Orbit Fit and Astrometric record for 14JQ92

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: 14JQ92    
# Created Mon Dec  6 02:12:24 2021
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting    112 observations of    112
# Arc:   8.45y
# First observation: 2010/02/28
#  Last observation: 2018/08/13
# Chi-squared of fit:    91.73 DOF:    218 RMS:  0.16
# Min/Max residuals:    -0.44    0.53
# Exact a, adot, b, bdot, g, gdot:
  1.987923E-05  5.466181E-02  3.269129E-06  7.447186E-03  3.877325E-02  1.083471E-03
# Covariance matrix:
  2.7334E-13 -9.5926E-14  2.7289E-14 -1.2874E-14 -1.4522E-14 -1.4870E-13
 -9.5926E-14  4.6065E-14 -1.7736E-14  6.8454E-15  2.2663E-14  7.8634E-14
  2.7289E-14 -1.7736E-14  1.1660E-13 -1.9405E-14 -1.6474E-14 -3.1158E-14
 -1.2874E-14  6.8454E-15 -1.9405E-14  3.9858E-15  3.1760E-15  1.2536E-14
 -1.4522E-14  2.2663E-14 -1.6474E-14  3.1760E-15  4.8701E-14  3.5382E-14
 -1.4870E-13  7.8634E-14 -3.1158E-14  1.2536E-14  3.5382E-14  1.4418E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
   22.938862 -128.862992    0.943518    0.123347   -0.291525  2455256.097976
# Heliocentric elements and errors
Epoch:              2455256.5000  =  2010/03/01
Mean Anomaly:          358.09572 +/-     0.001
Argument of Peri:       74.25457 +/-     0.001
Long of Asc Node:      160.48162 +/-     0.000
Inclination:            24.17033 +/-     0.000
Eccentricity:         0.33826062 +/-    0.0000
Semi-Major Axis:     39.41495812 +/-    0.0014
Time of Perihelion: 2455734.5994 +/-       4.8
Perihelion:          26.08242994 +/-    0.0012
Aphelion:            52.74748630 +/-    0.0020
Period (y)              247.4570 +/-      0.01
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -15.83205780 +/-    0.0001
Ecliptic Y          -18.15138717 +/-    0.0001
Ecliptic Z           10.05209659 +/-    0.0001
Ecliptic XDOT         0.00309222 +/-    0.0000
Ecliptic YDOT        -0.00231133 +/-    0.0000
Ecliptic ZDOT         0.00051404 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   26.09927394 +/-    0.0001
Geocenter to KBO     25.79099232 +/-    0.0001
# Hcoef:  8.37

The following table shows the complete astrometric record for 14JQ92. 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 (14JQ92) followed by the observatory code and reference code for the source of the astrometry.

2010 02  28.59721  15 38 22.672  +04 08 56.67  21.4G 14JQ92    F51  C~346Y      
2010 02  28.60780  15 38 22.644  +04 08 57.45  21.5G 14JQ92    F51  C~346Y      
2010 04  19.55065  15 35 42.385  +04 56 44.59  22.1G 14JQ92    F51  C~346Y      
2011 03  15.64329  15 50 49.515  +04 00 46.76  22.5G 14JQ92    F51  C~346Y      
2011 04  28.59505  15 47 41.455  +04 40 45.69  22.4G 14JQ92    F51  C~346Y      
2012 04  14.56168  16 01 48.526  +04 06 27.67  22.8G 14JQ92    F51  C~346Y      
2012 04  27.55954  16 00 35.240  +04 16 55.76  22.8G 14JQ92    F51  C~346Y      
2012 04  27.56995  16 00 35.179  +04 16 56.28  22.1G 14JQ92    F51  C~346Y      
2012 04  27.58204  16 00 35.091  +04 16 57.13  22.0G 14JQ92    F51  C~346Y      
2012 04  27.59326  16 00 35.039  +04 16 57.27  22.9G 14JQ92    F51  C~346Y      
