Orbit Fit and Astrometric record for 00CK105

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: 00CK105   
# Created Sun Dec 22 02:08:06 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     35 observations of     35
# Arc:  23.04y
# First observation: 2000/02/06
#  Last observation: 2023/02/20
# Chi-squared of fit:    86.69 DOF:     64 RMS:  0.28
# Min/Max residuals:    -0.80    0.59
# Exact a, adot, b, bdot, g, gdot:
  1.352041E-05  1.652699E-02 -3.039034E-06 -2.282600E-03  2.106168E-02  6.055086E-04
# Covariance matrix:
  1.3279E-13 -2.4875E-14 -5.2544E-15  2.6623E-15  5.8874E-14 -5.3880E-14
 -2.4875E-14  9.2923E-15  2.4364E-15 -1.1898E-15 -9.9177E-15  2.3957E-14
 -5.2544E-15  2.4364E-15  8.3400E-14 -5.6751E-15 -1.0792E-15  6.8010E-15
  2.6623E-15 -1.1898E-15 -5.6751E-15  8.4570E-16  1.1356E-15 -3.3132E-15
  5.8874E-14 -9.9177E-15 -1.0792E-15  1.1356E-15  2.4093E-13 -2.4579E-14
 -5.3880E-14  2.3957E-14  6.8010E-15 -3.3132E-15 -2.4579E-14  6.6690E-14
#      lat0       lon0       xBary       yBary       zBary        JD0
    2.131200  131.636154   -0.095696    0.036398   -0.983788  2451580.780463
# Heliocentric elements and errors
Epoch:              2451580.5000  =  2000/02/06
Mean Anomaly:          167.40964 +/-     0.018
Argument of Peri:      353.17586 +/-     0.004
Long of Asc Node:      326.49925 +/-     0.000
Inclination:             8.14463 +/-     0.000
Eccentricity:         0.23245715 +/-    0.0001
Semi-Major Axis:     39.43888785 +/-    0.0027
Time of Perihelion: 2409511.3844 +/-       6.2
Perihelion:          30.27103624 +/-    0.0030
Aphelion:            48.60673946 +/-    0.0040
Period (y)              247.6824 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -32.24265942 +/-    0.0007
Ecliptic Y           36.13551970 +/-    0.0008
Ecliptic Z            1.76553033 +/-    0.0000
Ecliptic XDOT        -0.00167092 +/-    0.0000
Ecliptic YDOT        -0.00135321 +/-    0.0000
Ecliptic ZDOT        -0.00029348 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   48.46111358 +/-    0.0008
Geocenter to KBO     47.47960559 +/-    0.0011
# Hcoef:  6.27

The following table shows the complete astrometric record for 00CK105. 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 (00CK105) followed by the observatory code and reference code for the source of the astrometry.

2000 02  06.27972  08 58 53.00   +19 20 30.7   22.7R 00CK105   695  Cb1115      
2000 02  06.40899  08 58 52.40   +19 20 32.7         00CK105   695  Cb1115      
2000 02  26.16705  08 57 26.66   +19 25 44.4   23.0R 00CK105   695  Cb1115      
2000 02  26.25132  08 57 26.32   +19 25 45.6         00CK105   695  Cb1115      
2001 02  03.32739  09 02 44.38   +18 56 16.3         00CK105   568  Cc6636      
2001 02  03.34939  09 02 44.28   +18 56 16.4         00CK105   568  Cc6636      
2001 02  04.41973  09 02 39.45   +18 56 34.9         00CK105   568  Cc6636      
2001 02  04.44081  09 02 39.33   +18 56 35.5         00CK105   568  Cc6636      
2001 03  13.04359  09 00 09.80   +19 05 37.8   22.7  00CK105   304  Ce8743      
2001 03  13.06549  09 00 09.77   +19 05 38.2         00CK105   304  Ce8743      
2001 04  26.26970  08 58 51.75   +19 08 23.7   23.2R 00CK105   568  Cd0809      
2001 04  27.25118  08 58 51.77   +19 08 19.4         00CK105   568  Cd0809      
2001 04  27.36001  08 58 51.78   +19 08 18.9         00CK105   568  Cd0809      
2002 02  04.49351  09 06 20.75   +18 32 40.8   22.2R 00CK105   568  Cf1711      
2002 02  05.44656  09 06 16.48   +18 32 57.9         00CK105   568  Cf1711      
2002 02  05.50379  09 06 16.23   +18 32 59.0         00CK105   568  Cf1711      
2005 02  04.223221 09 17 15.77   +17 19 36.5   22.8V 00CK105   645  C~1S6l      
2005 02  04.224050 09 17 15.77   +17 19 36.6   22.7V 00CK105   645  C~1S6l      
2005 02  04.226538 09 17 15.76   +17 19 36.6   24.6V 00CK105   645  C~1S6l      
2005 02  09.20385  09 16 53.60   +17 21 10.0   22.9R 00CK105   688  Cm6694      
2005 02  09.32529  09 16 53.07   +17 21 12.4         00CK105   688  Cm6694      
2006 12  21.37570  09 27 15.97   +16 16 57.8   22.8R 00CK105   695  Ct5419      
2006 12  21.51592  09 27 15.63   +16 16 59.9         00CK105   695  Ct5419      
2013 03  13.18565  09 42 57.97   +14 07 36.1   23.0R 00CK105   695  C~0uco      
2013 03  14.17857  09 42 54.29   +14 07 53.1         00CK105   695  C~0uco      
2013 03  14.26612  09 42 53.97   +14 07 54.9         00CK105   695  C~0uco      
2016 01  11.302737 09 57 32.63   +12 27 28.7         00CK105   W84  C~3i9V      
2016 01  11.303773 09 57 32.65   +12 27 29.0         00CK105   W84  C~3i9V      
2016 01  11.305006 09 57 32.64   +12 27 29.1         00CK105   W84  C~3i9V      
2016 01  11.306076 09 57 32.63   +12 27 29.0         00CK105   W84  C~3i9V      
2017 03  03.044994 09 57 32.57   +12 17 37.6         00CK105   W84  C~3i9V      
2017 03  03.046487 09 57 32.57   +12 17 37.7         00CK105   W84  C~3i9V      
2023 02  20.277870 10 18 56.119  +09 27 19.26  23.0G 00CK105   G37  C~6EkO      
2023 02  20.329820 10 18 55.882  +09 27 20.40        00CK105   G37  C~6EkO      
2023 02  20.382790 10 18 55.649  +09 27 21.22        00CK105   G37  C~6EkO      

