Orbit Fit and Astrometric record for 13SC112

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: 13SC112   
# Created Wed Dec  4 02:09:35 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     21 observations of     21
# Arc:   5.16y
# First observation: 2013/09/28
#  Last observation: 2018/11/26
# Chi-squared of fit:     5.16 DOF:     36 RMS:  0.09
# Min/Max residuals:    -0.26    0.14
# Exact a, adot, b, bdot, g, gdot:
  1.585570E-05  2.424584E-02  1.878657E-06  3.891329E-03  2.455347E-02 -2.566456E-03
# Covariance matrix:
  3.9162E-13 -1.5056E-13  4.8777E-15 -1.1548E-14  1.2723E-13 -6.1520E-13
 -1.5056E-13  2.7336E-13 -2.5496E-14  4.4133E-14  1.3861E-13  2.2975E-12
  4.8777E-15 -2.5496E-14  2.8084E-13 -7.5654E-14 -2.0517E-14 -2.3941E-13
 -1.1548E-14  4.4133E-14 -7.5654E-14  3.2041E-14  2.9475E-14  4.1027E-13
  1.2723E-13  1.3861E-13 -2.0517E-14  2.9475E-14  4.1058E-13  1.5071E-12
 -6.1520E-13  2.2975E-12 -2.3941E-13  4.1027E-13  1.5071E-12  2.1339E-11
#      lat0       lon0       xBary       yBary       zBary        JD0
   -2.654112    7.922951    0.054448   -0.046249   -0.999729  2456563.611158
# Heliocentric elements and errors
Epoch:              2456564.5000  =  2013/09/29
Mean Anomaly:          308.92313 +/-     0.033
Argument of Peri:       47.65164 +/-     0.050
Long of Asc Node:       23.57459 +/-     0.000
Inclination:             9.47869 +/-     0.000
Eccentricity:         0.12728266 +/-    0.0002
Semi-Major Axis:     44.81636966 +/-    0.0053
Time of Perihelion: 2472112.5235 +/-      19.5
Perihelion:          39.11202292 +/-    0.0094
Aphelion:            50.52071640 +/-    0.0102
Period (y)              300.0290 +/-      0.05
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           41.29366013 +/-    0.0011
Ecliptic Y            5.69501284 +/-    0.0001
Ecliptic Z           -1.88588060 +/-    0.0001
Ecliptic XDOT        -0.00064207 +/-    0.0000
Ecliptic YDOT         0.00263979 +/-    0.0000
Ecliptic ZDOT         0.00044683 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.72723166 +/-    0.0010
Geocenter to KBO     40.72753999 +/-    0.0011
# Hcoef:  7.04

The following table shows the complete astrometric record for 13SC112. 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 (13SC112) followed by the observatory code and reference code for the source of the astrometry.

2013 09  28.11038  00 33 17.637  +00 42 14.23  23.7g 13SC112   W84  C~52RU      
2013 10  13.11779  00 32 09.678  +00 35 39.19  23.1z 13SC112   W84  C~52RU      
2013 11  22.14218  00 29 42.971  +00 23 02.94  22.8i 13SC112   W84  C~52RU      
2013 12  02.11468  00 29 21.927  +00 21 47.10  23.4r 13SC112   W84  C~52RU      
2014 11  13.06939  00 34 52.925  +01 09 54.24  23.3i 13SC112   W84  C~52RU      
2014 11  13.15233  00 34 52.647  +01 09 52.87  22.7z 13SC112   W84  C~52RU      
2016 09  09.28195  00 49 00.333  +03 06 20.73  22.6i 13SC112   W84  C~52RU      
2016 11  08.11301  00 44 40.307  +02 41 36.66  22.7i 13SC112   W84  C~52RU      
2016 11  25.06487  00 43 46.829  +02 37 15.89  23.3r 13SC112   W84  C~52RU      
2016 11  25.06625  00 43 46.820  +02 37 15.55  23.1i 13SC112   W84  C~52RU      
2016 11  28.09982  00 43 39.346  +02 36 43.74  23.0z 13SC112   W84  C~52RU      
2017 08  28.27714  00 54 35.764  +03 56 25.67  22.9i 13SC112   W84  C~52RU      
2017 08  28.27853  00 54 35.754  +03 56 25.61  23.3r 13SC112   W84  C~52RU      
2017 08  28.27990  00 54 35.749  +03 56 25.62  23.5g 13SC112   W84  C~52RU      
2017 09  27.23225  00 52 34.420  +03 44 23.65  23.2r 13SC112   W84  C~52RU      
2017 09  27.23363  00 52 34.417  +03 44 23.60  22.6i 13SC112   W84  C~52RU      
2017 09  27.23499  00 52 34.401  +03 44 23.62  23.9g 13SC112   W84  C~52RU      
2017 10  20.16907  00 50 49.233  +03 34 21.78  22.9z 13SC112   W84  C~52RU      
2018 10  18.19756  00 55 51.609  +04 21 06.15  22.7z 13SC112   W84  C~52RU      
2018 10  18.19894  00 55 51.612  +04 21 06.29  22.7i 13SC112   W84  C~52RU      
2018 11  26.07524  00 53 22.120  +04 07 53.67  24.6g 13SC112   W84  C~52RU      

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    -0.10       0.00     0.10
     2   0.0411      0.00     0.02       0.00     0.01
     3   0.1507      0.00    -0.07       0.00     0.09
     4   0.1780      0.00     0.05       0.00     0.02
     5   1.1251      0.00     0.07       0.00    -0.08
     6   1.1254      0.00     0.03       0.00    -0.15
     7   2.9491      0.00    -0.08       0.00    -0.11
     8   3.1129      0.00    -0.03       0.00     0.01
     9   3.1594      0.00     0.14       0.00     0.06
    10   3.1594      0.00     0.06       0.00    -0.26
    11   3.1677      0.00    -0.07       0.00     0.14
    12   3.9156      0.00     0.09       0.00    -0.01
    13   3.9156      0.00     0.01       0.00    -0.04
    14   3.9156      0.00     0.00       0.00     0.00
    15   3.9976      0.00     0.09       0.00     0.03
    16   3.9976      0.00     0.14       0.00     0.02
    17   3.9976      0.00    -0.01       0.00     0.08
    18   4.0604      0.00    -0.10       0.00     0.14
    19   5.0543      0.00    -0.13       0.00    -0.08
    20   5.0543      0.00     0.01       0.00     0.09
    21   5.1608      0.00    -0.01       0.00    -0.02

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.

13SC112    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        45.074    45.074    45.074
ecceobj         0.129     0.129     0.129
incobj          9.455     9.455     9.455
qmin           38.294    38.286    38.322
qmax           51.607    51.568    51.584
amean          44.800    44.799    44.800
amin           44.428    44.429    44.431
amax           45.208    45.226    45.201
emean           0.127     0.127     0.127
emin            0.113     0.113     0.113
emax            0.142     0.142     0.142
imean           8.935     8.935     8.935
imin            8.291     8.291     8.297
imax            9.530     9.528     9.527
excite_mean     0.201     0.201     0.201
fracstop        1.000     1.000     1.000
cjmean          3.062     3.062     3.062

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       175.9     176.2     175.9
kozaiamp        180.0     179.9     179.9