Orbit Fit and Astrometric record for 22OH10

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: 22OH10    
# Created Fri Nov 22 02:11:15 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     65 observations of     65
# Arc:  15.28y
# First observation: 2009/05/31
#  Last observation: 2024/09/10
# Chi-squared of fit:    30.73 DOF:    124 RMS:  0.12
# Min/Max residuals:    -0.37    0.40
# Exact a, adot, b, bdot, g, gdot:
  2.127968E-05  7.617210E-02  8.139757E-06  2.669384E-02  5.628942E-02 -2.101629E-02
# Covariance matrix:
  1.8833E-08 -1.2401E-05  7.0718E-09 -4.6511E-06 -1.1089E-12  4.9151E-07
 -1.2401E-05  1.7323E-02 -4.6568E-06  6.4961E-03  7.2714E-10 -6.8663E-04
  7.0718E-09 -4.6568E-06  2.6563E-09 -1.7466E-06 -4.1639E-13  1.8457E-07
 -4.6511E-06  6.4961E-03 -1.7466E-06  2.4391E-03  2.7272E-10 -2.5752E-04
 -1.1089E-12  7.2714E-10 -4.1639E-13  2.7272E-10  6.5291E-17 -2.8819E-11
  4.9151E-07 -6.8663E-04  1.8457E-07 -2.5752E-04 -2.8819E-11  2.7219E-05
#      lat0       lon0       xBary       yBary       zBary        JD0
  -11.120026 -130.834406   -0.354954   -0.182655   -0.929087  2454982.901971
# Heliocentric elements and errors
Epoch:              2454982.5000  =  2009/05/31
Mean Anomaly:          293.31979 +/-     0.000
Argument of Peri:       64.59512 +/-     0.000
Long of Asc Node:      257.59001 +/-     0.000
Inclination:            22.11293 +/-     0.000
Eccentricity:         0.23600622 +/-    0.0001
Semi-Major Axis:     19.49963720 +/-    0.0000
Time of Perihelion: 2460807.9932 +/-       0.0
Perihelion:          14.89760160 +/-    0.0025
Aphelion:            24.10167279 +/-    0.0025
Period (y)               86.1089 +/-      0.00
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -11.74561412 +/-    0.0000
Ecliptic Y          -14.14169093 +/-    0.0000
Ecliptic Z           -3.42611648 +/-    0.0000
Ecliptic XDOT         0.00330012 +/-    0.0000
Ecliptic YDOT        -0.00184895 +/-    0.0000
Ecliptic ZDOT         0.00147103 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   18.69996640 +/-    0.0000
Geocenter to KBO     17.76546365 +/-    0.0000
# Hcoef: 10.40

The following table shows the complete astrometric record for 22OH10. 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 (22OH10) followed by the observatory code and reference code for the source of the astrometry.

