Orbit Fit and Astrometric record for 15GQ57

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: 15GQ57    
# Created Sun Nov 24 02:10:18 2024
# Orbit generated from Bernstein formalism
# Fitting     34 observations of     34
# Arc:   2.34y
# First observation: 2015/02/20
#  Last observation: 2017/06/25
Preliminary a, adot, b, bdot, g, gdot:
  -0.000094   0.024619   0.000001   0.000006   0.024306   0.000000
# Chi-squared of fit:     9.63 DOF:     62 RMS:  0.09
# Min/Max residuals:    -0.20    0.22
# Exact a, adot, b, bdot, g, gdot:
  1.583416E-05  2.447011E-02 -1.394940E-07  6.099205E-06  2.430686E-02 -1.489587E-03
# Covariance matrix:
  1.8027E-13 -5.7319E-15 -4.2536E-16  2.2288E-16  1.2359E-13  1.6088E-12
 -5.7319E-15  3.0224E-13 -6.7948E-16  6.3778E-16  1.8967E-13  7.4962E-12
 -4.2536E-16 -6.7948E-16  1.0097E-13 -6.5790E-14 -8.5107E-16 -2.0928E-14
  2.2288E-16  6.3778E-16 -6.5790E-14  7.4350E-14  5.9436E-16  2.0662E-14
  1.2359E-13  1.8967E-13 -8.5107E-16  5.9436E-16  2.4320E-13  5.8139E-12
  1.6088E-12  7.4962E-12 -2.0928E-14  2.0662E-14  5.8139E-12  2.4869E-10
#      lat0       lon0       xBary       yBary       zBary        JD0
    0.933148 -152.845518    0.815351    0.009160   -0.554124  2457074.098478
# Heliocentric elements and errors
Epoch:              2457070.5000  =  2015/02/17
Mean Anomaly:          319.10227 +/-     0.173
Argument of Peri:      138.04210 +/-     0.245
Long of Asc Node:      117.99490 +/-     0.040
Inclination:             0.92106 +/-     0.000
Eccentricity:         0.10951250 +/-    0.0005
Semi-Major Axis:     45.18258115 +/-    0.0057
Time of Perihelion: 2469672.8528 +/-      53.2
Perihelion:          40.23452381 +/-    0.0239
Aphelion:            50.13063849 +/-    0.0242
Period (y)              303.7140 +/-      0.06
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -37.46921170 +/-    0.0007
Ecliptic Y          -18.30118890 +/-    0.0004
Ecliptic Z            0.67000937 +/-    0.0000
Ecliptic XDOT         0.00140357 +/-    0.0000
Ecliptic YDOT        -0.00238147 +/-    0.0000
Ecliptic ZDOT        -0.00000195 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.70520654 +/-    0.0007
Geocenter to KBO     41.14065128 +/-    0.0008
# Hcoef:  8.35

The following table shows the complete astrometric record for 15GQ57. 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 (15GQ57) followed by the observatory code and reference code for the source of the astrometry.

2015 02  20.59770  13 42 10.154  -09 35 19.68  24.5r 15GQ57    568  C~2nvW      
2015 03  18.50144  13 40 50.708  -09 27 19.98  25.0r 15GQ57    568  C~2nvW      
2015 03  18.54235  13 40 50.557  -09 27 19.19  25.7r 15GQ57    568  C~2nvW      
2015 03  20.54594  13 40 42.735  -09 26 32.94  24.8r 15GQ57    568  C~2nvW      
2015 04  11.48071  13 39 07.904  -09 17 20.32  24.2r 15GQ57    568  C~2nvW      
2015 04  12.38760  13 39 03.764  -09 16 56.24  24.5r 15GQ57    568  C~2nvW      
2015 04  12.43323  13 39 03.533  -09 16 55.16  24.7r 15GQ57    568  C~2nvW      
2015 04  12.47547  13 39 03.338  -09 16 53.96  24.3r 15GQ57    568  C~2nvW      
2015 04  18.44608  13 38 35.977  -09 14 16.50  24.4r 15GQ57    568  C~2nvW      
2015 04  18.49382  13 38 35.741  -09 14 15.03  24.1r 15GQ57    568  C~2nvW      
2015 05  17.25497  13 36 31.288  -09 02 29.73  24.4r 15GQ57    568  C~2nvW      
2015 05  25.39688  13 36 01.615  -08 59 45.11  24.1r 15GQ57    568  C~2nvW      
2015 06  21.34643  13 34 53.883  -08 53 43.77  24.4r 15GQ57    568  C~2nvW      
2015 06  22.30309  13 34 52.501  -08 53 37.03  24.8r 15GQ57    568  C~2nvW      
2015 07  12.29701  13 34 41.186  -08 52 59.23  24.7r 15GQ57    568  C~2nvW      
2015 07  19.28682  13 34 45.508  -08 53 34.24  24.6r 15GQ57    568  C~2nvW      
2016 02  04.62644  13 47 51.849  -10 07 50.19  24.5w 15GQ57    568  C~2nvW      
2016 02  04.63139  13 47 51.824  -10 07 50.34  24.9w 15GQ57    568  C~2nvW      
2016 02  11.60966  13 47 45.417  -10 07 04.36  24.9w 15GQ57    568  C~2nvW      
2016 03  11.60894  13 46 35.278  -09 59 56.38  24.7w 15GQ57    568  C~2nvW      
2016 04  03.48576  13 45 03.455  -09 51 03.61  24.7w 15GQ57    568  C~2nvX      
2016 04  09.46692  13 44 36.529  -09 48 29.86  24.8w 15GQ57    568  C~2nvX      
2016 05  02.35585  13 42 52.081  -09 38 39.88  24.8w 15GQ57    568  C~2nvX      
2016 05  07.35921  13 42 30.252  -09 36 37.92  24.7w 15GQ57    568  C~2nvX      
2016 05  29.33148  13 41 06.379  -09 28 56.75  24.8w 15GQ57    568  C~2nvX      
2016 06  04.39391  13 40 47.899  -09 27 17.64  24.8w 15GQ57    568  C~2nvX      
2016 06  27.31561  13 40 02.457  -09 23 26.48  24.8w 15GQ57    568  C~2nvX      
2016 07  07.31185  13 39 56.152  -09 23 04.45  24.5w 15GQ57    568  C~2nvX      
2017 02  27.64549  13 52 35.844  -10 33 40.18        15GQ57    568  C~2nvX      
2017 03  30.51590  13 50 47.094  -10 23 10.64  24.2w 15GQ57    568  C~2nvX      
2017 03  31.45116  13 50 43.075  -10 22 47.75  24.6w 15GQ57    568  C~2nvX      
2017 05  24.25622  13 46 47.624  -10 01 02.95  24.5w 15GQ57    568  C~2nvX      
2017 06  25.27303  13 45 24.616  -09 53 51.72  24.6w 15GQ57    568  C~2nvX      
2017 06  25.28243  13 45 24.607  -09 53 51.95  24.9w 15GQ57    568  C~2nvX      

