Orbit Fit and Astrometric record for 13RF109

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: 13RF109   
# Created Fri May  3 01:14:47 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     79 observations of     79
# Arc:   7.12y
# First observation: 2013/09/02
#  Last observation: 2020/10/15
# Chi-squared of fit:    21.25 DOF:    152 RMS:  0.09
# Min/Max residuals:    -0.36    0.39
# Exact a, adot, b, bdot, g, gdot:
  1.578673E-05  2.552745E-02 -1.994095E-06 -3.584027E-03  2.534745E-02 -5.473026E-04
# Covariance matrix:
  1.1886E-13 -4.3455E-14 -5.2013E-15  4.4304E-15  4.8100E-14 -1.8888E-13
 -4.3455E-14  3.4562E-14  4.5217E-15 -4.4273E-15  9.0347E-15  1.9493E-13
 -5.2013E-15  4.5217E-15  6.3616E-14 -1.6457E-14 -2.7124E-16  3.0527E-14
  4.4304E-15 -4.4273E-15 -1.6457E-14  6.3019E-15 -1.0101E-15 -2.9838E-14
  4.8100E-14  9.0347E-15 -2.7124E-16 -1.0101E-15  1.1210E-13  5.6389E-14
 -1.8888E-13  1.9493E-13  3.0527E-14 -2.9838E-14  5.6389E-14  1.3132E-12
#      lat0       lon0       xBary       yBary       zBary        JD0
   -5.607748   -0.608086    0.340206   -0.092842   -0.946494  2456537.838463
# Heliocentric elements and errors
Epoch:              2456538.5000  =  2013/09/03
Mean Anomaly:          333.04102 +/-     0.037
Argument of Peri:      245.07793 +/-     0.042
Long of Asc Node:      144.90112 +/-     0.001
Inclination:             9.72531 +/-     0.000
Eccentricity:         0.06637960 +/-    0.0000
Semi-Major Axis:     42.89473514 +/-    0.0024
Time of Perihelion: 2464222.8201 +/-      13.2
Perihelion:          40.04739994 +/-    0.0028
Aphelion:            45.74207035 +/-    0.0031
Period (y)              280.9404 +/-      0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           40.20780960 +/-    0.0005
Ecliptic Y           -0.76387060 +/-    0.0000
Ecliptic Z           -3.85521374 +/-    0.0001
Ecliptic XDOT        -0.00007358 +/-    0.0000
Ecliptic YDOT         0.00275707 +/-    0.0000
Ecliptic ZDOT        -0.00037935 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   40.39945247 +/-    0.0005
Geocenter to KBO     39.45174581 +/-    0.0005
# Hcoef:  6.53

The following table shows the complete astrometric record for 13RF109. 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 (13RF109) followed by the observatory code and reference code for the source of the astrometry.

