Orbit Fit and Astrometric record for 15KL199

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: 15KL199   
# Created Sun Nov 24 02:10:22 2024
# Orbit generated from Bernstein formalism
# Fitting     34 observations of     35
# Arc:   2.10y
# First observation: 2014/05/29
#  Last observation: 2016/07/05
Preliminary a, adot, b, bdot, g, gdot:
  -0.000019   0.024007   0.000000   0.000561   0.024086   0.000000
# Chi-squared of fit:    20.42 DOF:     62 RMS:  0.14
# Min/Max residuals:    -0.32    0.28
# Exact a, adot, b, bdot, g, gdot:
  1.544084E-05  2.407418E-02  4.745236E-07  5.632781E-04  2.438478E-02  2.681375E-05
# Covariance matrix:
  2.8270E-13 -3.8450E-13  6.1744E-16 -4.6783E-15 -1.6276E-13 -4.7942E-12
 -3.8450E-13  8.1409E-13 -1.8908E-15  1.2145E-14  3.9727E-13  1.2770E-11
  6.1744E-16 -1.8908E-15  1.8340E-13 -1.2053E-13  3.3951E-17 -3.0546E-14
 -4.6783E-15  1.2145E-14 -1.2053E-13  1.0406E-13  8.8917E-15  2.2499E-13
 -1.6276E-13  3.9727E-13  3.3951E-17  8.8917E-15  4.1528E-13  7.7527E-12
 -4.7942E-12  1.2770E-11 -3.0546E-14  2.2499E-13  7.7527E-12  2.3152E-10
#      lat0       lon0       xBary       yBary       zBary        JD0
    5.651986 -127.250723   -0.264102    0.096533   -0.974832  2456806.847808
# Heliocentric elements and errors
Epoch:              2456800.5000  =  2014/05/23
Mean Anomaly:           14.41383 +/-     0.906
Argument of Peri:       61.27800 +/-     0.980
Long of Asc Node:      156.35428 +/-     0.008
Inclination:             5.67027 +/-     0.000
Eccentricity:         0.03690507 +/-    0.0002
Semi-Major Axis:     43.53671536 +/-    0.0035
Time of Perihelion: 2452599.4407 +/-     264.2
Perihelion:          41.92998983 +/-    0.0087
Aphelion:            45.14344089 +/-    0.0088
Period (y)              287.2709 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -25.08639835 +/-    0.0006
Ecliptic Y          -33.42255664 +/-    0.0009
Ecliptic Z            4.03889979 +/-    0.0001
Ecliptic XDOT         0.00214825 +/-    0.0000
Ecliptic YDOT        -0.00163719 +/-    0.0000
Ecliptic ZDOT         0.00006336 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   41.98460892 +/-    0.0008
Geocenter to KBO     41.00918212 +/-    0.0011
# Hcoef:  8.61

The following table shows the complete astrometric record for 15KL199. 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 (15KL199) followed by the observatory code and reference code for the source of the astrometry.

2014 05  29.34703  15 27 16.109  -12 59 13.22  24.9r 15KL199   568  C~4n9s      
2014 05  29.38590  15 27 15.943  -12 59 12.61  25.0r 15KL199   568  C~4n9s      
2014 05  29.42474  15 27 15.721  -12 59 11.92  24.5r 15KL199   568  C~4n9s      
2014 05  30.45456  15 27 10.989  -12 58 56.21  24.8r 15KL199   568  C~4n9s      
2014 05  31.37090  15 27 06.833  -12 58 42.71  25.4r 15KL199   568  C~4n9s      
2015 02  20.65666  15 37 53.262  -13 43 21.33  24.8r 15KL199   568  C~4n9s      
2015 03  19.57074  15 37 31.674  -13 38 21.94  25.2r 15KL199   568  C~4n9s      
2015 04  12.48811  15 36 20.824  -13 31 39.52  24.5r 15KL199   568  C~4n9s      
2015 04  12.52910  15 36 20.641  -13 31 38.57  24.9r 15KL199   568  C~4n9s      
2015 05  17.38343  15 33 45.530  -13 20 53.57  24.4r 15KL199   568  C~4n9s      
2015 05  17.42514  15 33 45.314  -13 20 52.70  24.4r 15KL199   568  C~4n9s      
2015 05  17.46733  15 33 45.120  -13 20 52.23  24.8r 15KL199   568  C~4n9s      
2015 05  24.36910  15 33 12.187  -13 18 56.60  24.5r 15KL199   568  C~4n9s      
2015 05  24.41533  15 33 11.979  -13 18 55.87  24.6r 15KL199   568  C~4n9s      
2015 05  24.45620  15 33 11.746  -13 18 55.16  24.3r 15KL199   568  C~4n9s      
2015 05  26.44379  15 33 02.363  -13 18 23.68  24.5r 15KL199   568  C~4n9s      
2015 06  18.34328  15 31 21.923  -13 13 25.39  25.0r 15KL199   568  C~4n9s      
2015 06  18.38434  15 31 21.764  -13 13 24.86  24.7r 15KL199   568  C~4n9s      
2015 06  21.35896  15 31 10.343  -13 12 56.95  24.8r 15KL199   568  C~4n9s      
2015 07  10.39102  15 30 10.238  -13 11 06.58  24.1r 15KL199   568  C~4n9s      
2015 07  17.34619  15 29 54.858  -13 10 57.81  25.3r 15KL199   568  C~4n9s      
2015 07  18.31678  15 29 53.012  -13 10 58.00  24.8r 15KL199   568  C~4n9s      
2016 02  12.61062  15 43 10.994  -14 01 12.30  25.3w 15KL199   568  C~4n9s      
2016 03  15.61859  15 43 07.069  -13 56 26.56  25.2w 15KL199   568  C~4n9s      
2016 04  03.53855  15 42 20.937  -13 51 36.25  25.4w 15KL199   568  C~4n9s      
2016 04  03.54259  15 42 20.924  -13 51 36.36  25.6w 15KL199   568  C~4n9s      
2016 04  08.58811  15 42 04.054  -13 50 09.10  24.9w 15KL199   568  C~4n9s      
2016 04  08.59215  15 42 04.022  -13 50 08.90  25.1w 15KL199   568  C~4n9s      
2016 04  29.46970  15 40 39.105  -13 43 50.00        15KL199   568  C~4n9s      
2016 04  29.47374  15 40 39.116  -13 43 49.92  25.4w 15KL199   568  C~4n9s      
2016 05  04.40478  15 40 16.487  -13 42 19.78  24.8w 15KL199   568  C~4n9s      
2016 05  04.40882  15 40 16.479  -13 42 19.81  24.9w 15KL199   568  C~4n9s      
2016 07  04.28603  15 35 54.532  -13 29 24.51  24.8w 15KL199   568  C~4n9s      
2016 07  05.35431  15 35 51.353  -13 29 19.64        15KL199   568  C~4n9s      
2016 07  05.37863  15 35 51.327  -13 29 19.52  25.1w 15KL199   568  C~4n9s      