2013 06  18.33773  16 07 38.854  +04 10 40.11  22.9G 14JQ92    F51  C~346Y      
2013 06  18.34881  16 07 38.809  +04 10 40.52  22.2G 14JQ92    F51  C~346Y      
2013 06  18.36041  16 07 38.745  +04 10 40.09  22.4G 14JQ92    F51  C~346Y      
2013 06  18.37057  16 07 38.688  +04 10 40.19  21.5G 14JQ92    F51  C~346Y      
2014 04  23.56992  16 26 34.790  +03 24 18.10  22.0G 14JQ92    F51  C~346Y      
2014 05  09.41168  16 25 00.305  +03 35 12.39  22.2G 14JQ92    F51  C~346Y      
2014 05  09.41244  16 25 00.314  +03 35 12.63  22.0G 14JQ92    F51  C~346Y      
2014 05  09.42492  16 25 00.230  +03 35 12.75  22.5G 14JQ92    F51  C~346Y      
2014 05  09.43666  16 25 00.146  +03 35 13.26  22.6G 14JQ92    F51  C~346Y      
2014 05  09.43743  16 25 00.158  +03 35 13.35  22.1G 14JQ92    F51  C~346Y      
2014 05  09.44918  16 25 00.055  +03 35 13.60  22.1G 14JQ92    F51  C~346Y      
2014 05  09.44995  16 25 00.057  +03 35 13.58  22.8G 14JQ92    F51  C~346Y      
2014 05  09.53633  16 24 59.493  +03 35 16.83  22.3G 14JQ92    F51  C~346Y      
2014 05  09.53699  16 24 59.493  +03 35 16.72  22.4G 14JQ92    F51  C~346Y      
2014 05  09.54846  16 24 59.405  +03 35 17.34  23.1G 14JQ92    F51  C~346Y      
2014 05  09.54912  16 24 59.402  +03 35 17.13  22.6G 14JQ92    F51  C~346Y      
2014 05  09.56055  16 24 59.313  +03 35 17.97  22.1G 14JQ92    F51  C~346Y      
2014 05  09.56121  16 24 59.351  +03 35 17.34  23.0G 14JQ92    F51  C~346Y      
2014 05  09.57267  16 24 59.239  +03 35 17.98  22.5G 14JQ92    F51  C~346Y      
2014 05  09.57333  16 24 59.254  +03 35 18.12  22.4G 14JQ92    F51  C~346Y      
2014 05  21.49244  16 23 38.646  +03 41 15.32  22.5G 14JQ92    F51  C~346Y      
2014 05  21.50384  16 23 38.556  +03 41 15.12  22.2G 14JQ92    F51  C~346Y      
2014 06  28.37501  16 19 25.251  +03 44 29.95  22.4G 14JQ92    F51  C~346Y      
2014 06  28.38656  16 19 25.171  +03 44 29.81  22.8G 14JQ92    F51  C~346Y      
2014 06  28.39810  16 19 25.117  +03 44 29.70  22.6G 14JQ92    F51  C~346Y      
2014 06  28.40966  16 19 25.065  +03 44 29.48  22.4G 14JQ92    F51  C~346Y      
2014 08  21.25167  16 16 56.776  +03 10 07.58  22.0G 14JQ92    F51  C~346Y      
2014 08  21.26382  16 16 56.795  +03 10 06.60  22.1G 14JQ92    F51  C~346Y      
2014 08  21.27590  16 16 56.791  +03 10 06.02  22.5G 14JQ92    F51  C~346Y      
2014 08  21.28800  16 16 56.825  +03 10 05.64  22.6G 14JQ92    F51  C~346Y      
2015 03  23.55337  16 40 53.139  +02 31 35.76  22.3G 14JQ92    F51  C~346Y      
2015 03  23.58031  16 40 53.105  +02 31 38.03  23.3G 14JQ92    F51  C~346Y      
2015 05  14.51261  16 37 12.273  +03 12 29.37  23.1G 14JQ92    F51  C~346Y      
2015 06  20.31479  16 32 58.958  +03 20 47.51  22.0G 14JQ92    F51  C~346Y      
2015 06  20.32741  16 32 58.877  +03 20 47.36  22.0G 14JQ92    F51  C~346Y      
2015 06  20.34010  16 32 58.793  +03 20 47.25  22.0G 14JQ92    F51  C~346Y      
2015 06  20.35278  16 32 58.712  +03 20 47.27  22.1G 14JQ92    F51  C~346Y      
2015 08  17.32580  16 29 17.350  +02 49 43.77  22.6G 14JQ92    F51  C~346Y      
