664
amean          57.688    57.687    57.687
amin           57.051    57.051    57.056
amax           58.519    58.480    58.484
emean           0.359     0.359     0.359
emin            0.338     0.338     0.339
emax            0.379     0.380     0.380
imean          28.087    28.088    28.087
imin           27.464    27.465    27.464
imax           28.819    28.824    28.813
excite_mean     0.592     0.592     0.592
fracstop        1.000     1.000     1.000
cjmean          2.802     2.802     2.802

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       155.2     155.2     155.2
kozaiamp        180.0     180.0     180.0