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     0.04       0.00    -0.02
     2   0.0001     -2.50     0.27      -0.01     0.05
     3   0.0002     -5.82    -0.32      -0.14    -0.00
     4   0.0030    -76.72    -0.23      -2.01     0.05
     5   0.0055   -138.92     0.22      -3.95    -0.08
     6   0.7319   9670.25     0.03    -319.76    -0.01
     7   0.8055   9292.85    -0.14    -103.19     0.23
     8   0.8710   8191.80     0.25      42.29     0.00
     9   0.8711   8188.98    -0.14      42.58     0.11
    10   0.9666   5834.65     0.01     126.70     0.00
    11   0.9667   5831.38    -0.20     126.78     0.10
    12   0.9668   5828.51     0.03     126.56    -0.11
    13   0.9857   5333.77     0.06     122.87     0.08
    14   0.9858   5330.64     0.28     122.84     0.12
    15   0.9859   5327.17    -0.24     122.71     0.04
    16   0.9914   5186.57    -0.04     120.19    -0.09
    17   1.0541   3690.89    -0.14      54.17    -0.17
    18   1.0542   3688.51    -0.09      54.12    -0.03
    19   1.0623   3519.90     0.12      40.62    -0.16
    20   1.1144   2641.53     0.08     -66.38    -0.26
    21   1.1335   2421.55     0.18    -112.79     0.02
    22   1.1361   2395.45    -0.02    -119.56     0.00
    23   1.7091  14435.80     0.17    -278.22     0.06
    24   1.7968  14313.50     0.03     -12.81     0.04
    25   1.8486  13589.48    -0.05     114.13     0.03
    26   1.8486  13589.32    -0.00     113.97    -0.15
    27   1.8624  13328.97     0.15     141.80     0.05
    28   1.8624  13328.47    -0.13     141.88     0.12
    29   1.9196  12032.25    -0.14     221.87    -0.14
    30   1.9196  12032.39     0.28     221.98    -0.04
    31   1.9331  11689.57    -0.24     232.40     0.14
    32   1.9331  11689.46    -0.06     232.34     0.08
    33   2.0998   7786.59     0.13      81.97    -0.12
    34   2.1027   7740.33    -0.17      75.63     0.08
    35   2.1028   7739.94 (   0.49)     75.65 (   0.26)

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.

15KL199    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        43.278    43.289    43.268
ecceobj         0.031     0.031     0.031
incobj          5.679     5.679     5.679
qmin           41.527    41.508    41.513
qmax           45.835    45.878    45.822
amean          43.601    43.612    43.591
amin           43.269    43.280    43.262
amax           43.939    43.951    43.937
emean           0.029     0.029     0.029
emin            0.013     0.013     0.013
emax            0.044     0.044     0.044
imean           5.273     5.270     5.276
imin            4.603     4.604     4.605
imax            5.974     5.969     5.978
excite_mean     0.097     0.097     0.097
fracstop        1.000     1.000     1.000
cjmean          3.086     3.086     3.086

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       176.6     176.8     176.8
kozaiamp        180.0     180.0     180.0