Orbit Fit and Astrometric record for 14UV228

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: 14UV228   
# Created Fri Nov 22 02:10:06 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     50 observations of     50
# Arc:  11.21y
# First observation: 2004/09/21
#  Last observation: 2015/12/07
# Chi-squared of fit:    61.70 DOF:     94 RMS:  0.20
# Min/Max residuals:    -0.61    0.85
# Exact a, adot, b, bdot, g, gdot:
  1.888945E-05  4.171086E-02  1.989724E-06  7.452730E-03  3.374561E-02  1.996390E-03
# Covariance matrix:
  4.0631E-13 -1.7889E-13  3.3406E-14 -2.7917E-14 -9.2119E-14 -3.3138E-13
 -1.7889E-13  1.4647E-13 -3.1143E-14  2.6041E-14  9.7874E-14  3.0868E-13
  3.3406E-14 -3.1143E-14  2.4640E-13 -3.1083E-14 -2.0906E-14 -6.7084E-14
 -2.7917E-14  2.6041E-14 -3.1083E-14  7.8391E-15  1.7569E-14  5.6088E-14
 -9.2119E-14  9.7874E-14 -2.0906E-14  1.7569E-14  1.3348E-13  2.0573E-13
 -3.3138E-13  3.0868E-13 -6.7084E-14  5.6088E-14  2.0573E-13  6.6503E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
    0.318520    6.742812    0.142035    0.005626   -0.997995  2453269.914053
# Heliocentric elements and errors
Epoch:              2453270.5000  =  2004/09/22
Mean Anomaly:            8.13881 +/-     0.004
Argument of Peri:      348.59867 +/-     0.006
Long of Asc Node:        4.75970 +/-     0.000
Inclination:            10.15693 +/-     0.000
Eccentricity:         0.22477758 +/-    0.0000
Semi-Major Axis:     39.31823346 +/-    0.0018
Time of Perihelion: 2451234.6397 +/-       0.9
Perihelion:          30.48037622 +/-    0.0017
Aphelion:            48.15609069 +/-    0.0024
Period (y)              246.5467 +/-      0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           30.43159939 +/-    0.0003
Ecliptic Y            3.45700778 +/-    0.0000
Ecliptic Z            0.16481365 +/-    0.0000
Ecliptic XDOT        -0.00024146 +/-    0.0000
Ecliptic YDOT         0.00337223 +/-    0.0000
Ecliptic ZDOT         0.00060565 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   30.62774567 +/-    0.0003
Geocenter to KBO     29.63349740 +/-    0.0003
# Hcoef:  8.56

The following table shows the complete astrometric record for 14UV228. 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 (14UV228) followed by the observatory code and reference code for the source of the astrometry.