2016 04  02.54767  16 53 00.405  +02 16 08.44  23.0G 14JQ92    F51  C~346Y      
2016 04  02.56077  16 53 00.372  +02 16 09.23  23.0G 14JQ92    F51  C~346Y      
2016 04  02.57393  16 53 00.319  +02 16 09.86  22.6G 14JQ92    F51  C~346Y      
2016 04  02.58726  16 53 00.317  +02 16 10.64  23.0G 14JQ92    F51  C~346Y      
2016 04  10.58569  16 52 38.549  +02 23 11.21  23.2G 14JQ92    F51  C~346Y      
2016 04  10.59759  16 52 38.518  +02 23 11.91  22.4G 14JQ92    F51  C~346Y      
2016 04  10.60946  16 52 38.468  +02 23 12.41  22.8G 14JQ92    F51  C~346Y      
2016 04  10.62133  16 52 38.446  +02 23 13.22  22.5G 14JQ92    F51  C~346Y      
2016 05  06.52447  16 50 36.120  +02 42 38.62  21.3G 14JQ92    F51  C~346Y      
2016 05  06.53651  16 50 36.046  +02 42 39.29  21.4G 14JQ92    F51  C~346Y      
2016 05  06.54835  16 50 35.961  +02 42 39.77  21.7G 14JQ92    F51  C~346Y      
2016 05  06.56024  16 50 35.898  +02 42 40.08  22.0G 14JQ92    F51  C~346Y      
2016 05  13.50674  16 49 52.781  +02 46 37.16  22.5G 14JQ92    F51  C~346Y      
2016 05  13.51943  16 49 52.702  +02 46 37.53  22.5G 14JQ92    F51  C~346Y      
2016 05  13.53211  16 49 52.625  +02 46 38.11  22.7G 14JQ92    F51  C~346Y      
2016 05  13.54493  16 49 52.530  +02 46 38.42  22.3G 14JQ92    F51  C~346Y      
2016 05  27.46642  16 48 18.681  +02 52 28.85  22.0G 14JQ92    F51  C~346Y      
2016 06  03.47127  16 47 29.523  +02 54 16.06  22.4G 14JQ92    F51  C~346Y      
2016 06  03.48246  16 47 29.434  +02 54 16.29  22.2G 14JQ92    F51  C~346Y      
2016 06  03.49364  16 47 29.361  +02 54 16.36  22.2G 14JQ92    F51  C~346Y      
2016 06  03.50483  16 47 29.270  +02 54 16.63  22.4G 14JQ92    F51  C~346Y      
2016 06  10.50818  16 46 40.110  +02 55 14.44  22.3G 14JQ92    F51  C~346Y      
2016 06  23.40880  16 45 12.797  +02 54 50.44  22.1G 14JQ92    F51  C~346Y      
2016 07  01.42162  16 44 22.746  +02 53 09.63  22.9G 14JQ92    F51  C~346Y      
2016 07  05.39641  16 43 59.556  +02 51 56.16  22.0G 14JQ92    F51  C~346Y      
2016 07  05.40846  16 43 59.489  +02 51 56.37  20.8G 14JQ92    F51  C~346Y      
2016 07  05.42052  16 43 59.420  +02 51 55.49  22.3G 14JQ92    F51  C~346Y      
2016 07  05.43262  16 43 59.334  +02 51 55.40  22.7G 14JQ92    F51  C~346Y      
2016 07  28.30733  16 42 15.600  +02 40 09.07  22.7G 14JQ92    F51  C~346Y      
2017 03  29.58728  17 05 26.327  +01 46 58.13  22.6G 14JQ92    F51  C~346Y      
2017 03  29.59938  17 05 26.317  +01 46 58.69  22.5G 14JQ92    F51  C~346Y      
2017 03  29.61148  17 05 26.301  +01 46 59.46  22.7G 14JQ92    F51  C~346Y      
2017 03  29.62360  17 05 26.290  +01 46 59.79  22.5G 14JQ92    F51  C~346Y      
2017 04  20.57514  17 04 27.480  +02 05 28.94  23.1G 14JQ92    F51  C~346Y      
2017 05  04.48322  17 03 20.107  +02 15 20.91  22.6G 14JQ92    F51  C~346Y      
2017 05  06.48903  17 03 08.839  +02 16 35.69  22.7G 14JQ92    F51  C~346Y      
2017 05  18.58269  17 01 54.586  +02 23 03.52  21.9G 14JQ92    F51  C~346Y      
2017 05  30.49475  17 00 33.868  +02 27 22.41  23.1G 14JQ92    F51  C~346Y      