2013 09  02.337685 00 06 43.08   -05 23 07.6   23.4g 13RF109   W84  C~35bW      
2013 09  02.33821  00 06 43.081  -05 23 07.76  23.9g 13RF109   W84  C~4yQo      
2013 09  08.19449  00 06 18.088  -05 26 18.20  22.5g 13RF109   W84  C~4yQo      
2013 09  08.19449  00 06 18.09   -05 26 18.4   23.5g 13RF109   W84  C~3cl7      
2013 09  10.32435  00 06 08.749  -05 27 28.04  23.6g 13RF109   W84  C~4yQo      
2013 09  10.32435  00 06 08.75   -05 27 28.0   23.6g 13RF109   W84  C~3cl7      
2013 10  13.15178  00 03 41.183  -05 44 10.28  22.1i 13RF109   W84  C~4yQo      
2013 10  13.15178  00 03 41.18   -05 44 10.3   22.2i 13RF109   W84  C~3cl7      
2013 10  13.15458  00 03 41.172  -05 44 10.44  21.8z 13RF109   W84  C~4yQo      
2013 10  13.15458  00 03 41.17   -05 44 10.5   21.9z 13RF109   W84  C~3cl7      
2013 12  02.107014 00 01 17.92   -05 55 52.4   22.7r 13RF109   W84  C~35bW      
2013 12  02.10754  00 01 17.927  -05 55 52.66  22.8r 13RF109   W84  C~4yQo      
2014 08  18.29436  00 13 23.334  -04 51 20.56  22.1i 13RF109   W84  C~4yQo      
2014 08  18.29436  00 13 23.33   -04 51 20.6   22.1i 13RF109   W84  C~3cl7      
2014 08  18.29573  00 13 23.334  -04 51 20.56  21.8z 13RF109   W84  C~4yQo      
2014 11  13.12250  00 07 32.572  -05 30 41.94  22.1i 13RF109   W84  C~4yQo      
2014 11  13.12250  00 07 32.57   -05 30 41.9   22.1i 13RF109   W84  C~3cl7      
2014 11  14.029676 00 07 30.17   -05 30 52.5   22.2z 13RF109   W84  C~35bW      
2014 11  14.03021  00 07 30.170  -05 30 52.45  22.4z 13RF109   W84  C~4yQo      
2014 11  14.03021  00 07 30.17   -05 30 52.5   22.4z 13RF109   W84  C~3cl7      
2014 11  14.11836  00 07 29.927  -05 30 53.56  22.7r 13RF109   W84  C~4yQo      
2014 11  14.11836  00 07 29.93   -05 30 53.6   22.8r 13RF109   W84  C~3cl7      
2014 11  16.05964  00 07 24.974  -05 31 14.53  22.1z 13RF109   W84  C~4yQo      
2014 11  16.05964  00 07 24.97   -05 31 14.5   22.2z 13RF109   W84  C~3cl7      
2015 08  18.322905 00 19 05.33   -04 27 15.5   22.6r 13RF109   W84  C~35bW      
2015 08  18.32343  00 19 05.341  -04 27 15.66  22.6r 13RF109   W84  C~4yQo      
2015 11  03.09876  00 13 45.114  -05 04 24.55  22.4r 13RF109   W84  C~4yQo      
2015 11  03.09876  00 13 45.11   -05 04 24.5   22.6r 13RF109   W84  C~3cl7      
2016 09  05.24094  00 23 37.705  -04 12 46.39  22.2i 13RF109   W84  C~4yQo      
2016 09  05.24094  00 23 37.70   -04 12 46.4   22.4i 13RF109   W84  C~3cl7      
2016 09  05.24232  00 23 37.697  -04 12 46.40  22.7r 13RF109   W84  C~4yQo      
2016 09  05.24232  00 23 37.70   -04 12 46.4   22.7r 13RF109   W84  C~3cl7      
2016 09  09.16597  00 23 21.235  -04 14 54.41  21.9z 13RF109   W84  C~4yQo      
2016 09  09.16597  00 23 21.24   -04 14 54.4   22.0z 13RF109   W84  C~3cl7      
2016 09  09.34807  00 23 20.446  -04 15 00.47  23.4g 13RF109   W84  C~4yQo      
2016 09  09.34807  00 23 20.44   -04 15 00.4   23.5g 13RF109   W84  C~3cl7      
2016 09  30.18411  00 21 46.879  -04 26 12.73  22.6r 13RF109   W84  C~4yQo      
2016 09  30.18411  00 21 46.88   -04 26 12.7   22.6r 13RF109   W84  C~3cl7      
2016 09  30.18548  00 21 46.880  -04 26 12.78  22.1i 13RF109   W84  C~4yQo      
2016 09  30.18548  00 21 46.88   -04 26 12.8   22.2i 13RF109   W84  C~3cl7      
