Orbit Fit and Astrometric record for 13TC188

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: 13TC188   
# Created Sun Nov 24 02:09:40 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     35 observations of     35
# Arc:   7.18y
# First observation: 2013/09/09
#  Last observation: 2020/11/14
# Chi-squared of fit:    26.34 DOF:     64 RMS:  0.15
# Min/Max residuals:    -0.32    0.84
# Exact a, adot, b, bdot, g, gdot:
  1.705312E-05  2.780953E-02 -1.094321E-06 -1.499143E-04  2.614624E-02 -2.152226E-04
# Covariance matrix:
  3.8385E-13 -1.1118E-13 -2.0738E-15  5.7498E-17  9.4321E-14 -4.0099E-13
 -1.1118E-13  1.9041E-13  7.1477E-16 -1.5261E-15  1.9911E-13  1.0804E-12
 -2.0738E-15  7.1477E-16  2.0725E-13 -5.0950E-14 -1.0962E-15  4.7543E-15
  5.7498E-17 -1.5261E-15 -5.0950E-14  1.5821E-14 -2.2309E-15 -9.3583E-15
  9.4321E-14  1.9911E-13 -1.0962E-15 -2.2309E-15  3.9757E-13  1.2025E-12
 -4.0099E-13  1.0804E-12  4.7543E-15 -9.3583E-15  1.2025E-12  6.6906E-12
#      lat0       lon0       xBary       yBary       zBary        JD0
  -11.501750   23.002953    0.599660   -0.161477   -0.794063  2456544.844978
# Heliocentric elements and errors
Epoch:              2456544.5000  =  2013/09/09
Mean Anomaly:          349.70234 +/-     0.035
Argument of Peri:      280.73014 +/-     0.045
Long of Asc Node:      114.68009 +/-     0.001
Inclination:            11.27423 +/-     0.000
Eccentricity:         0.12267484 +/-    0.0001
Semi-Major Axis:     44.37632070 +/-    0.0041
Time of Perihelion: 2459633.0976 +/-      17.9
Perihelion:          38.93246279 +/-    0.0047
Aphelion:            49.82017860 +/-    0.0055
Period (y)              295.6209 +/-      0.04
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           35.47794393 +/-    0.0008
Ecliptic Y           14.41349237 +/-    0.0003
Ecliptic Z           -7.62631876 +/-    0.0002
Ecliptic XDOT        -0.00116734 +/-    0.0000
Ecliptic YDOT         0.00266946 +/-    0.0000
Ecliptic ZDOT        -0.00001075 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   39.04606591 +/-    0.0008
Geocenter to KBO     38.24645611 +/-    0.0009
# Hcoef:  7.20

The following table shows the complete astrometric record for 13TC188. 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 (13TC188) followed by the observatory code and reference code for the source of the astrometry.

2013 09  09.34420  01 42 05.171  -01 45 17.37  23.3g 13TC188   W84  C~4yRF      
2013 10  03.29120  01 40 27.653  -01 58 05.59  23.2g 13TC188   W84  C~4yRF      
2013 10  03.29120  01 40 27.65   -01 58 05.6   23.6g 13TC188   W84  C~3clR      
2014 11  16.15940  01 43 01.195  -01 41 17.06  22.9i 13TC188   W84  C~4yRF      
2014 11  16.15940  01 43 01.20   -01 41 17.1   23.0i 13TC188   W84  C~3clR      
2015 11  01.20010  01 50 08.434  -01 01 49.03  22.8i 13TC188   W84  C~4yRF      
2015 11  01.20010  01 50 08.43   -01 01 49.0   22.8i 13TC188   W84  C~3clR      
2015 11  02.14393  01 50 03.907  -01 02 10.38  23.0r 13TC188   W84  C~4yRF      
2015 11  02.14393  01 50 03.91   -01 02 10.4   23.5r 13TC188   W84  C~3clR      
2015 12  18.08459  01 47 10.973  -01 09 40.87  23.0z 13TC188   W84  C~4yRF      
2015 12  18.13287  01 47 10.881  -01 09 40.66  22.8i 13TC188   W84  C~4yRF      
2015 12  18.13287  01 47 10.88   -01 09 40.7   23.0i 13TC188   W84  C~3clR      
2016 01  12.06145  01 46 44.905  -01 04 24.71  22.5r 13TC188   W84  C~4yRF      
2016 01  12.06145  01 46 44.91   -01 04 24.7   22.9r 13TC188   W84  C~3clR      
2016 11  03.17412  01 55 53.436  -00 28 05.74  23.1r 13TC188   W84  C~4yRF      
2016 11  03.17412  01 55 53.44   -00 28 05.7   23.3r 13TC188   W84  C~3clR      
2016 11  10.13098  01 55 20.635  -00 30 27.41  22.2z 13TC188   W84  C~4yRF      
2016 11  10.13098  01 55 20.63   -00 30 27.4   22.5z 13TC188   W84  C~3clR      
2016 12  06.08106  01 53 36.235  -00 35 24.22  21.9z 13TC188   W84  C~4yRF      
2016 12  06.08106  01 53 36.22   -00 35 24.2   22.5z 13TC188   W84  C~3clR      
2017 11  16.16122  02 00 51.927  +00 02 35.46  23.2r 13TC188   W84  C~4yRF      
2017 11  16.16261  02 00 51.922  +00 02 35.52  23.1i 13TC188   W84  C~4yRF      
2017 11  16.16399  02 00 51.918  +00 02 35.69  24.2g 13TC188   W84  C~4yRF      
2018 01  10.23916  01 58 25.37   +00 03 09.0   24.2g 13TC188   T09  C~7xNr      
2018 01  10.26745  01 58 25.36   +00 03 09.5   24.2g 13TC188   T09  C~7xNr      
2018 01  10.33162  01 58 25.35   +00 03 10.9   24.2g 13TC188   T09  C~7xNr      
2018 01  10.34309  01 58 25.35   +00 03 11.0   24.5g 13TC188   T09  C~7xNr      
2018 09  14.36786  02 11 32.772  +01 05 16.63  23.1r 13TC188   W84  C~4yRF      
2018 09  14.36923  02 11 32.772  +01 05 16.65  22.6i 13TC188   W84  C~4yRF      
2018 09  14.37060  02 11 32.775  +01 05 16.66  23.5g 13TC188   W84  C~4yRF      
2018 10  20.20080  02 09 01.108  +00 47 33.21  22.8z 13TC188   W84  C~4yRF      
2018 11  07.22536  02 07 32.966  +00 40 13.50  22.7r 13TC188   W84  C~4yRF      
2018 11  07.22811  02 07 32.969  +00 40 13.28  23.5g 13TC188   W84  C~4yRF      
2020 11  14.216890 02 18 55.417  +01 47 26.93  23.3G 13TC188   G37  C~4Nkr      
2020 11  14.297940 02 18 55.039  +01 47 24.60        13TC188   G37  C~4Nkr      

