Orbit Fit and Astrometric record for 13TH187

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: 13TH187   
# Created Tue Apr 16 01:15:11 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     35 observations of     35
# Arc:  12.05y
# First observation: 2005/08/09
#  Last observation: 2017/08/28
# Chi-squared of fit:    11.56 DOF:     64 RMS:  0.10
# Min/Max residuals:    -0.24    0.25
# Exact a, adot, b, bdot, g, gdot:
  1.557107E-05  2.425582E-02  5.074225E-07  7.104470E-05  2.432443E-02  8.093391E-04
# Covariance matrix:
  4.8671E-13 -1.0297E-13  1.5917E-16 -1.6575E-16 -5.2986E-14 -2.1640E-13
 -1.0297E-13  9.0872E-14 -2.5126E-16  2.7519E-16  1.6049E-13  2.9012E-13
  1.5917E-16 -2.5126E-16  4.0834E-13 -4.1518E-14 -5.0345E-16 -8.4028E-16
 -1.6575E-16  2.7519E-16 -4.1518E-14  4.6855E-15  5.6662E-16  9.1791E-16
 -5.2986E-14  1.6049E-13 -5.0345E-16  5.6662E-16  4.0816E-13  5.2328E-13
 -2.1640E-13  2.9012E-13 -8.4028E-16  9.1791E-16  5.2328E-13  9.7923E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
   -2.880862    2.649496    0.728595   -0.035476   -0.707289  2453591.685953
# Heliocentric elements and errors
Epoch:              2453592.5000  =  2005/08/10
Mean Anomaly:           17.51404 +/-     0.054
Argument of Peri:      252.98421 +/-     0.060
Long of Asc Node:       89.24136 +/-     0.003
Inclination:             2.83442 +/-     0.000
Eccentricity:         0.05197164 +/-    0.0000
Semi-Major Axis:     43.98896071 +/-    0.0039
Time of Perihelion: 2448408.1073 +/-      15.9
Perihelion:          41.70278241 +/-    0.0043
Aphelion:            46.27513902 +/-    0.0046
Period (y)              291.7587 +/-      0.04
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           41.75196092 +/-    0.0011
Ecliptic Y            1.20229036 +/-    0.0001
Ecliptic Z           -2.06618841 +/-    0.0001
Ecliptic XDOT        -0.00003333 +/-    0.0000
Ecliptic YDOT         0.00272461 +/-    0.0000
Ecliptic ZDOT         0.00000344 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.82032985 +/-    0.0011
Geocenter to KBO     41.11091857 +/-    0.0011
# Hcoef:  7.19

The following table shows the complete astrometric record for 13TH187. 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 (13TH187) followed by the observatory code and reference code for the source of the astrometry.

2005 08  09.18521  00 14 18.26   -01 35 24.1   22.2R 13TH187   807  C~3clQ      
2005 08  10.16987  00 14 15.52   -01 35 44.8         13TH187   807  C~3clQ      
2005 08  10.30462  00 14 15.14   -01 35 47.8         13TH187   807  C~3clQ      
2013 09  29.23112  00 51 54.810  +02 29 54.39  23.8r 13TH187   W84  C~4yRC      
2013 10  11.21533  00 51 01.154  +02 24 17.91  24.4g 13TH187   W84  C~4yRC      
2013 10  13.10477  00 50 52.725  +02 23 26.04  22.7z 13TH187   W84  C~4yRC      
2013 10  13.14869  00 50 52.539  +02 23 24.71  22.7i 13TH187   W84  C~4yRC      
2013 10  13.14869  00 50 52.54   +02 23 24.7   23.0i 13TH187   W84  C~3clQ      
2013 11  08.18539  00 49 04.755  +02 12 50.68  23.5r 13TH187   W84  C~4yRC      
2013 11  08.18539  00 49 04.76   +02 12 50.7   23.4r 13TH187   W84  C~3clQ      
2013 11  08.18675  00 49 04.745  +02 12 50.74  22.8i 13TH187   W84  C~4yRC      
2013 11  08.18675  00 49 04.75   +02 12 50.7   23.1i 13TH187   W84  C~3clQ      
2013 11  22.13050  00 48 19.622  +02 08 49.67  23.5i 13TH187   W84  C~4yRD      
2013 11  22.13189  00 48 19.616  +02 08 49.59  22.9z 13TH187   W84  C~4yRD      
2014 08  18.32090  00 59 34.669  +03 20 27.66  23.0i 13TH187   W84  C~4yRD      
2014 08  18.32090  00 59 34.67   +03 20 27.7   23.0i 13TH187   W84  C~3clQ      
2014 10  21.21035  00 55 23.522  +02 53 04.98  23.6r 13TH187   W84  C~4yRD      
2014 10  21.21035  00 55 23.52   +02 53 05.0   23.7r 13TH187   W84  C~3clQ      
2014 11  13.07356  00 53 52.464  +02 44 22.51  24.4g 13TH187   W84  C~4yRD      
2014 11  13.08217  00 53 52.424  +02 44 22.16  23.2r 13TH187   W84  C~4yRD      
2014 11  13.08217  00 53 52.43   +02 44 22.1   23.2r 13TH187   W84  C~3clQ      
2015 11  07.10209  00 59 19.200  +03 19 22.85  23.5r 13TH187   W84  C~4yRD      
2015 11  07.10209  00 59 19.20   +03 19 22.9   23.6r 13TH187   W84  C~3clQ      
2015 11  07.10346  00 59 19.192  +03 19 22.67  23.5i 13TH187   W84  C~4yRD      
2015 11  07.10484  00 59 19.203  +03 19 22.75  24.3g 13TH187   W84  C~4yRD      
2016 08  26.37683  01 09 17.566  +04 22 49.52  23.3i 13TH187   W84  C~4yRD      
2016 08  26.37821  01 09 17.551  +04 22 49.52  23.1z 13TH187   W84  C~4yRD      
2016 09  01.36467  01 08 59.034  +04 20 39.73  23.1i 13TH187   W84  C~4yRD      
2016 09  01.36604  01 08 59.036  +04 20 39.82  23.6r 13TH187   W84  C~4yRD      
2016 09  01.36604  01 08 59.03   +04 20 39.8   23.8r 13TH187   W84  C~3clQ      
2016 09  01.36741  01 08 59.011  +04 20 39.66  24.2g 13TH187   W84  C~4yRD      
2016 11  05.16171  01 04 27.874  +03 52 35.63  23.0r 13TH187   W84  C~4yRD      
2016 11  05.16308  01 04 27.870  +03 52 35.40  22.7i 13TH187   W84  C~4yRD      
2017 08  28.28950  01 14 15.759  +04 54 36.17  23.3r 13TH187   W84  C~4yRD      
2017 08  28.29088  01 14 15.757  +04 54 36.28  22.9i 13TH187   W84  C~4yRD      