2009 05  31.401205 14 53 09.81   -28 10 51.7   23.0z 22OH10    568  C~5j3j      
2009 05  31.404347 14 53 09.78   -28 10 51.4   22.5i 22OH10    568  C~5j3j      
2011 06  07.385817 15 35 25.772  -27 17 10.41  22.3G 22OH10    F51  C~5j3j      
2011 06  07.400059 15 35 25.625  -27 17 09.90  22.6G 22OH10    F51  C~5j3j      
2011 06  07.414263 15 35 25.463  -27 17 08.88  22.8G 22OH10    F51  C~5j3j      
2011 06  07.428415 15 35 25.318  -27 17 08.13  23.0G 22OH10    F51  C~5j3j      
2013 06  30.324004 16 17 15.723  -25 11 58.67  21.8G 22OH10    F51  C~5j3j      
2013 06  30.351753 16 17 15.440  -25 11 56.83  22.9G 22OH10    F51  C~5j3j      
2013 06  30.365670 16 17 15.322  -25 11 56.40  23.0G 22OH10    F51  C~5j3j      
2014 05  21.446941 16 48 29.942  -24 24 49.27  23.2G 22OH10    F51  C~5j3j      
2014 05  21.460017 16 48 29.793  -24 24 48.82  22.5G 22OH10    F51  C~5j3j      
2014 05  21.473128 16 48 29.640  -24 24 48.34  22.4G 22OH10    F51  C~5j3j      
2014 05  21.486179 16 48 29.487  -24 24 47.91  23.6G 22OH10    F51  C~5j3j      
2014 06  28.339415 16 41 13.129  -23 58 13.64  22.5G 22OH10    F51  C~5j3j      
2014 06  28.349999 16 41 13.017  -23 58 13.30  22.4G 22OH10    F51  C~5j3j      
2014 06  28.360586 16 41 12.904  -23 58 12.75  22.3G 22OH10    F51  C~5j3j      
2014 06  28.371167 16 41 12.793  -23 58 12.26  22.0G 22OH10    F51  C~5j3j      
2014 07  17.102785 16 38 23.86   -23 45 12.2         22OH10    W84  C~5j3j      
2015 07  09.354527 17 03 27.031  -22 18 42.59  22.3G 22OH10    F51  C~5j3j      
2015 07  09.366342 17 03 26.888  -22 18 42.14  22.9G 22OH10    F51  C~5j3j      
2015 07  09.378241 17 03 26.753  -22 18 41.51  22.5G 22OH10    F51  C~5j3j      
2015 07  09.390024 17 03 26.654  -22 18 41.31  22.7G 22OH10    F51  C~5j3j      
2015 07  12.357405 17 02 58.183  -22 17 00.60  23.7G 22OH10    F51  C~5j3j      
2015 07  12.369173 17 02 58.072  -22 17 00.05  22.3G 22OH10    F51  C~5j3j      
2015 07  12.380981 17 02 57.962  -22 16 59.58  22.9G 22OH10    F51  C~5j3j      
2021 07  16.095363 19 32 42.25   -07 05 16.9   22.0i 22OH10    W84  C~5j3j      
2022 06  06.472694 20 05 15.749  -03 57 46.70  22.2G 22OH10    F52  C~5j3j      
2022 06  06.484114 20 05 15.660  -03 57 46.13  22.4G 22OH10    F52  C~5j3j      
2022 06  06.495548 20 05 15.578  -03 57 45.57  22.6G 22OH10    F52  C~5j3j      
2022 06  06.506969 20 05 15.477  -03 57 44.95  22.4G 22OH10    F52  C~5j3j      
2022 06  06.577873 20 05 14.953  -03 57 41.76  22.1G 22OH10    F52  C~5j3j      
2022 06  06.578502 20 05 14.956  -03 57 41.79  22.2G 22OH10    F52  C~5j3j      
2022 06  24.509971 20 02 36.479  -03 47 37.56  22.2G 22OH10    F52  C~5j3j      
