Orbit Fit and Astrometric record for 13TD172

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: 13TD172   
# Created Sat Apr 27 01:15:17 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     37 observations of     37
# Arc:   6.15y
# First observation: 2013/10/04
#  Last observation: 2019/11/27
# Chi-squared of fit:    16.07 DOF:     68 RMS:  0.12
# Min/Max residuals:    -0.32    0.35
# Exact a, adot, b, bdot, g, gdot:
  1.447243E-05  2.459223E-02  2.989324E-06  4.781614E-03  2.520016E-02 -3.972576E-03
# Covariance matrix:
  2.4450E-13 -8.8384E-14  7.7586E-15 -1.7621E-14  3.5092E-13 -5.9332E-13
 -8.8384E-14  2.2183E-13 -1.8611E-14  4.4847E-14  4.3666E-14  1.4650E-12
  7.7586E-15 -1.8611E-14  5.7474E-14 -1.7820E-14 -1.2661E-15 -1.3034E-13
 -1.7621E-14  4.4847E-14 -1.7820E-14  2.1404E-14  5.4798E-15  3.1359E-13
  3.5092E-13  4.3666E-14 -1.2661E-15  5.4798E-15  8.3676E-13  1.3903E-13
 -5.9332E-13  1.4650E-12 -1.3034E-13  3.1359E-13  1.3903E-13  1.0252E-11
#      lat0       lon0       xBary       yBary       zBary        JD0
    0.311281    7.520408   -0.056375    0.005531   -0.998755  2456569.653808
# Heliocentric elements and errors
Epoch:              2456570.5000  =  2013/10/05
Mean Anomaly:          294.79977 +/-     0.027
Argument of Peri:       85.07029 +/-     0.040
Long of Asc Node:        6.04240 +/-     0.000
Inclination:            11.00880 +/-     0.000
Eccentricity:         0.16348302 +/-    0.0001
Semi-Major Axis:     42.57409675 +/-    0.0065
Time of Perihelion: 2474947.0186 +/-      20.4
Perihelion:          35.61395495 +/-    0.0076
Aphelion:            49.53423854 +/-    0.0093
Period (y)              277.7962 +/-      0.06
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           40.32265947 +/-    0.0014
Ecliptic Y            5.38313238 +/-    0.0002
Ecliptic Z            0.21568274 +/-    0.0000
Ecliptic XDOT        -0.00078653 +/-    0.0000
Ecliptic YDOT         0.00259060 +/-    0.0000
Ecliptic ZDOT         0.00051728 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   40.68107135 +/-    0.0014
Geocenter to KBO     39.68242621 +/-    0.0014
# Hcoef:  6.90

The following table shows the complete astrometric record for 13TD172. 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 (13TD172) followed by the observatory code and reference code for the source of the astrometry.

2013 10  04.15303  00 27 07.914  +03 16 12.68  23.5g 13TD172   W84  C~4yR8      
2013 10  04.15303  00 27 07.92   +03 16 12.7   24.0g 13TD172   W84  C~3clO      
2013 10  13.09336  00 26 26.438  +03 12 11.00  22.3z 13TD172   W84  C~4yR8      
2013 10  13.09336  00 26 26.44   +03 12 11.0   22.4z 13TD172   W84  C~3clO      
2013 10  13.12065  00 26 26.316  +03 12 10.36  22.6i 13TD172   W84  C~4yR8      
2013 10  13.12065  00 26 26.31   +03 12 10.3   22.6i 13TD172   W84  C~3clO      
2013 10  28.06792  00 25 21.469  +03 05 53.34  23.0r 13TD172   W84  C~4yR8      
2013 10  28.06792  00 25 21.47   +03 05 53.4   23.4r 13TD172   W84  C~3clO      
2013 11  08.16809  00 24 39.581  +03 01 52.59  23.1r 13TD172   W84  C~4yR8      
2013 11  08.16809  00 24 39.58   +03 01 52.6   23.3r 13TD172   W84  C~3clO      
2013 11  22.07536  00 23 58.110  +02 57 59.81  22.7r 13TD172   W84  C~4yR9      
2013 11  22.07536  00 23 58.11   +02 57 59.8   23.1r 13TD172   W84  C~3clO      
2013 11  22.07674  00 23 58.107  +02 58 00.13  22.1i 13TD172   W84  C~4yR9      
2013 11  22.07674  00 23 58.11   +02 58 00.0   22.6i 13TD172   W84  C~3clO      
2013 11  22.12663  00 23 57.987  +02 57 59.08  22.5z 13TD172   W84  C~4yR9      
2013 11  22.12663  00 23 57.99   +02 57 59.1   22.5z 13TD172   W84  C~3clO      
2013 11  23.10640  00 23 55.605  +02 57 46.05  22.5i 13TD172   W84  C~4yR9      
2013 11  23.10640  00 23 55.61   +02 57 46.1   22.6i 13TD172   W84  C~3clO      
2014 10  21.21921  00 30 36.775  +03 57 19.64  22.8r 13TD172   W84  C~4yR9      
2014 10  21.21921  00 30 36.78   +03 57 19.6   22.9r 13TD172   W84  C~3clO      
2014 10  27.19966  00 30 11.014  +03 54 49.47  23.3g 13TD172   W84  C~4yR9      
2014 10  28.17823  00 30 06.963  +03 54 26.01  23.1r 13TD172   W84  C~4yR9      
2014 10  28.17823  00 30 06.96   +03 54 26.0   23.2r 13TD172   W84  C~3clO      
2014 10  28.18239  00 30 06.949  +03 54 26.03  23.8g 13TD172   W84  C~4yR9      
2014 10  28.18239  00 30 06.95   +03 54 26.0   23.7g 13TD172   W84  C~3clO      
2014 10  29.12351  00 30 03.078  +03 54 03.35  22.9z 13TD172   W84  C~4yR9      
2014 10  29.17651  00 30 02.845  +03 54 02.18  22.5i 13TD172   W84  C~4yR9      
2014 10  29.17651  00 30 02.85   +03 54 02.2   22.5i 13TD172   W84  C~3clO      
2014 10  29.19088  00 30 02.794  +03 54 01.64  23.0r 13TD172   W84  C~4yR9      
2014 10  29.19088  00 30 02.79   +03 54 01.7   23.2r 13TD172   W84  C~3clO      
2014 11  13.09695  00 29 07.642  +03 48 42.40  22.9z 13TD172   W84  C~4yR9      
2014 11  15.10387  00 29 01.258  +03 48 05.96  22.8z 13TD172   W84  C~4yR9      
2014 11  15.10387  00 29 01.26   +03 48 06.0   22.7z 13TD172   W84  C~3clO      
2019 10  26.113940 00 54 46.949  +08 01 42.78  22.6G 13TD172   G37  C~3clO      
2019 10  26.182540 00 54 46.629  +08 01 40.81        13TD172   G37  C~3clO      
2019 11  27.176060 00 52 44.221  +07 49 32.83  23.1G 13TD172   G37  C~3clO      
2019 11  27.237880 00 52 44.033  +07 49 31.75        13TD172   G37  C~3clO      

