Orbit Fit and Astrometric record for 15GJ57

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: 15GJ57    
# Created Wed May  8 01:17:04 2024
# Orbit generated from Bernstein formalism
# Fitting     36 observations of     36
# Arc:   2.11y
# First observation: 2015/02/17
#  Last observation: 2017/03/29
Preliminary a, adot, b, bdot, g, gdot:
  -0.000124   0.022468   0.000002  -0.000290   0.023368   0.000000
# Chi-squared of fit:    12.64 DOF:     66 RMS:  0.10
# Min/Max residuals:    -0.37    0.29
# Exact a, adot, b, bdot, g, gdot:
  1.514935E-05  2.234469E-02 -6.150898E-08 -2.892525E-04  2.339735E-02  1.130608E-03
# Covariance matrix:
  1.8748E-13 -6.3844E-15 -4.7139E-16 -8.3337E-16  1.4618E-13  2.0653E-12
 -6.3844E-15  2.7766E-13 -1.2199E-16 -2.9246E-15  1.8006E-13  6.6036E-12
 -4.7139E-16 -1.2199E-16  9.2905E-14 -6.5609E-14 -6.3188E-16 -4.4905E-15
 -8.3337E-16 -2.9246E-15 -6.5609E-14  8.2133E-14 -2.6301E-15 -9.8706E-14
  1.4618E-13  1.8006E-13 -6.3188E-16 -2.6301E-15  2.7539E-13  6.1583E-12
  2.0653E-12  6.6036E-12 -4.4905E-15 -9.8706E-14  6.1583E-12  2.2303E-10
#      lat0       lon0       xBary       yBary       zBary        JD0
    1.130657 -154.059690    0.832842    0.010535   -0.526366  2457071.015468
# Heliocentric elements and errors
Epoch:              2457070.5000  =  2015/02/17
Mean Anomaly:           78.90809 +/-     0.091
Argument of Peri:       40.00550 +/-     0.150
Long of Asc Node:       82.08180 +/-     0.026
Inclination:             1.32766 +/-     0.000
Eccentricity:         0.03382182 +/-    0.0007
Semi-Major Axis:     43.51144673 +/-    0.0032
Time of Perihelion: 2434091.9427 +/-      26.4
Perihelion:          42.03981060 +/-    0.0291
Aphelion:            44.98308285 +/-    0.0291
Period (y)              287.0209 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -39.26684460 +/-    0.0009
Ecliptic Y          -18.17360575 +/-    0.0004
Ecliptic Z            0.84335336 +/-    0.0000
Ecliptic XDOT         0.00102055 +/-    0.0000
Ecliptic YDOT        -0.00241497 +/-    0.0000
Ecliptic ZDOT        -0.00003114 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   43.27674058 +/-    0.0008
Geocenter to KBO     42.73987776 +/-    0.0010
# Hcoef:  7.51

The following table shows the complete astrometric record for 15GJ57. 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 (15GJ57) followed by the observatory code and reference code for the source of the astrometry.

2015 02  17.51469  13 37 52.110  -08 58 00.76  23.6r 15GJ57    568  C~2nvV      
2015 02  17.55579  13 37 52.031  -08 58 00.30  24.1r 15GJ57    568  C~2nvV      
2015 02  20.48657  13 37 45.959  -08 57 21.42  24.7r 15GJ57    568  C~2nvV      
2015 03  18.49249  13 36 26.366  -08 49 16.07  23.6r 15GJ57    568  C~2nvV      
2015 03  18.53407  13 36 26.202  -08 49 15.08  23.4r 15GJ57    568  C~2nvV      
2015 03  20.53726  13 36 18.499  -08 48 29.24  23.4r 15GJ57    568  C~2nvV      
2015 04  11.47256  13 34 45.778  -08 39 25.51  23.4r 15GJ57    568  C~2nvV      
2015 04  12.37938  13 34 41.749  -08 39 01.97  24.1r 15GJ57    568  C~2nvV      
2015 04  12.42509  13 34 41.545  -08 39 00.72  24.2r 15GJ57    568  C~2nvV      
2015 04  12.46730  13 34 41.359  -08 38 59.71  24.2r 15GJ57    568  C~2nvV      
2015 04  18.43790  13 34 14.782  -08 36 26.37  24.0r 15GJ57    568  C~2nvV      
2015 04  18.48560  13 34 14.581  -08 36 25.39  24.0r 15GJ57    568  C~2nvV      
2015 05  16.28656  13 32 18.221  -08 25 25.88  23.8r 15GJ57    568  C~2nvV      
2015 05  17.24686  13 32 14.641  -08 25 06.03  23.8r 15GJ57    568  C~2nvV      
2015 05  25.38864  13 31 46.266  -08 22 29.95  23.6r 15GJ57    568  C~2nvV      
2015 05  25.44647  13 31 46.078  -08 22 28.91  23.4r 15GJ57    568  C~2nvV      
2015 07  12.28879  13 30 31.036  -08 16 28.39  24.4r 15GJ57    568  C~2nvV      
2015 07  15.27908  13 30 32.458  -08 16 42.68  23.6r 15GJ57    568  C~2nvV      
2016 02  04.61430  13 42 58.390  -09 28 35.66  24.4w 15GJ57    568  C~2nvV      
2016 02  11.59753  13 42 51.121  -09 27 44.18  24.3w 15GJ57    568  C~2nvV      
2016 03  11.60487  13 41 39.796  -09 20 24.73  24.5w 15GJ57    568  C~2nvV      
2016 04  03.47362  13 40 09.651  -09 11 36.97  23.6w 15GJ57    568  C~2nvV      
2016 04  09.45477  13 39 43.468  -09 09 06.22  23.8w 15GJ57    568  C~2nvV      
2016 05  01.46556  13 38 06.315  -08 59 54.81  24.0w 15GJ57    568  C~2nvV      
2016 05  02.33963  13 38 02.615  -08 59 34.00  24.6w 15GJ57    568  C~2nvV      
2016 05  07.34298  13 37 41.640  -08 57 36.91  23.9w 15GJ57    568  C~2nvV      
2016 05  29.32744  13 36 21.592  -08 50 18.55  24.1w 15GJ57    568  C~2nvV      
2016 06  04.38987  13 36 04.107  -08 48 46.10  24.2w 15GJ57    568  C~2nvV      
2016 06  27.32010  13 35 21.723  -08 45 17.87  23.9w 15GJ57    568  C~2nvV      
2016 06  27.32513  13 35 21.708  -08 45 17.84  23.9w 15GJ57    568  C~2nvV      
2016 07  07.31590  13 35 16.298  -08 45 04.33  23.5w 15GJ57    568  C~2nvV      
2017 02  24.65166  13 47 15.177  -09 53 24.40        15GJ57    568  C~2nvV      
2017 02  27.64150  13 47 07.812  -09 52 39.57        15GJ57    568  C~2nvV      
2017 02  27.66186  13 47 07.739  -09 52 39.03        15GJ57    568  C~2nvV      
2017 03  29.48748  13 45 24.370  -09 42 33.63  23.9w 15GJ57    568  C~2nvV      
2017 03  29.50900  13 45 24.284  -09 42 33.10  23.8w 15GJ57    568  C~2nvV      

