Orbit Fit and Astrometric record for 14PS70

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: 14PS70    
# Created Fri Nov 22 02:09:57 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     37 observations of     37
# Arc:   9.08y
# First observation: 2013/09/03
#  Last observation: 2022/10/02
# Chi-squared of fit:    22.52 DOF:     68 RMS:  0.14
# Min/Max residuals:    -0.36    0.32
# Exact a, adot, b, bdot, g, gdot:
  1.675642E-05  2.560873E-02  2.581435E-06  6.941989E-03  2.595609E-02  1.110984E-03
# Covariance matrix:
  2.0512E-13 -1.1046E-13  3.0760E-14 -2.4907E-14 -1.1103E-13 -3.9330E-13
 -1.1046E-13  8.5132E-14 -2.6038E-14  2.1097E-14  1.1073E-13  3.3286E-13
  3.0760E-14 -2.6038E-14  1.0255E-13 -2.3710E-14 -3.2599E-14 -1.0904E-13
 -2.4907E-14  2.1097E-14 -2.3710E-14  1.0789E-14  2.6631E-14  8.8309E-14
 -1.1103E-13  1.1073E-13 -3.2599E-14  2.6631E-14  4.1005E-13  4.1562E-13
 -3.9330E-13  3.3286E-13 -1.0904E-13  8.8309E-14  4.1562E-13  1.3941E-12
#      lat0       lon0       xBary       yBary       zBary        JD0
    0.737106  -10.039319    0.161469    0.012868   -0.996695  2456538.924748
# Heliocentric elements and errors
Epoch:              2456538.5000  =  2013/09/03
Mean Anomaly:           35.64208 +/-     0.051
Argument of Peri:      322.94875 +/-     0.059
Long of Asc Node:      347.08478 +/-     0.000
Inclination:            15.20094 +/-     0.000
Eccentricity:         0.05850866 +/-    0.0001
Semi-Major Axis:     41.44159290 +/-    0.0038
Time of Perihelion: 2446891.0261 +/-      14.0
Perihelion:          39.01690091 +/-    0.0041
Aphelion:            43.86628488 +/-    0.0045
Period (y)              266.7859 +/-      0.04
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           38.88679448 +/-    0.0009
Ecliptic Y           -7.04519969 +/-    0.0002
Ecliptic Z            0.49575896 +/-    0.0000
Ecliptic XDOT         0.00057081 +/-    0.0000
Ecliptic YDOT         0.00263996 +/-    0.0000
Ecliptic ZDOT         0.00073383 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   39.52292555 +/-    0.0009
Geocenter to KBO     38.52662274 +/-    0.0010
# Hcoef:  6.76

The following table shows the complete astrometric record for 14PS70. 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 (14PS70) followed by the observatory code and reference code for the source of the astrometry.

2013 09  03.42397  23 21 56.245  -03 17 53.66  22.4w 14PS70    F51  C~3jRY      
2013 09  03.43887  23 21 56.204  -03 17 54.20  22.4w 14PS70    F51  C~3jRY      
2013 09  03.45376  23 21 56.133  -03 17 54.66  22.5w 14PS70    F51  C~3jRY      
2013 09  03.46865  23 21 56.062  -03 17 54.95  22.5w 14PS70    F51  C~3jRY      
2014 08  03.54729  23 28 53.362  -02 10 02.56  22.6w 14PS70    F51  C~1vXh      
2014 08  03.55858  23 28 53.318  -02 10 02.95  22.6w 14PS70    F51  C~1vXh      
2014 08  03.56990  23 28 53.276  -02 10 02.87  22.7w 14PS70    F51  C~1vXh      
2014 08  22.47315  23 27 38.253  -02 16 26.86  22.3w 14PS70    F51  C~1vXh      
2014 08  22.48541  23 27 38.204  -02 16 26.77  22.8w 14PS70    F51  C~1vXh      
2014 08  22.49768  23 27 38.144  -02 16 27.25  22.6w 14PS70    F51  C~1vXh      
2014 08  22.50997  23 27 38.084  -02 16 27.52  22.2w 14PS70    F51  C~1vXh      
2014 09  19.33076  23 25 26.947  -02 28 23.18  22.5w 14PS70    F51  C~1vXh      
2014 09  19.34220  23 25 26.912  -02 28 23.76  22.7w 14PS70    F51  C~1vXh      
2014 09  19.36508  23 25 26.811  -02 28 24.25  22.7w 14PS70    F51  C~1vXh      
2016 09  05.35046  23 36 00.44   -00 29 49.3   22.5i 14PS70    T09  C~7bJS      
2016 09  05.36940  23 36 00.35   -00 29 49.9   22.4i 14PS70    T09  C~7bJS      
2016 09  05.38564  23 36 00.26   -00 29 49.9   22.9i 14PS70    T09  C~7bJS      
2016 09  05.40188  23 36 00.20   -00 29 50.4   22.6i 14PS70    T09  C~7bJS      
2016 09  07.36512  23 35 50.90   -00 30 41.2   23.8r 14PS70    T09  C~7bJS      
2016 09  07.46935  23 35 50.40   -00 30 44.2   24.2r 14PS70    T09  C~7bJS      
2016 09  07.47153  23 35 50.38   -00 30 43.9   23.8r 14PS70    T09  C~7bJS      
2016 09  30.092512 23 34 02.45   -00 40 49.9   22.8r 14PS70    W84  C~352P      
2016 09  30.093889 23 34 02.44   -00 40 49.9   22.7i 14PS70    W84  C~352P      
2016 09  30.095266 23 34 02.44   -00 40 50.0   24.0g 14PS70    W84  C~352P      
2016 09  30.130729 23 34 02.26   -00 40 50.9   22.4z 14PS70    W84  C~352P      
2016 10  05.148032 23 33 39.32   -00 43 02.9   22.4i 14PS70    W84  C~352P      
2016 10  05.149410 23 33 39.32   -00 43 02.8   22.7r 14PS70    W84  C~352P      
2016 10  05.150787 23 33 39.32   -00 43 02.9   23.2g 14PS70    W84  C~352P      
2016 11  05.052789 23 31 44.00   -00 54 16.8   22.3z 14PS70    W84  C~352P      
2019 10  26.098590 23 46 22.766  +01 56 18.13  22.7G 14PS70    G37  C~3cmw      
2019 10  26.165530 23 46 22.519  +01 56 16.54        14PS70    G37  C~3cmw      
2021 08  08.354400 00 01 26.349  +04 17 56.22  23.0G 14PS70    G37  C~4xRv      
2021 08  08.403110 00 01 26.180  +04 17 55.69        14PS70    G37  C~4xRv      
2021 08  08.448770 00 01 26.043  +04 17 55.04        14PS70    G37  C~4xRv      
2022 10  02.434881 00 02 12.150  +04 53 09.18  22.5w 14PS70    F51  C~5qzK      
2022 10  02.446057 00 02 12.086  +04 53 08.72  22.6w 14PS70    F51  C~5qzK      
2022 10  02.457458 00 02 12.019  +04 53 08.77  22.7w 14PS70    F51  C~5qzK      