2016 09  30.18685  00 21 46.876  -04 26 12.84  23.7g 13RF109   W84  C~4yQo      
2016 09  30.18685  00 21 46.88   -04 26 12.8   23.6g 13RF109   W84  C~3cl7      
2016 09  30.18822  00 21 46.863  -04 26 12.84  22.5r 13RF109   W84  C~4yQo      
2016 09  30.18822  00 21 46.86   -04 26 12.8   22.5r 13RF109   W84  C~3cl7      
2016 09  30.18960  00 21 46.855  -04 26 12.89  22.1i 13RF109   W84  C~4yQo      
2016 09  30.18960  00 21 46.85   -04 26 12.9   22.1i 13RF109   W84  C~3cl8      
2016 09  30.19096  00 21 46.850  -04 26 12.95  23.3g 13RF109   W84  C~4yQo      
2016 09  30.19096  00 21 46.85   -04 26 13.0   23.3g 13RF109   W84  C~3cl8      
2016 10  01.19162  00 21 42.251  -04 26 43.96  22.2r 13RF109   W84  C~4yQo      
2016 10  01.19162  00 21 42.25   -04 26 43.9   22.4r 13RF109   W84  C~3cl8      
2016 10  01.19299  00 21 42.248  -04 26 43.94  22.1i 13RF109   W84  C~4yQo      
2016 10  01.19299  00 21 42.25   -04 26 43.9   22.2i 13RF109   W84  C~3cl8      
2016 10  01.19436  00 21 42.246  -04 26 44.04  23.6g 13RF109   W84  C~4yQo      
2016 10  01.19436  00 21 42.25   -04 26 44.0   23.7g 13RF109   W84  C~3cl8      
2016 11  18.14793  00 18 37.768  -04 44 14.68  21.2z 13RF109   W84  C~4yQo      
2016 11  18.14793  00 18 37.77   -04 44 14.6   21.6z 13RF109   W84  C~3cl8      
2017 09  24.307488 00 27 58.03   -03 58 35.8   22.1i 13RF109   W84  C~35bW      
2017 09  24.30801  00 27 58.038  -03 58 35.81  22.1i 13RF109   W84  C~4yQo      
2017 09  25.260556 00 27 53.69   -03 59 06.5   22.6r 13RF109   W84  C~35bW      
2017 09  25.26109  00 27 53.691  -03 59 06.57  22.6r 13RF109   W84  C~4yQo      
2017 09  25.26245  00 27 53.678  -03 59 06.46  23.2g 13RF109   W84  C~4yQo      
2017 09  26.301123 00 27 48.92   -03 59 39.8   22.1i 13RF109   W84  C~35bW      
2017 09  26.30165  00 27 48.923  -03 59 39.85  22.1i 13RF109   W84  C~4yQo      
2017 09  27.259769 00 27 44.53   -04 00 10.3   23.7g 13RF109   W84  C~35bW      
2017 09  27.26030  00 27 44.527  -04 00 10.34  23.2g 13RF109   W84  C~4yQo      
2017 10  17.238796 00 26 14.03   -04 09 58.9   22.7r 13RF109   W84  C~35bW      
2017 10  17.23932  00 26 14.029  -04 09 58.92  22.5r 13RF109   W84  C~4yQo      
2017 10  27.169398 00 25 32.44   -04 14 02.2   21.8z 13RF109   W84  C~35bW      
2017 10  27.16992  00 25 32.441  -04 14 02.22  21.6z 13RF109   W84  C~4yQo      
2017 10  29.123333 00 25 24.73   -04 14 45.2   21.8z 13RF109   W84  C~35bW      
2018 09  09.34532  00 34 48.069  -03 25 44.26  22.6r 13RF109   W84  C~4yQo      
2018 11  08.17258  00 30 30.440  -03 53 30.12  22.7r 13RF109   W84  C~4yQo      
2018 11  26.08235  00 29 39.479  -03 57 02.11  24.0g 13RF109   W84  C~4yQo      
2020 09  16.41215  00 45 43.210  -02 40 05.13  22.6w 13RF109   F51  C~48Af      
2020 09  16.42997  00 45 43.098  -02 40 06.19  22.5w 13RF109   F51  C~48Af      
2020 09  16.44785  00 45 43.034  -02 40 06.64  22.6w 13RF109   F51  C~48Af      
2020 10  15.47159  00 43 31.270  -02 55 07.70  22.5w 13RF109   F51  C~49w4      
2020 10  15.48922  00 43 31.191  -02 55 08.58  22.6w 13RF109   F51  C~49w4      
2020 10  15.52470  00 43 31.047  -02 55 08.97  22.4w 13RF109   F51  C~49w4      