2022 06  24.522847 20 02 36.347  -03 47 37.17  22.4G 22OH10    F52  C~5j3j      
2022 06  24.535724 20 02 36.197  -03 47 37.13  22.6G 22OH10    F52  C~5j3j      
2022 06  29.458500 20 01 44.346  -03 46 09.28  22.1G 22OH10    F52  C~5j3j      
2022 06  29.469974 20 01 44.205  -03 46 08.95  21.9G 22OH10    F52  C~5j3j      
2022 06  29.493014 20 01 43.994  -03 46 08.66  22.1G 22OH10    F52  C~5j3j      
2022 06  29.548620 20 01 43.353  -03 46 07.90  22.3G 22OH10    F52  C~5j3j      
2022 06  29.549257 20 01 43.343  -03 46 07.75  22.8G 22OH10    F52  C~5j3j      
2022 07  29.342185 19 55 54.966  -03 48 46.42  22.2w 22OH10    F52  C~5j3j      
2022 07  29.354292 19 55 54.814  -03 48 46.92  22.4w 22OH10    F52  C~5j3j      
2022 07  29.366388 19 55 54.662  -03 48 47.01  21.8w 22OH10    F52  C~5j3j      
2022 08  01.265358 19 55 20.675  -03 49 59.64  22.1G 22OH10    568  C~5j3j      
2022 08  01.266567 19 55 20.658  -03 49 59.67  22.1G 22OH10    568  C~5j3j      
2022 08  01.267785 19 55 20.647  -03 49 59.70  22.2G 22OH10    568  C~5j3j      
2022 08  05.380184 19 54 33.299  -03 51 57.27  21.9G 22OH10    568  C~5j3j      
2022 08  05.381159 19 54 33.288  -03 51 57.30  21.9G 22OH10    568  C~5j3j      
2022 08  05.382143 19 54 33.278  -03 51 57.31  21.9G 22OH10    568  C~5j3j      
2023 09  05.245935 20 15 19.539  -00 50 07.76  22.2w 22OH10    F52  C~79Nx      
2023 09  05.257426 20 15 19.449  -00 50 08.45  22.0w 22OH10    F52  C~79Ny      
2023 09  05.280378 20 15 19.268  -00 50 09.88  22.2w 22OH10    F52  C~79Ny      
2023 09  13.251572 20 14 22.581  -00 58 06.88  21.8w 22OH10    F52  C~7Bnx      
2023 09  13.261216 20 14 22.500  -00 58 07.24  22.1w 22OH10    F52  C~7Bnx      
2023 09  13.270793 20 14 22.427  -00 58 07.86  22.4w 22OH10    F52  C~7Bnx      
2024 07  01.531010 20 53 00.412  +03 07 12.67  21.9w 22OH10    F51  C~873H      
2024 07  01.543852 20 53 00.300  +03 07 13.08  22.1w 22OH10    F51  C~873H      
2024 07  01.556745 20 53 00.162  +03 07 13.25  21.9w 22OH10    F51  C~873H      
2024 07  01.569669 20 53 00.045  +03 07 13.81  22.1w 22OH10    F51  C~873H      
2024 08  03.459867 20 46 57.586  +03 05 02.04  21.9w 22OH10    F51  C~8AkO      
2024 08  03.469186 20 46 57.481  +03 05 02.10  21.9w 22OH10    F51  C~8AkO      
2024 08  03.478444 20 46 57.377  +03 05 01.83  21.8w 22OH10    F51  C~8AkO      
2024 09  10.304277 20 40 22.370  +02 31 09.22  21.9w 22OH10    F52  C~8G18      
2024 09  10.312949 20 40 22.296  +02 31 08.68  22.0w 22OH10    F52  C~8G18      
2024 09  10.321622 20 40 22.243  +02 31 08.09  22.2w 22OH10    F52  C~8G18      