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    -0.35       0.00     0.22
     2   0.0000      0.00     0.12       0.00     0.07
     3   0.0001      0.00     0.14       0.00    -0.01
     4   0.0001      0.00     0.16       0.00     0.09
     5   0.9148      0.00     0.11       0.00     0.12
     6   0.9148      0.00     0.05       0.00    -0.08
     7   0.9148      0.00     0.02       0.00     0.19
     8   0.9666      0.00    -0.12       0.00    -0.36
     9   0.9666      0.00    -0.03       0.00     0.02
    10   0.9667      0.00    -0.10       0.00    -0.18
    11   0.9667      0.00    -0.18       0.00    -0.16
    12   1.0429      0.00    -0.15       0.00     0.04
    13   1.0429      0.00     0.16       0.00    -0.23
    14   1.0430      0.00     0.32       0.00    -0.11
    15   3.0060      0.00    -0.05       0.00    -0.06
    16   3.0060      0.00    -0.03       0.00    -0.17
    17   3.0061      0.00    -0.21       0.00     0.25
    18   3.0061      0.00     0.06       0.00     0.17
    19   3.0115      0.00     0.09       0.00     0.16
    20   3.0118      0.00     0.16       0.00    -0.12
    21   3.0118      0.00     0.02       0.00     0.23
    22   3.0737      0.00     0.00       0.00    -0.03
    23   3.0737      0.00    -0.05       0.00     0.01
    24   3.0737      0.00     0.05       0.00    -0.06
    25   3.0738      0.00    -0.14       0.00    -0.01
    26   3.0875      0.00    -0.08       0.00    -0.09
    27   3.0875      0.00     0.01       0.00     0.04
    28   3.0875      0.00     0.11       0.00    -0.02
    29   3.1722      0.00     0.05       0.00     0.25
    30   6.1428      0.00    -0.05       0.00    -0.03
    31   6.1430      0.00     0.05       0.00    -0.07
    32   7.9286      0.00     0.07       0.00     0.06
    33   7.9288      0.00    -0.09       0.00     0.11
    34   7.9289      0.00     0.07       0.00     0.01
    35   9.0787      0.00     0.14       0.00    -0.09
    36   9.0788      0.00    -0.01       0.00    -0.24
    37   9.0788      0.00    -0.19       0.00     0.13

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.

14PS70    quality flag:3

Type:       SCATEXTD  SCATEXTD  SCATEXTD

axisobj        41.644    41.644    41.644
ecceobj         0.063     0.063     0.063
incobj         15.156    15.156    15.156
qmin           38.257    38.239    38.282
qmax           44.984    44.984    44.997
amean          41.514    41.514    41.514
amin           41.202    41.202    41.203
amax           41.840    41.840    41.840
emean           0.061     0.061     0.061
emin            0.048     0.048     0.048
emax            0.075     0.075     0.076
imean          15.553    15.553    15.553
imin           14.816    14.815    14.817
imax           16.261    16.262    16.261
excite_mean     0.275     0.275     0.275
fracstop        1.000     1.000     1.000
cjmean          2.983     2.983     2.983

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       176.3     176.3     176.1
kozaiamp        180.0     180.0     180.0