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    -0.12       0.00     0.17
     2   0.0656      0.00    -0.14       0.00     0.08
     3   0.0656      0.00    -0.10       0.00     0.09
     4   1.1850      0.00     0.09       0.00     0.02
     5   1.1850      0.00     0.01       0.00     0.06
     6   2.1433      0.00    -0.02       0.00    -0.01
     7   2.1433      0.00     0.04       0.00    -0.04
     8   2.1459      0.00    -0.04       0.00     0.02
     9   2.1459      0.00    -0.08       0.00     0.04
    10   2.2717      0.00    -0.08       0.00     0.06
    11   2.2718      0.00     0.17       0.00     0.01
    12   2.2718      0.00     0.19       0.00     0.05
    13   2.3401      0.00     0.12       0.00     0.02
    14   2.3401      0.00     0.05       0.00     0.01
    15   3.1508      0.00    -0.01       0.00     0.01
    16   3.1508      0.00     0.05       0.00     0.05
    17   3.1698      0.00     0.05       0.00     0.07
    18   3.1698      0.00     0.13       0.00     0.06
    19   3.2409      0.00    -0.18       0.00    -0.21
    20   3.2409      0.00     0.05       0.00    -0.23
    21   4.1857      0.00     0.08       0.00    -0.21
    22   4.1857      0.00     0.10       0.00    -0.13
    23   4.1857      0.00     0.14       0.00     0.06
    24   4.3365      0.00    -0.21       0.00    -0.09
    25   4.3365      0.00    -0.21       0.00    -0.10
    26   4.3367      0.00    -0.03       0.00     0.15
    27   4.3368      0.00     0.02       0.00     0.04
    28   5.0131      0.00    -0.03       0.00    -0.13
    29   5.0131      0.00     0.04       0.00    -0.07
    30   5.0131      0.00     0.15       0.00    -0.02
    31   5.1112      0.00    -0.03       0.00    -0.09
    32   5.1605      0.00     0.01       0.00    -0.16
    33   5.1605      0.00     0.25       0.00    -0.32
    34   7.1810      0.00    -0.23       0.00     0.84
    35   7.1813      0.00    -0.04       0.00    -0.03

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.

13TC188    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.638    44.638    44.638
ecceobj         0.127     0.127     0.127
incobj         11.274    11.274    11.274
qmin           38.017    38.092    38.057
qmax           51.006    50.969    50.952
amean          44.311    44.307    44.313
amin           43.924    43.925    43.924
amax           44.734    44.734    44.724
emean           0.125     0.124     0.124
emin            0.110     0.110     0.110
emax            0.140     0.139     0.140
imean           9.782     9.784     9.795
imin            9.141     9.141     9.140
imax           10.498    10.495    10.520
excite_mean     0.211     0.210     0.211
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       177.4     177.6     177.2
kozaiamp        180.0     180.0     179.9