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     0.08       0.00    -0.07
     2   0.0027      0.00    -0.11       0.00     0.16
     3   0.0031      0.00    -0.01       0.00     0.05
     4   8.1398      0.00    -0.07       0.00    -0.02
     5   8.1726      0.00    -0.14       0.00     0.02
     6   8.1777      0.00    -0.11       0.00     0.05
     7   8.1779      0.00     0.08       0.00    -0.08
     8   8.1779      0.00     0.10       0.00    -0.09
     9   8.2491      0.00     0.17       0.00    -0.05
    10   8.2491      0.00     0.09       0.00    -0.07
    11   8.2491      0.00     0.09       0.00    -0.02
    12   8.2491      0.00     0.02       0.00     0.02
    13   8.2873      0.00     0.00       0.00     0.06
    14   8.2873      0.00    -0.03       0.00    -0.00
    15   9.0243      0.00    -0.01       0.00     0.05
    16   9.0243      0.00     0.00       0.00     0.09
    17   9.1992      0.00    -0.21       0.00    -0.08
    18   9.1992      0.00    -0.18       0.00    -0.10
    19   9.2618      0.00     0.25       0.00     0.01
    20   9.2619      0.00     0.20       0.00    -0.24
    21   9.2619      0.00     0.11       0.00    -0.18
    22  10.2448      0.00    -0.08       0.00     0.07
    23  10.2448      0.00    -0.08       0.00     0.02
    24  10.2448      0.00    -0.12       0.00    -0.13
    25  10.2448      0.00     0.12       0.00    -0.02
    26  11.0478      0.00     0.09       0.00     0.07
    27  11.0478      0.00    -0.07       0.00     0.10
    28  11.0641      0.00     0.03       0.00     0.04
    29  11.0642      0.00     0.04       0.00     0.14
    30  11.0642      0.00     0.13       0.00     0.16
    31  11.0642      0.00    -0.17       0.00     0.03
    32  11.2416      0.00    -0.05       0.00     0.14
    33  11.2416      0.00    -0.03       0.00    -0.05
    34  12.0523      0.00    -0.01       0.00    -0.07
    35  12.0523      0.00     0.02       0.00     0.07

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.

13TH187    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.506    44.506    44.506
ecceobj         0.062     0.062     0.062
incobj          2.834     2.834     2.834
qmin           40.906    40.906    40.906
qmax           47.775    47.775    47.775
amean          44.232    44.232    44.232
amin           43.885    43.885    43.884
amax           44.590    44.590    44.591
emean           0.056     0.056     0.056
emin            0.041     0.041     0.040
emax            0.072     0.072     0.071
imean           1.150     1.150     1.150
imin            0.457     0.457     0.457
imax            1.704     1.704     1.705
excite_mean     0.060     0.060     0.060
fracstop        1.000     1.000     1.000
cjmean          3.100     3.100     3.100

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       164.6     164.5     164.6
kozaiamp        180.0     180.0     180.0