Orbit Fit and Astrometric record for 16EW391

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: 16EW391   
# Created Wed Nov 27 02:10:35 2024
# Orbit generated from Bernstein formalism
# Fitting     17 observations of     17
# Arc:   8.04d
# First observation: 2016/03/04
#  Last observation: 2016/03/12
Preliminary a, adot, b, bdot, g, gdot:
  -0.000000   0.025688   0.000001   0.001015   0.023723   0.000000
# WARNING MRQMIN stopped after  13 iterations -- oscilliatory solution
# WARNING Fitting with energy constraint
# Chi-squared of fit:     6.53 DOF:     29 RMS:  0.11
# Min/Max residuals:    -0.22    0.39
# Exact a, adot, b, bdot, g, gdot:
  1.501832E-05  2.193089E-02  1.377586E-06  1.379973E-03  2.308257E-02 -1.615176E-03
# Covariance matrix:
  6.5320E-12  8.8838E-09 -4.1453E-13 -8.5444E-10  1.5601E-09 -4.7976E-08
  8.8838E-09  1.2420E-05 -5.7621E-10 -1.1941E-06  2.1756E-06 -7.5739E-05
 -4.1453E-13 -5.7621E-10  1.7360E-13  4.7572E-11 -1.0120E-10  2.8755E-09
 -8.5444E-10 -1.1941E-06  4.7572E-11  1.1583E-07 -2.0911E-07  7.4319E-06
  1.5601E-09  2.1756E-06 -1.0120E-10 -2.0911E-07  3.8144E-07 -1.2448E-05
 -4.7976E-08 -7.5739E-05  2.8755E-09  7.4319E-06 -1.2448E-05  2.4671E-03
#      lat0       lon0       xBary       yBary       zBary        JD0
  -10.842829  140.133788   -0.396885   -0.170166   -0.889335  2457451.844529
# Heliocentric elements and errors
Epoch:              2457450.5000  =  2016/03/03
Mean Anomaly:          294.65480 +/-   272.175
Argument of Peri:        1.82301 +/-   109.754
Long of Asc Node:      211.39199 +/-     6.431
Inclination:            11.23601 +/-     0.435
Eccentricity:         0.07009260 +/-    2.2469
Semi-Major Axis:     45.35023916 +/-   22.4227
Time of Perihelion: 2477698.3531 +/-   82988.5
Perihelion:          42.17152315 +/-  104.0094
Aphelion:            48.52895518 +/-  104.6848
Period (y)              305.4060 +/-    226.50
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -33.61201066 +/-    0.8738
Ecliptic Y           27.54741787 +/-    0.7298
Ecliptic Z           -8.14962872 +/-    0.2180
Ecliptic XDOT        -0.00154677 +/-    0.0043
Ecliptic YDOT        -0.00210442 +/-    0.0038
Ecliptic ZDOT         0.00019681 +/-    0.0011
# Distances at JD0 (AU)
Heliocenter to KBO   44.21587882 +/-    0.8059
Geocenter to KBO     43.32274138 +/-    1.1592
# Hcoef:  8.04

The following table shows the complete astrometric record for 16EW391. 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 (16EW391) followed by the observatory code and reference code for the source of the astrometry.

2016 03  04.34374  09 16 29.89   +04 27 49.7   24.0i 16EW391   T09  C~8HEj      
2016 03  04.34717  09 16 29.88   +04 27 49.9   24.3i 16EW391   T09  C~8HEj      
2016 03  04.35871  09 16 29.84   +04 27 50.2   24.4i 16EW391   T09  C~8HEj      
2016 03  04.36703  09 16 29.79   +04 27 50.2   24.0i 16EW391   T09  C~8HEj      
2016 03  04.37528  09 16 29.76   +04 27 50.6   24.3i 16EW391   T09  C~8HEj      
2016 03  04.38892  09 16 29.71   +04 27 51.1   24.1i 16EW391   T09  C~8HEj      
2016 03  04.40242  09 16 29.66   +04 27 51.4   24.0i 16EW391   T09  C~8HEj      
2016 03  04.41331  09 16 29.62   +04 27 51.6   24.3i 16EW391   T09  C~8HEj      
2016 03  07.35383  09 16 18.32   +04 29 08.2   25.3g 16EW391   T09  C~8HEj      
2016 03  07.35667  09 16 18.31   +04 29 08.3   25.2g 16EW391   T09  C~8HEj      
2016 03  07.37512  09 16 18.23   +04 29 08.7   25.2g 16EW391   T09  C~8HEj      
2016 03  07.40643  09 16 18.12   +04 29 09.7   25.1g 16EW391   T09  C~8HEj      
2016 03  12.30861  09 16 00.22   +04 31 17.6   24.4z 16EW391   T09  C~8HEj      
2016 03  12.31203  09 16 00.21   +04 31 17.6   24.0z 16EW391   T09  C~8HEj      
2016 03  12.32378  09 16 00.16   +04 31 18.1   24.2z 16EW391   T09  C~8HEj      
2016 03  12.35418  09 16 00.09   +04 31 18.8   24.2z 16EW391   T09  C~8HEj      
2016 03  12.37925  09 15 59.97   +04 31 19.6   24.2z 16EW391   T09  C~8HEj      

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     0.00       0.00    -0.09
     2   0.0000     -0.20     0.02       0.14     0.03
     3   0.0000     -0.86     0.11       0.25     0.06
     4   0.0001     -1.58    -0.07       0.02    -0.22
     5   0.0001     -2.13    -0.08       0.26    -0.03
     6   0.0001     -2.99    -0.06       0.51     0.13
     7   0.0002     -3.79     0.01       0.57     0.10
     8   0.0002     -4.43     0.08       0.57     0.03
     9   0.0082   -188.75     0.02      21.75    -0.02
    10   0.0082   -188.92     0.03      21.80     0.01
    11   0.0083   -190.18    -0.07      21.81    -0.11
    12   0.0084   -192.05     0.02      22.26     0.11
    13   0.0218   -486.03    -0.09      62.08    -0.07
    14   0.0218   -486.17    -0.03      62.03    -0.14
    15   0.0218   -487.04    -0.20      62.28     0.01
    16   0.0219   -488.25     0.39      62.63     0.10
    17   0.0220   -490.20    -0.08      62.84     0.10

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.