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    -0.02       0.00    -0.13
     2   0.0000      0.00    -0.00       0.00    -0.05
     3   2.0178      0.00     0.03       0.00     0.32
     4   2.0178      0.00     0.10       0.00    -0.03
     5   2.0178      0.00    -0.07       0.00     0.12
     6   2.0179      0.00     0.02       0.00     0.01
     7   4.0819      0.00     0.13       0.00    -0.19
     8   4.0820      0.00    -0.18       0.00     0.27
     9   4.0820      0.00     0.02       0.00     0.01
    10   4.9721      0.00    -0.07       0.00    -0.15
    11   4.9721      0.00    -0.01       0.00    -0.20
    12   4.9721      0.00    -0.01       0.00    -0.22
    13   4.9722      0.00    -0.01       0.00    -0.29
    14   5.0758      0.00    -0.05       0.00     0.04
    15   5.0758      0.00    -0.04       0.00    -0.07
    16   5.0759      0.00    -0.05       0.00     0.02
    17   5.0759      0.00    -0.03       0.00     0.06
    18   5.1272      0.00     0.10       0.00     0.07
    19   6.1053      0.00     0.40       0.00    -0.01
    20   6.1053      0.00     0.04       0.00     0.03
    21   6.1053      0.00    -0.19       0.00     0.25
    22   6.1054      0.00     0.10       0.00     0.05
    23   6.1135      0.00    -0.05       0.00    -0.09
    24   6.1135      0.00    -0.02       0.00     0.06
    25   6.1136      0.00     0.03       0.00     0.13
    26  12.1251      0.00    -0.02       0.00    -0.02
    27  13.0159      0.00     0.07       0.00    -0.12
    28  13.0160      0.00     0.01       0.00    -0.08
    29  13.0160      0.00     0.06       0.00    -0.04
    30  13.0160      0.00    -0.18       0.00     0.05
    31  13.0162      0.00    -0.08       0.00    -0.01
    32  13.0162      0.00     0.04       0.00    -0.07
    33  13.0653      0.00     0.00       0.00    -0.01
    34  13.0654      0.00     0.05       0.00     0.10
    35  13.0654      0.00    -0.18       0.00    -0.13
    36  13.0789      0.00    -0.08       0.00    -0.20
    37  13.0789      0.00    -0.29       0.00    -0.03
    38  13.0790      0.00     0.37       0.00    -0.07
    39  13.0791      0.00    -0.01       0.00    -0.11
    40  13.0791      0.00    -0.06       0.00     0.03
    41  13.1607      0.00     0.15       0.00     0.21
    42  13.1607      0.00     0.05       0.00    -0.00
    43  13.1608      0.00    -0.04       0.00     0.19
    44  13.1687      0.00    -0.03       0.00     0.05
    45  13.1687      0.00    -0.07       0.00     0.05
    46  13.1687      0.00    -0.02       0.00     0.05
    47  13.1800      0.00     0.01       0.00     0.01
    48  13.1800      0.00     0.02       0.00     0.01
    49  13.1800      0.00     0.04       0.00     0.03
    50  14.2638      0.00    -0.00       0.00     0.01
    51  14.2638      0.00     0.05       0.00    -0.00
    52  14.2639      0.00     0.13       0.00    -0.09
    53  14.2857      0.00     0.16       0.00    -0.19
    54  14.2857      0.00    -0.11       0.00     0.04
    55  14.2857      0.00    -0.27       0.00     0.00
    56  15.0859      0.00    -0.05       0.00     0.01
    57  15.0859      0.00     0.11       0.00     0.10
    58  15.0860      0.00    -0.10       0.00    -0.05
    59  15.0860      0.00    -0.00       0.00     0.19
    60  15.1761      0.00    -0.10       0.00    -0.37
    61  15.1761      0.00     0.01       0.00    -0.02
    62  15.1761      0.00     0.13       0.00     0.00
    63  15.2797      0.00    -0.03       0.00     0.05
    64  15.2797      0.00    -0.08       0.00     0.11
    65  15.2797      0.00     0.19       0.00     0.12

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.

22OH10    quality flag:3

Type:       CENTAURR  CENTAURR  CENTAURR

axisobj        19.381    19.381    19.382
ecceobj         0.236     0.236     0.236
incobj         22.154    22.154    22.154
qmin           14.485    14.485    14.484
qmax           24.062    24.062    24.062
amean          19.218    19.218    19.218
amin           18.884    18.884    18.884
amax           19.478    19.478    19.476
emean           0.229     0.228     0.229
emin            0.217     0.217     0.218
emax            0.238     0.238     0.238
imean          24.092    24.101    24.085
imin           23.469    23.469    23.469
imax           24.653    24.673    24.642
excite_mean     0.468     0.468     0.468
fracstop        0.002     0.002     0.002
cjmean          2.991     2.991     2.991

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        67.8      67.8      67.8
kozaiamp          6.9       6.9       6.9