Orbit Fit and Astrometric record for 10HG109

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: 10HG109   
# Created Sat Apr 27 01:13:20 2024
# Orbit generated from Bernstein formalism
# Fitting      6 observations of      6
# Arc:  48.82d
# First observation: 2010/04/21
#  Last observation: 2010/06/09
# WARNING Fitting with energy constraint
# WARNING and with gdot fixed = 0
# Chi-squared of fit:     1.62 DOF:      8 RMS:  0.09
# Min/Max residuals:    -0.20    0.16
# Exact a, adot, b, bdot, g, gdot:
  1.516435E-05  3.083788E-02 -1.001737E-05 -2.071463E-02  3.270791E-02  0.000000E+00
# Covariance matrix:
  9.1628E-11  1.9042E-07  4.8448E-13 -2.0424E-10  3.1554E-08  0.0000E+00
  1.9042E-07  3.9785E-04  1.0122E-09 -4.2672E-07  6.5925E-05  0.0000E+00
  4.8448E-13  1.0122E-09  4.8998E-13 -4.7389E-12  1.6773E-10  0.0000E+00
 -2.0424E-10 -4.2672E-07 -4.7389E-12  5.1275E-10 -7.0710E-08  0.0000E+00
  3.1554E-08  6.5925E-05  1.6773E-10 -7.0710E-08  1.0924E-05  0.0000E+00
  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  4.6045E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
   -2.153736 -127.745982    0.370585   -0.035214   -0.935873  2455307.749526
# Heliocentric elements and errors
Epoch:              2455300.5000  =  2010/04/14
Mean Anomaly:          337.72115 +/-   313.098
Argument of Peri:      207.37913 +/-    20.230
Long of Asc Node:       48.48714 +/-     2.055
Inclination:            33.99960 +/-    17.107
Eccentricity:         0.03110513 +/-    0.6057
Semi-Major Axis:     32.44029922 +/-   17.1565
Time of Perihelion: 2459477.0342 +/-  193642.7
Perihelion:          31.43123946 +/-   25.7375
Aphelion:            33.44935897 +/-   26.4394
Period (y)              184.7717 +/-    146.58
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -19.56474710 +/-    1.8901
Ecliptic Y          -24.67475038 +/-    2.4411
Ecliptic Z           -1.14928451 +/-    0.1161
Ecliptic XDOT         0.00208293 +/-    0.0016
Ecliptic YDOT        -0.00152273 +/-    0.0017
Ecliptic ZDOT        -0.00173276 +/-    0.0002
# Distances at JD0 (AU)
Heliocenter to KBO   31.51100586 +/-    2.2430
Geocenter to KBO     30.57364086 +/-    3.0895
# Hcoef:  7.21

The following table shows the complete astrometric record for 10HG109. 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 (10HG109) followed by the observatory code and reference code for the source of the astrometry.

2010 04  21.24876  15 17 00.715  -20 24 48.62  21.9R 10HG109   304  C~0Jan      
2010 04  21.29638  15 17 00.406  -20 24 48.05  22.0R 10HG109   304  C~0Jan      
2010 04  21.39268  15 16 59.790  -20 24 47.21  21.9R 10HG109   304  C~0Jan      
2010 06  09.01768  15 11 35.653  -20 13 43.67  21.6R 10HG109   807  C~0Jan      
2010 06  09.04240  15 11 35.495  -20 13 43.24        10HG109   807  C~0Jan      
2010 06  09.06569  15 11 35.336  -20 13 42.93        10HG109   807  C~0Jan      

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     0.00
     2   0.0001     -4.34    -0.06      -0.58     0.07
     3   0.0004    -12.92     0.11      -2.02    -0.07
     4   0.1335  -4586.66     0.16    -564.86    -0.03
     5   0.1336  -4588.92     0.03    -565.04     0.05
     6   0.1337  -4591.16    -0.20    -565.34    -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.

10HG109    quality flag:0

Type:      ERR2LARGE ERR2LARGE ERR2LARGE

axisobj         0.000     0.000     0.000
ecceobj        -1.000    -1.000    -1.000
incobj         -1.000    -1.000    -1.000
qmin            0.000     0.000     0.000
qmax            0.000     0.000     0.000
amean           0.000     0.000     0.000
amin            0.000     0.000     0.000
amax            0.000     0.000     0.000
emean           0.000     0.000     0.000
emin            0.000     0.000     0.000
emax            0.000     0.000     0.000
imean           0.000     0.000     0.000
imin            0.000     0.000     0.000
imax            0.000     0.000     0.000
excite_mean     0.000     0.000     0.000
fracstop        0.000     0.000     0.000
cjmean          0.000     0.000     0.000

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         0.0       0.0       0.0
kozaiamp          0.0       0.0       0.0