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    -0.01       0.00    -0.03
     2   0.0001     -1.26     0.07       0.00    -0.05
     3   0.0081    -99.20    -0.07       3.66    -0.00
     4   0.0793  -1374.49    -0.00      28.26    -0.00
     5   0.0795  -1377.11    -0.05      28.30     0.03
     6   0.0849  -1500.15     0.05      29.56     0.04
     7   0.1450  -2978.63     0.01      36.26    -0.03
     8   0.1475  -3042.86    -0.21      36.43     0.11
     9   0.1476  -3046.14    -0.20      36.49     0.20
    10   0.1477  -3049.08    -0.10      36.43     0.15
    11   0.1641  -3472.10    -0.05      35.67     0.07
    12   0.1642  -3475.24     0.24      35.50    -0.07
    13   0.2403  -5323.88     0.29      19.53     0.05
    14   0.2429  -5380.61     0.02      18.59     0.01
    15   0.2652  -5829.92    -0.09       9.86    -0.02
    16   0.2654  -5832.90    -0.03       9.81     0.01
    17   0.3964  -7002.46    -0.06     -62.66     0.04
    18   0.4046  -6977.55     0.15     -68.22    -0.37
    19   0.9640   4892.28     0.08     -76.85    -0.05
    20   0.9831   4773.35     0.08     -67.39     0.08
    21   1.0625   3629.96    -0.04     -36.49    -0.13
    22   1.1251   2194.62     0.04     -24.79    -0.00
    23   1.1415   1778.59     0.05     -24.08     0.01
    24   1.2018    237.48    -0.14     -30.11    -0.01
    25   1.2042    178.84     0.19     -30.56     0.01
    26   1.2179   -153.24    -0.02     -33.96    -0.05
    27   1.2781  -1417.74     0.02     -55.65     0.03
    28   1.2947  -1692.81    -0.05     -63.63    -0.12
    29   1.3574  -2353.89     0.01     -98.02    -0.06
    30   1.3575  -2354.11    -0.13     -98.07    -0.11
    31   1.3848  -2433.74    -0.01    -114.66    -0.09
    32   2.0209   8975.23     0.04    -110.55     0.02
    33   2.0291   8857.34     0.09    -107.38     0.04
    34   2.0292   8856.14    -0.26    -107.26     0.14
    35   2.1108   7210.27     0.01     -86.41     0.04
    36   2.1109   7208.89     0.08     -86.37     0.08

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.

15GJ57    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        43.111    43.121    43.100
ecceobj         0.032     0.033     0.031
incobj          1.328     1.328     1.328
qmin           40.777    40.667    40.752
qmax           46.203    46.291    46.176
amean          43.384    43.394    43.373
amin           43.048    43.056    43.042
amax           43.729    43.753    43.715
emean           0.040     0.041     0.039
emin            0.021     0.022     0.020
emax            0.057     0.058     0.056
imean           0.866     0.863     0.868
imin            0.368     0.371     0.366
imax            1.282     1.278     1.286
excite_mean     0.043     0.044     0.042
fracstop        1.000     1.000     1.000
cjmean          3.092     3.092     3.092

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       164.9     164.9     164.6
kozaiamp        180.0     180.0     179.9