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     0.18       0.00     0.08
     2   0.0000      0.00     0.27       0.00     0.10
     3   0.0245      0.00    -0.08       0.00    -0.17
     4   0.0245      0.00    -0.05       0.00    -0.17
     5   0.0246      0.00    -0.11       0.00    -0.14
     6   0.0246      0.00    -0.02       0.00    -0.08
     7   0.0655      0.00     0.11       0.00    -0.12
     8   0.0655      0.00     0.12       0.00    -0.06
     9   0.0959      0.00     0.02       0.00     0.06
    10   0.0959      0.00     0.00       0.00     0.07
    11   0.1339      0.00    -0.11       0.00     0.00
    12   0.1339      0.00    -0.11       0.00     0.01
    13   0.1339      0.00    -0.06       0.00     0.22
    14   0.1339      0.00    -0.11       0.00     0.35
    15   0.1341      0.00    -0.00       0.00    -0.02
    16   0.1341      0.00     0.04       0.00    -0.00
    17   0.1368      0.00     0.06       0.00    -0.02
    18   0.1368      0.00    -0.02       0.00    -0.07
    19   1.0460      0.00     0.17       0.00    -0.05
    20   1.0460      0.00     0.10       0.00    -0.01
    21   1.0624      0.00    -0.32       0.00    -0.28
    22   1.0651      0.00    -0.04       0.00    -0.03
    23   1.0651      0.00     0.00       0.00    -0.02
    24   1.0651      0.00     0.07       0.00     0.07
    25   1.0651      0.00     0.06       0.00     0.10
    26   1.0677      0.00     0.09       0.00    -0.01
    27   1.0678      0.00    -0.01       0.00     0.10
    28   1.0678      0.00    -0.08       0.00     0.08
    29   1.0679      0.00    -0.01       0.00    -0.05
    30   1.0679      0.00     0.05       0.00    -0.11
    31   1.1087      0.00    -0.16       0.00    -0.07
    32   1.1142      0.00     0.02       0.00     0.17
    33   1.1142      0.00    -0.01       0.00     0.13
    34   6.0588      0.00    -0.13       0.00     0.06
    35   6.0589      0.00    -0.14       0.00    -0.09
    36   6.1465      0.00     0.23       0.00     0.02
    37   6.1467      0.00     0.08       0.00     0.00

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.

13TD172    quality flag:3

Type:       SCATNEAR  SCATNEAR  SCATNEAR

axisobj        42.798    42.798    42.798
ecceobj         0.163     0.163     0.163
incobj         10.973    10.973    10.973
qmin           33.903    34.025    34.010
qmax           51.712    51.731    51.632
amean          42.582    42.580    42.581
amin           42.136    42.119    42.132
amax           43.074    43.046    43.038
emean           0.168     0.168     0.168
emin            0.142     0.142     0.141
emax            0.202     0.203     0.201
imean           6.911     6.850     6.867
imin            2.229     2.085     2.105
imax           11.986    11.985    11.987
excite_mean     0.212     0.211     0.211
fracstop        1.000     1.000     1.000
cjmean          3.030     3.030     3.030

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       180.8     181.2     181.1
kozaiamp        180.0     180.0     180.0