2004 09  21.41331  00 24 15.550  +02 58 10.10  23.6r 14UV228   568  C~2SDh      
2004 09  21.44443  00 24 15.35   +02 58 09.2   23.4r 14UV228   568  C~2SDh      
2004 09  21.47327  00 24 15.19   +02 58 07.9   23.6r 14UV228   568  C~2SDh      
2004 09  22.41821  00 24 09.59   +02 57 36.8   23.1r 14UV228   568  C~2SDh      
2005 10  04.24293  00 31 05.92   +04 10 56.6   23.2R 14UV228   675  C~2SDh      
2005 10  04.32035  00 31 05.44   +04 10 54.0         14UV228   675  C~2SDh      
2005 10  04.37171  00 31 05.14   +04 10 52.3         14UV228   675  C~2SDh      
2005 11  05.18175  00 28 10.13   +03 54 14.3         14UV228   695  C~2SDh      
2005 11  05.22530  00 28 09.90   +03 54 13.3         14UV228   695  C~2SDh      
2006 09  26.30155  00 40 00.360  +05 34 48.10        14UV228   696  C~2SDh      
2006 09  26.33853  00 40 00.14   +05 34 47.0         14UV228   696  C~2SDh      
2006 09  26.37552  00 39 59.92   +05 34 45.7         14UV228   696  C~2SDh      
2013 08  09.50685  01 39 39.673  +14 28 21.32  23.4r 14UV228   568  C~2SDh      
2013 08  09.55027  01 39 39.621  +14 28 21.38  23.6r 14UV228   568  C~2SDh      
2013 09  02.42521  01 38 38.765  +14 26 57.64  23.4r 14UV228   568  C~2SDh      
2013 09  02.46835  01 38 38.586  +14 26 57.14  23.4r 14UV228   568  C~2SDh      
2013 09  03.44432  01 38 34.854  +14 26 45.83  23.2r 14UV228   568  C~2SDh      
2013 09  03.49095  01 38 34.658  +14 26 45.27  23.5r 14UV228   568  C~2SDh      
2013 10  08.50533  01 35 34.372  +14 14 22.05  23.5r 14UV228   568  C~2SDh      
2013 10  30.49811  01 33 20.411  +14 03 04.15  23.6r 14UV228   568  C~2SDh      
2013 11  01.50035  01 33 08.484  +14 02 00.43  23.5r 14UV228   568  C~2SDh      
2013 11  28.28696  01 30 49.347  +13 48 41.63  23.6r 14UV228   568  C~2SDh      
2013 12  04.39432  01 30 25.275  +13 46 09.91  23.6r 14UV228   568  C~2SDh      
2013 12  05.28909  01 30 22.057  +13 45 49.17  23.5r 14UV228   568  C~2SDh      
2013 12  29.25967  01 29 28.701  +13 39 16.11  23.4r 14UV228   568  C~2SDh      
2013 12  30.36406  01 29 27.876  +13 39 06.64  23.5r 14UV228   568  C~2SDh      
2014 01  02.24156  01 29 26.487  +13 38 45.94  23.5r 14UV228   568  C~2SDh      
2014 01  02.28865  01 29 26.467  +13 38 45.61  23.3r 14UV228   568  C~2SDh      
2014 01  02.37231  01 29 26.428  +13 38 45.14  23.4r 14UV228   568  C~2SDh      
2014 01  03.25404  01 29 26.249  +13 38 39.99  23.1r 14UV228   568  C~2SDh      
2014 07  26.53369  01 47 40.830  +15 33 07.56  23.7r 14UV228   568  C~2SDh      
2014 07  26.57688  01 47 40.852  +15 33 08.37  23.8r 14UV228   568  C~2SDh      
2014 08  24.47423  01 47 12.037  +15 36 17.35  23.7r 14UV228   568  C~2SDh      
2014 08  24.54416  01 47 11.847  +15 36 17.11  23.7r 14UV228   568  C~2SDh      
2014 08  30.44951  01 46 54.308  +15 35 46.60  23.7r 14UV228   568  C~2SDh      
2014 08  30.55611  01 46 53.939  +15 35 45.94  23.6r 14UV228   568  C~2SDh      
2014 09  18.47464  01 45 35.276  +15 31 41.35  23.5r 14UV228   568  C~2SDh      
2014 09  18.51737  01 45 35.055  +15 31 40.56  23.6r 14UV228   568  C~2SDh      
2014 09  23.51567  01 45 09.472  +15 30 02.08  23.7r 14UV228   568  C~2SDh      
2014 10  22.29873  01 42 20.163  +15 17 17.38  23.4r 14UV228   568  C~2SDh      
2014 10  22.34444  01 42 19.872  +15 17 16.04  23.6r 14UV228   568  C~2SDh      
2014 10  22.38820  01 42 19.596  +15 17 14.73  23.4r 14UV228   568  C~2SDh      
2014 10  25.50246  01 42 00.395  +15 15 38.57  23.5r 14UV228   568  C~2SDh      
2014 11  20.23375  01 39 32.698  +15 02 19.97  23.4r 14UV228   568  C~2SDh      
2014 11  20.37417  01 39 31.976  +15 02 15.93  23.4r 14UV228   568  C~2SDh      
2014 11  21.27833  01 39 27.428  +15 01 49.47  23.6r 14UV228   568  C~2SDh      
2014 11  21.43358  01 39 26.628  +15 01 44.83  23.6r 14UV228   568  C~2SDh      
2015 10  12.48210  01 51 30.954  +16 30 02.60        14UV228   568  C~2SDh      
2015 10  12.54868  01 51 30.546  +16 30 00.86        14UV228   568  C~2SDh      
2015 12  07.40375  01 46 21.032  +16 02 43.02  23.7w 14UV228   568  C~2SDh      

