Orbit Fit and Astrometric record for 20QH83

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: 20QH83    
# Created Fri Mar 13 01:12:09 2026
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     34 observations of     34
# Arc:   5.18y
# First observation: 2020/08/16
#  Last observation: 2025/10/22
# Chi-squared of fit:    16.94 DOF:     62 RMS:  0.12
# Min/Max residuals:    -0.41    0.54
# Exact a, adot, b, bdot, g, gdot:
  1.577883E-05  2.981470E-02  6.488078E-06  1.218778E-02  2.950504E-02 -7.698336E-03
# Covariance matrix:
  1.0747E-13 -6.8472E-14  1.0001E-14 -2.0912E-14  2.6489E-14 -3.7377E-13
 -6.8472E-14  1.1740E-13 -2.1829E-14  4.3268E-14  4.7479E-14  7.7127E-13
  1.0001E-14 -2.1829E-14  8.8652E-14 -4.1517E-14 -5.0832E-15 -1.8927E-13
 -2.0912E-14  4.3268E-14 -4.1517E-14  4.5843E-14  4.5080E-15  3.8275E-13
  2.6489E-14  4.7479E-14 -5.0832E-15  4.5080E-15  2.5783E-13  7.5201E-14
 -3.7377E-13  7.7127E-13 -1.8927E-13  3.8275E-13  7.5201E-14  6.8298E-12
#      lat0       lon0       xBary       yBary       zBary        JD0
   -3.651808  -47.681713   -0.196997   -0.062847   -0.982580  2459077.711691
# Heliocentric elements and errors
Epoch:              2459078.5000  =  2020/08/17
Mean Anomaly:          310.74331 +/-     0.008
Argument of Peri:       66.58016 +/-     0.013
Long of Asc Node:      321.27123 +/-     0.000
Inclination:            22.45098 +/-     0.000
Eccentricity:         0.25341747 +/-    0.0001
Semi-Major Axis:     39.57927117 +/-    0.0032
Time of Perihelion: 2471522.5815 +/-       9.8
Perihelion:          29.54919223 +/-    0.0040
Aphelion:            49.60935011 +/-    0.0052
Period (y)              249.0060 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           23.58635133 +/-    0.0004
Ecliptic Y          -25.61155028 +/-    0.0004
Ecliptic Z           -2.15843428 +/-    0.0000
Ecliptic XDOT         0.00162189 +/-    0.0000
Ecliptic YDOT         0.00234098 +/-    0.0000
Ecliptic ZDOT         0.00117391 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   34.88460641 +/-    0.0004
Geocenter to KBO     33.89268141 +/-    0.0006
# Hcoef:  7.57

The following table shows the complete astrometric record for 20QH83. 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 (20QH83) followed by the observatory code and reference code for the source of the astrometry.

2020 08  16.21089  21 03 29.78   -20 36 26.7   23.0R 20QH83    G37  C~4qof      
2020 08  16.23677  21 03 29.62   -20 36 27.2   22.6R 20QH83    G37  C~4qof      
2020 08  16.27702  21 03 29.38   -20 36 27.8   22.0R 20QH83    G37  C~4qof      
2020 08  16.29120  21 03 29.29   -20 36 28.0   22.3R 20QH83    G37  C~4qof      
2020 08  16.31867  21 03 29.13   -20 36 28.5   22.6R 20QH83    G37  C~4qof      
2020 09  20.11116  21 00 30.82   -20 42 48.1   22.2R 20QH83    G37  C~4qof      
2020 09  20.14420  21 00 30.69   -20 42 48.2   22.7R 20QH83    G37  C~4qof      
2020 09  20.16523  21 00 30.60   -20 42 48.3   23.3R 20QH83    G37  C~4qof      
2020 09  20.17927  21 00 30.54   -20 42 48.3   22.6R 20QH83    G37  C~4qof      
2020 09  20.19324  21 00 30.49   -20 42 48.4   22.9R 20QH83    G37  C~4qof      
2020 09  24.15293  21 00 15.62   -20 43 01.3         20QH83    G37  C~4qof      
2020 09  24.16003  21 00 15.58   -20 43 01.8         20QH83    G37  C~4qof      
2020 09  24.16672  21 00 15.56   -20 43 01.9         20QH83    G37  C~4qof      
2020 09  24.19183  21 00 15.46   -20 43 02.2         20QH83    G37  C~4qof      
2021 07  08.38678  21 13 24.49   -19 13 44.2   22.8R 20QH83    G37  C~4v6j      
2021 07  08.42792  21 13 24.29   -19 13 45.1   22.7R 20QH83    G37  C~4v6j      
2021 07  08.43503  21 13 24.22   -19 13 44.9   22.7R 20QH83    G37  C~4v6j      
2021 07  08.44361  21 13 24.21   -19 13 45.2   23.0R 20QH83    G37  C~4v6j      
2021 07  08.45071  21 13 24.18   -19 13 45.4   22.8R 20QH83    G37  C~4v6j      
2021 09  13.14456  21 07 09.64   -19 32 19.9   22.6R 20QH83    G37  C~52gG      
2021 09  13.18734  21 07 09.44   -19 32 20.3   22.5R 20QH83    G37  C~52gG      
2022 09  25.10290  21 12 27.63   -18 22 24.7         20QH83    G37  C~5tbg      
2022 09  25.11669  21 12 27.58   -18 22 25.0         20QH83    G37  C~5tbg      
2022 09  25.13022  21 12 27.52   -18 22 25.0         20QH83    G37  C~5tbg      
2022 09  25.14403  21 12 27.47   -18 22 25.1         20QH83    G37  C~5tbg      
2022 09  25.17490  21 12 27.35   -18 22 25.3         20QH83    G37  C~5tbg      
2022 09  30.10951  21 12 09.72   -18 22 51.3         20QH83    G37  C~5tbg      
2022 09  30.11546  21 12 09.71   -18 22 51.5         20QH83    G37  C~5tbg      
2022 09  30.12153  21 12 09.68   -18 22 51.2         20QH83    G37  C~5tbg      
2022 09  30.12748  21 12 09.67   -18 22 51.3         20QH83    G37  C~5tbg      
2022 09  30.13345  21 12 09.65   -18 22 51.3         20QH83    G37  C~5tbg      
2022 09  30.13939  21 12 09.62   -18 22 51.3         20QH83    G37  C~5tbg      
2025 10  22.14822  21 29 30.45   -14 40 31.2         20QH83    G37  C~9DI5      
2025 10  22.18363  21 29 30.39   -14 40 31.2         20QH83    G37  C~9DI5      

