Orbit Fit and Astrometric record for 17EY59

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: 17EY59    
# Created Wed Nov 27 02:10:50 2024
# Orbit generated from Bernstein formalism
# Fitting     19 observations of     19
# Arc:  24.96d
# First observation: 2017/03/04
#  Last observation: 2017/03/29
Preliminary a, adot, b, bdot, g, gdot:
  -0.000001   0.030890   0.000001   0.001946   0.025890   0.000000
# WARNING Fitting with energy constraint
# Chi-squared of fit:    12.71 DOF:     33 RMS:  0.14
# Min/Max residuals:    -0.27    0.32
# Exact a, adot, b, bdot, g, gdot:
  1.563456E-05  2.551087E-02  1.404083E-06  2.288539E-03  2.503010E-02 -7.059909E-03
# Covariance matrix:
  6.5054E-13  5.3589E-10  5.6519E-14 -3.4117E-11  8.7729E-11 -4.3504E-09
  5.3589E-10  8.2840E-07  9.1251E-11 -5.2748E-08  1.3189E-07 -8.6522E-06
  5.6519E-14  9.1251E-11  2.6571E-13 -1.0406E-11  1.4412E-11 -1.0454E-09
 -3.4117E-11 -5.2748E-08 -1.0406E-11  3.4790E-09 -8.3876E-09  5.6021E-07
  8.7729E-11  1.3189E-07  1.4412E-11 -8.3876E-09  2.1068E-08 -1.3269E-06
 -4.3504E-09 -8.6522E-06 -1.0454E-09  5.6021E-07 -1.3269E-06  1.2991E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
   -8.627593  152.113107   -0.195890   -0.145412   -0.959333  2457816.953241
# Heliocentric elements and errors
Epoch:              2457810.5000  =  2017/02/26
Mean Anomaly:          318.47774 +/-    25.157
Argument of Peri:       14.24673 +/-    17.408
Long of Asc Node:      210.59810 +/-     1.237
Inclination:             9.88401 +/-     0.131
Eccentricity:         0.31043276 +/-    0.4837
Semi-Major Axis:     49.42548324 +/-   18.7060
Time of Perihelion: 2472449.2271 +/-    3098.4
Perihelion:          34.08219399 +/-   27.1634
Aphelion:            64.76877250 +/-   34.2396
Period (y)              347.4838 +/-    197.27
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -35.86554039 +/-    0.2024
Ecliptic Y           18.75093990 +/-    0.1072
Ecliptic Z           -5.99318089 +/-    0.0348
Ecliptic XDOT        -0.00066027 +/-    0.0011
Ecliptic YDOT        -0.00281257 +/-    0.0006
Ecliptic ZDOT         0.00036327 +/-    0.0002
# Distances at JD0 (AU)
Heliocenter to KBO   40.91274804 +/-    0.1842
Geocenter to KBO     39.95189502 +/-    0.2317
# Hcoef:  9.03

The following table shows the complete astrometric record for 17EY59. 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 (17EY59) followed by the observatory code and reference code for the source of the astrometry.

2017 03  04.45244  10 04 05.39   +02 39 16.2   24.7i 17EY59    T09  C~8HKl      
2017 03  04.47432  10 04 05.28   +02 39 16.9   25.0i 17EY59    T09  C~8HKl      
2017 03  04.49602  10 04 05.18   +02 39 17.6   24.9i 17EY59    T09  C~8HKl      
2017 03  06.50200  10 03 56.20   +02 40 16.8   25.5r 17EY59    T09  C~8HKl      
2017 03  06.51583  10 03 56.15   +02 40 17.3   25.1r 17EY59    T09  C~8HKl      
2017 03  06.52957  10 03 56.09   +02 40 17.4   25.3r 17EY59    T09  C~8HKl      
2017 03  22.43886  10 02 50.15   +02 48 11.3   24.9z 17EY59    T09  C~8HKl      
2017 03  22.46449  10 02 50.06   +02 48 11.6   24.7z 17EY59    T09  C~8HKl      
2017 03  22.48627  10 02 49.95   +02 48 12.5   24.1z 17EY59    T09  C~8HKl      
2017 03  23.24858  10 02 47.11   +02 48 35.2   25.0i 17EY59    T09  C~8HKl      
2017 03  23.25932  10 02 47.07   +02 48 35.3   24.7i 17EY59    T09  C~8HKl      
2017 03  23.27035  10 02 47.04   +02 48 35.7   25.0i 17EY59    T09  C~8HKl      
2017 03  25.23822  10 02 39.82   +02 49 33.3   25.2r 17EY59    T09  C~8Meo      
2017 03  25.25752  10 02 39.71   +02 49 34.0   25.5r 17EY59    T09  C~8Meo      
2017 03  25.28496  10 02 39.63   +02 49 34.7   25.1r 17EY59    T09  C~8Meo      
2017 03  25.29309  10 02 39.61   +02 49 34.7   26.0r 17EY59    T09  C~8Meo      
2017 03  29.28925  10 02 25.60   +02 51 30.5   25.6g 17EY59    T09  C~8HKl      
2017 03  29.39490  10 02 25.22   +02 51 33.3   24.4z 17EY59    T09  C~8HKl      
2017 03  29.41023  10 02 25.18   +02 51 33.7   24.5z 17EY59    T09  C~8HKl      

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     0.10       0.00     0.01
     2   0.0001     -1.79    -0.06       0.08     0.01
     3   0.0001     -3.44    -0.09       0.20     0.06
     4   0.0056   -150.22    -0.12       8.26    -0.03
     5   0.0056   -151.10     0.02       8.46     0.13
     6   0.0057   -151.97     0.16       8.24    -0.15
     7   0.0492  -1243.52    -0.03     104.25     0.11
     8   0.0493  -1244.89     0.25     104.06    -0.27
     9   0.0494  -1246.75    -0.21     104.32    -0.17
    10   0.0515  -1294.57    -0.22     110.60     0.11
    11   0.0515  -1295.16    -0.13     110.49    -0.08
    12   0.0515  -1295.72     0.02     110.70     0.05
    13   0.0569  -1417.25     0.32     126.58     0.14
    14   0.0570  -1419.04    -0.27     126.66     0.07
    15   0.0570  -1420.40     0.07     126.89     0.09
    16   0.0571  -1420.68     0.30     126.79    -0.08
    17   0.0680  -1657.91    -0.02     161.38     0.18
    18   0.0683  -1664.22    -0.15     162.00    -0.10
    19   0.0683  -1664.92     0.05     162.16    -0.07

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.