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     0.03
     2   0.0709  -1269.16    -0.15      25.26    -0.01
     3   0.0710  -1271.53     0.05      25.20    -0.09
     4   0.0765  -1396.17     0.09      26.69     0.00
     5   0.1366  -2904.68     0.16      36.27    -0.04
     6   0.1391  -2970.54     0.02      36.60     0.10
     7   0.1392  -2974.12    -0.19      36.37    -0.11
     8   0.1393  -2977.25    -0.20      36.45    -0.02
     9   0.1556  -3411.95     0.22      36.98     0.04
    10   0.1558  -3415.74    -0.03      37.09     0.17
    11   0.2345  -5390.06     0.00      27.35     0.04
    12   0.2568  -5859.78    -0.05      21.26     0.06
    13   0.3306  -6927.13    -0.08      -6.77    -0.01
    14   0.3332  -6948.68     0.06      -7.94    -0.03
    15   0.3880  -7118.83    -0.04     -33.75     0.04
    16   0.4071  -7046.34     0.08     -43.06     0.10
    17   0.9556   5414.52     0.05     -19.35     0.12
    18   0.9556   5414.23    -0.18     -19.62    -0.15
    19   0.9747   5309.39    -0.03     -10.22     0.05
    20   1.0541   4188.40     0.12      21.58    -0.02
    21   1.1167   2730.47     0.09      35.78     0.10
    22   1.1331   2303.78    -0.02      37.28    -0.07
    23   1.1958    650.62    -0.06      35.55    -0.19
    24   1.2095    305.53     0.03      33.63    -0.06
    25   1.2696  -1018.00     0.05      18.38    -0.04
    26   1.2862  -1308.78    -0.04      12.49    -0.08
    27   1.3490  -2019.39     0.09     -14.02    -0.09
    28   1.3764  -2114.38    -0.02     -27.10    -0.12
    29   2.0207   9888.85     0.09      10.97     0.03
    30   2.1052   8162.53    -0.07      35.27     0.03
    31   2.1077   8098.87    -0.02      35.76     0.09
    32   2.2551   4382.61     0.13      24.26    -0.02
    33   2.3427   3082.65    -0.17      -9.67     0.20
    34   2.3427   3082.61    -0.00      -9.94    -0.04

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.

15GQ57    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.742    44.754    44.730
ecceobj         0.105     0.106     0.104
incobj          0.921     0.921     0.921
qmin           39.623    39.586    39.642
qmax           50.813    50.977    50.714
amean          45.068    45.101    45.053
amin           44.696    44.710    44.688
amax           45.479    45.524    45.453
emean           0.103     0.104     0.102
emin            0.087     0.088     0.087
emax            0.118     0.120     0.116
imean           1.256     1.233     1.244
imin            0.576     0.564     0.563
imax            1.888     1.822     1.876
excite_mean     0.105     0.107     0.105
fracstop        1.000     1.000     1.000
cjmean          3.101     3.101     3.101

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       170.1     167.9     167.3
kozaiamp        179.9     180.0     180.0