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     0.04       0.00     0.02
     2   0.0001      0.00    -0.03       0.00    -0.05
     3   0.0002      0.00     0.01       0.00     0.00
     4   0.0002      0.00    -0.06       0.00     0.03
     5   0.0003      0.00     0.01       0.00    -0.03
     6   0.0956      0.00    -0.06       0.00    -0.07
     7   0.0956      0.00    -0.02       0.00    -0.03
     8   0.0957      0.00    -0.09       0.00    -0.03
     9   0.0957      0.00    -0.14       0.00     0.03
    10   0.0958      0.00    -0.05       0.00    -0.01
    11   0.1066      0.00     0.17       0.00     0.54
    12   0.1066      0.00    -0.04       0.00     0.06
    13   0.1067      0.00     0.03       0.00    -0.02
    14   0.1067      0.00    -0.09       0.00    -0.26
    15   0.8930      0.00    -0.08       0.00     0.04
    16   0.8931      0.00     0.09       0.00    -0.13
    17   0.8932      0.00    -0.41       0.00     0.19
    18   0.8932      0.00     0.10       0.00     0.04
    19   0.8932      0.00     0.20       0.00    -0.03
    20   1.0758      0.00    -0.02       0.00    -0.08
    21   1.0759      0.00     0.02       0.00    -0.08
    22   2.1078      0.00     0.01       0.00     0.19
    23   2.1079      0.00     0.06       0.00    -0.02
    24   2.1079      0.00    -0.05       0.00     0.07
    25   2.1080      0.00     0.01       0.00     0.06
    26   2.1080      0.00     0.01       0.00     0.06
    27   2.1216      0.00    -0.06       0.00    -0.16
    28   2.1216      0.00     0.10       0.00    -0.34
    29   2.1216      0.00    -0.04       0.00    -0.01
    30   2.1216      0.00     0.12       0.00    -0.09
    31   2.1216      0.00     0.12       0.00    -0.06
    32   2.1216      0.00    -0.02       0.00    -0.04
    33   5.1826      0.00    -0.02       0.00     0.08
    34   5.1827      0.00    -0.10       0.00     0.06

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.

20QH83    quality flag:3

Type:           3:2E      3:2E      3:2E

axisobj        39.239    39.238    39.239
ecceobj         0.254     0.254     0.254
incobj         22.503    22.503    22.503
qmin           27.827    28.135    28.214
qmax           51.893    51.590    51.569
amean          39.455    39.455    39.455
amin           38.876    38.889    38.882
amax           40.121    40.119    40.128
emean           0.267     0.263     0.259
emin            0.238     0.238     0.236
emax            0.297     0.289     0.287
imean          23.064    23.247    23.569
imin           21.970    22.571    22.583
imax           24.122    24.122    24.355
excite_mean     0.474     0.475     0.476
fracstop        1.000     1.000     1.000
cjmean          2.792     2.791     2.789

libcent 0       177.9     180.7     181.6
libamp  0       150.8     152.6     150.6
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       188.3     188.3     179.0
kozaiamp        180.0     179.9     179.9