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    -0.03
     2   0.0000      0.00     0.09       0.00    -0.18
     3   0.0160      0.00    -0.06       0.00    -0.03
     4   0.0160      0.00    -0.09       0.00     0.17
     5   0.0219      0.00     0.05       0.00    -0.00
     6   0.0219      0.00     0.03       0.00    -0.04
     7   0.1117      0.00    -0.05       0.00     0.10
     8   0.1117      0.00    -0.09       0.00     0.08
     9   0.1118      0.00    -0.06       0.00    -0.05
    10   0.1118      0.00    -0.03       0.00     0.01
    11   0.2485      0.00    -0.04       0.00     0.18
    12   0.2485      0.00     0.07       0.00    -0.08
    13   0.9581      0.00    -0.09       0.00    -0.06
    14   0.9581      0.00    -0.03       0.00    -0.02
    15   0.9581      0.00     0.04       0.00     0.02
    16   1.1959      0.00    -0.05       0.00     0.06
    17   1.1959      0.00    -0.02       0.00     0.02
    18   1.1983      0.00     0.10       0.00     0.06
    19   1.1983      0.00     0.12       0.00     0.06
    20   1.1983      0.00     0.12       0.00     0.11
    21   1.1986      0.00     0.10       0.00    -0.03
    22   1.1986      0.00     0.06       0.00     0.01
    23   1.2039      0.00    -0.08       0.00    -0.00
    24   1.2039      0.00    -0.02       0.00    -0.03
    25   1.9575      0.00    -0.18       0.00     0.08
    26   1.9575      0.00     0.01       0.00    -0.06
    27   2.1677      0.00    -0.18       0.00     0.08
    28   2.1677      0.00    -0.12       0.00     0.03
    29   3.0086      0.00    -0.03       0.00    -0.00
    30   3.0086      0.00     0.04       0.00     0.01
    31   3.0086      0.00     0.01       0.00     0.04
    32   3.0086      0.00     0.05       0.00     0.04
    33   3.0194      0.00     0.15       0.00    -0.01
    34   3.0194      0.00     0.07       0.00    -0.02
    35   3.0199      0.00     0.01       0.00    -0.06
    36   3.0199      0.00     0.10       0.00    -0.13
    37   3.0769      0.00    -0.01       0.00     0.04
    38   3.0769      0.00    -0.02       0.00     0.01
    39   3.0769      0.00     0.09       0.00    -0.01
    40   3.0769      0.00     0.09       0.00     0.01
    41   3.0769      0.00     0.18       0.00     0.03
    42   3.0769      0.00     0.12       0.00    -0.01
    43   3.0769      0.00    -0.02       0.00     0.07
    44   3.0769      0.00     0.02       0.00     0.03
    45   3.0769      0.00    -0.07       0.00     0.02
    46   3.0769      0.00     0.00       0.00     0.03
    47   3.0769      0.00     0.02       0.00    -0.04
    48   3.0769      0.00     0.02       0.00     0.01
    49   3.0797      0.00    -0.06       0.00    -0.01
    50   3.0797      0.00    -0.04       0.00    -0.07
    51   3.0797      0.00     0.04       0.00     0.03
    52   3.0797      0.00     0.01       0.00    -0.01
    53   3.0797      0.00     0.13       0.00    -0.03
    54   3.0797      0.00     0.07       0.00    -0.07
    55   3.2110      0.00     0.02       0.00    -0.06
    56   3.2110      0.00    -0.01       0.00    -0.14
    57   4.0602      0.00    -0.19       0.00     0.12
    58   4.0602      0.00    -0.03       0.00     0.13
    59   4.0628      0.00    -0.01       0.00     0.00
    60   4.0628      0.00     0.04       0.00    -0.05
    61   4.0628      0.00    -0.06       0.00     0.10
    62   4.0656      0.00    -0.06       0.00    -0.05
    63   4.0656      0.00     0.03       0.00    -0.08
    64   4.0682      0.00    -0.01       0.00    -0.06
    65   4.0682      0.00    -0.02       0.00    -0.08
    66   4.1229      0.00    -0.02       0.00    -0.01
    67   4.1229      0.00    -0.00       0.00    -0.02
    68   4.1501      0.00     0.05       0.00     0.06
    69   4.1501      0.00     0.10       0.00     0.05
    70   4.1555      0.00    -0.04       0.00    -0.13
    71   5.0185      0.00     0.04       0.00    -0.04
    72   5.1823      0.00     0.01       0.00    -0.07
    73   5.2313      0.00     0.02       0.00    -0.07
    74   7.0392      0.00     0.33       0.00     0.39
    75   7.0393      0.00    -0.17       0.00    -0.09
    76   7.0393      0.00     0.05       0.00     0.04
    77   7.1188      0.00    -0.21       0.00     0.03
    78   7.1188      0.00    -0.18       0.00    -0.36
    79   7.1189      0.00     0.10       0.00     0.24

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.

13RF109    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        43.129    43.129    43.129
ecceobj         0.071     0.071     0.071
incobj          9.703     9.703     9.703
qmin           38.933    38.964    38.903
qmax           47.258    47.214    47.239
amean          42.925    42.925    42.925
amin           42.587    42.588    42.580
amax           43.294    43.277    43.291
emean           0.074     0.074     0.074
emin            0.059     0.059     0.059
emax            0.092     0.091     0.091
imean           9.085     9.085     9.085
imin            8.185     8.185     8.185
imax            9.914     9.914     9.911
excite_mean     0.174     0.174     0.174
fracstop        1.000     1.000     1.000
cjmean          3.052     3.052     3.052

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       184.7     184.8     184.6
kozaiamp        180.0     180.0     179.9