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     0.34
     2   0.0001      0.00    -0.18       0.00     0.48
     3   0.0002      0.00     0.04       0.00     0.15
     4   0.0028      0.00     0.12       0.00     0.85
     5   1.0344      0.00    -0.34       0.00    -0.61
     6   1.0347      0.00    -0.46       0.00    -0.58
     7   1.0348      0.00    -0.26       0.00    -0.53
     8   1.1219      0.00     0.40       0.00    -0.05
     9   1.1220      0.00     0.05       0.00     0.09
    10   2.0120      0.00     0.14       0.00    -0.13
    11   2.0121      0.00     0.20       0.00    -0.01
    12   2.0122      0.00     0.25       0.00    -0.09
    13   8.8818      0.00    -0.05       0.00     0.12
    14   8.8820      0.00     0.03       0.00    -0.03
    15   8.9473      0.00     0.26       0.00    -0.07
    16   8.9474      0.00     0.09       0.00    -0.09
    17   8.9501      0.00     0.16       0.00    -0.04
    18   8.9502      0.00     0.00       0.00    -0.05
    19   9.0461      0.00     0.06       0.00     0.05
    20   9.1063      0.00     0.36       0.00    -0.10
    21   9.1118      0.00     0.05       0.00     0.12
    22   9.1851      0.00    -0.13       0.00     0.03
    23   9.2019      0.00     0.17       0.00    -0.04
    24   9.2043      0.00     0.07       0.00     0.02
    25   9.2699      0.00     0.08       0.00    -0.07
    26   9.2730      0.00     0.05       0.00    -0.04
    27   9.2808      0.00     0.01       0.00    -0.01
    28   9.2810      0.00    -0.00       0.00    -0.04
    29   9.2812      0.00    -0.12       0.00     0.03
    30   9.2836      0.00     0.10       0.00    -0.03
    31   9.8429      0.00     0.04       0.00    -0.06
    32   9.8430      0.00    -0.03       0.00     0.03
    33   9.9221      0.00    -0.03       0.00    -0.06
    34   9.9223      0.00     0.01       0.00    -0.09
    35   9.9385      0.00     0.03       0.00    -0.08
    36   9.9388      0.00    -0.09       0.00     0.00
    37   9.9906      0.00     0.02       0.00     0.01
    38   9.9907      0.00    -0.05       0.00     0.00
    39  10.0044      0.00    -0.01       0.00    -0.09
    40  10.0832      0.00     0.00       0.00    -0.03
    41  10.0833      0.00    -0.06       0.00     0.02
    42  10.0834      0.00    -0.08       0.00     0.05
    43  10.0920      0.00    -0.06       0.00     0.02
    44  10.1624      0.00    -0.08       0.00    -0.11
    45  10.1628      0.00     0.02       0.00    -0.03
    46  10.1653      0.00     0.01       0.00     0.03
    47  10.1657      0.00    -0.08       0.00    -0.07
    48  11.0556      0.00    -0.25       0.00     0.39
    49  11.0558      0.00    -0.21       0.00     0.46
    50  11.2087      0.00    -0.12       0.00    -0.02

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.

14UV228    quality flag:3

Type:           3:2E      3:2E      3:2E

axisobj        39.854    39.854    39.854
ecceobj         0.235     0.235     0.235
incobj         10.114    10.114    10.114
qmin           29.507    29.507    29.507
qmax           49.898    49.901    49.897
amean          39.456    39.455    39.456
amin           38.992    38.992    38.992
amax           39.978    39.978    39.978
emean           0.216     0.216     0.216
emin            0.184     0.184     0.184
emax            0.250     0.250     0.250
imean          10.976    10.976    10.976
imin            9.534     9.533     9.534
imax           12.329    12.329    12.329
excite_mean     0.288     0.288     0.288
fracstop        1.000     1.000     1.000
cjmean          2.957     2.957     2.957

libcent 0       179.3     179.3     179.3
libamp  0        93.0      93.0      93.0
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       202.3     202.3     202.3
kozaiamp        180.0     180.0     180.0