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    -0.15       0.00     0.33
     2   0.0004      0.00    -0.26       0.00     0.13
     3   0.0544      0.00    -0.21       0.00     0.15
     4   0.0547      0.00    -0.10       0.00     0.16
     5   0.9940      0.00     0.08       0.00    -0.20
     6   0.9940      0.00     0.09       0.00    -0.49
     7   0.9970      0.00     0.14       0.00    -0.80
     8   0.9970      0.00    -0.21       0.00    -0.57
     9   1.0972      0.00    -0.61       0.00     0.06
    10   1.0973      0.00     0.06       0.00     0.22
    11   1.2183      0.00     0.44       0.00     0.59
    12   1.2210      0.00     0.24       0.00     0.21
    13   1.2213      0.00     0.36       0.00     0.19
    14   1.9965      0.00    -0.04       0.00     0.11
    15   1.9991      0.00     0.09       0.00     0.19
    16   1.9992      0.00     0.26       0.00     0.28
    17   4.9964      0.00     0.20       0.00    -0.46
    18   4.9964      0.00     0.26       0.00    -0.38
    19   4.9964      0.00     0.28       0.00    -0.43
    20   5.0101      0.00    -0.53       0.00    -0.11
    21   5.0104      0.00    -0.29       0.00     0.02
    22   6.8723      0.00    -0.43       0.00     0.02
    23   6.8727      0.00     0.12       0.00     0.38
    24  13.0976      0.00     0.00       0.00    -0.04
    25  13.1003      0.00    -0.24       0.00     0.07
    26  13.1006      0.00    -0.14       0.00     0.39
    27  15.9289      0.00    -0.11       0.00    -0.21
    28  15.9289      0.00     0.24       0.00     0.08
    29  15.9289      0.00     0.16       0.00     0.16
    30  15.9289      0.00     0.06       0.00     0.04
    31  17.0699      0.00     0.14       0.00     0.17
    32  17.0699      0.00     0.23       0.00     0.24
    33  23.0390      0.00     0.07       0.00     0.01
    34  23.0392      0.00    -0.13       0.00    -0.03
    35  23.0393      0.00    -0.21       0.00    -0.41

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.

00CK105    quality flag:3

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

axisobj        39.430    39.430    39.430
ecceobj         0.233     0.233     0.233
incobj          8.146     8.146     8.146
qmin           28.201    28.202    28.201
qmax           51.293    51.294    51.292
amean          39.455    39.455    39.455
amin           39.118    39.117    39.118
amax           39.908    39.908    39.907
emean           0.229     0.229     0.229
emin            0.180     0.180     0.180
emax            0.285     0.285     0.285
imean           9.677     9.677     9.677
imin            5.240     5.240     5.239
imax           12.050    12.050    12.050
excite_mean     0.286     0.286     0.286
fracstop        1.000     1.000     1.000
cjmean          2.958     2.958     2.958

libcent 0       179.8     179.8     179.8
libamp  0        20.0      20.1      20.0
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       208.0     208.0     208.0
kozaiamp        180.0     180.0     180.0