2017 05  30.50704  17 00 33.774  +02 27 23.08  22.1G 14JQ92    F51  C~346Y      
2017 06  25.34856  16 57 35.192  +02 28 51.70  22.6G 14JQ92    F51  C~346Y      
2017 06  25.36134  16 57 35.087  +02 28 51.75  22.5G 14JQ92    F51  C~346Y      
2017 06  25.37412  16 57 35.026  +02 28 51.36  22.4G 14JQ92    F51  C~346Y      
2017 06  25.38681  16 57 34.952  +02 28 51.49  22.3G 14JQ92    F51  C~346Y      
2018 05  23.49192  17 13 50.552  +01 59 02.91  22.7G 14JQ92    F51  C~346Y      
2018 05  23.50421  17 13 50.486  +01 59 03.26  22.3G 14JQ92    F51  C~346Y      
2018 05  23.51641  17 13 50.408  +01 59 03.61  22.9G 14JQ92    F51  C~346Y      
2018 05  23.52875  17 13 50.314  +01 59 03.86  22.7G 14JQ92    F51  C~346Y      
2018 06  08.46122  17 12 00.943  +02 03 11.48  22.1G 14JQ92    F51  C~346Y      
2018 06  08.47255  17 12 00.854  +02 03 11.57  22.2G 14JQ92    F51  C~346Y      
2018 06  08.48329  17 12 00.793  +02 03 11.80  22.9G 14JQ92    F51  C~346Y      
2018 06  08.49403  17 12 00.710  +02 03 11.99  22.6G 14JQ92    F51  C~346Y      
2018 06  15.42419  17 11 12.127  +02 03 43.47  22.5G 14JQ92    F51  C~346Y      
2018 06  15.43620  17 11 12.038  +02 03 43.64  22.7G 14JQ92    F51  C~346Y      
2018 06  15.44816  17 11 11.947  +02 03 43.57  22.5G 14JQ92    F51  C~346Y      
2018 06  15.46008  17 11 11.864  +02 03 43.41  22.7G 14JQ92    F51  C~346Y      
2018 07  08.40047  17 08 41.246  +01 59 50.05  22.4G 14JQ92    F51  C~346Y      
2018 07  08.41235  17 08 41.173  +01 59 49.75  22.8G 14JQ92    F51  C~346Y      
2018 07  08.42423  17 08 41.107  +01 59 49.65  22.6G 14JQ92    F51  C~346Y      
2018 07  08.43608  17 08 41.035  +01 59 49.34  23.0G 14JQ92    F51  C~346Y      
2018 08  03.31788  17 06 38.868  +01 45 52.07  22.0G 14JQ92    F51  C~346Y      
2018 08  03.32996  17 06 38.824  +01 45 51.07  22.2G 14JQ92    F51  C~346Y      
2018 08  03.34198  17 06 38.785  +01 45 51.18  22.5G 14JQ92    F51  C~346Y      
2018 08  03.35402  17 06 38.733  +01 45 50.50  21.9G 14JQ92    F51  C~346Y      
2018 08  13.29115  17 06 12.285  +01 38 17.50  23.0G 14JQ92    F51  C~346Y      

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     0.47       0.00    -0.17
     2   0.0000      0.00     0.04       0.00     0.01
     3   0.1368      0.00     0.27       0.00     0.30
     4   1.0405      0.00    -0.17       0.00    -0.32
     5   1.1608      0.00    -0.23       0.00     0.23
     6   2.1245      0.00    -0.04       0.00    -0.01
     7   2.1601      0.00    -0.22       0.00    -0.09
     8   2.1601      0.00    -0.15       0.00    -0.03
     9   2.1601      0.00    -0.34       0.00     0.29
    10   2.1602      0.00    -0.06       0.00    -0.07
    11   3.3011      0.00    -0.44       0.00    -0.21
    12   3.3012      0.00    -0.06       0.00     0.26
    13   3.3012      0.00     0.09       0.00    -0.11
    14   3.3012      0.00     0.21       0.00     0.04
    15   4.1478      0.00     0.26       0.00     0.23
    16   4.1911      0.00    -0.21       0.00     0.01
    17   4.1911      0.00    -0.00       0.00     0.22
    18   4.1912      0.00    -0.02       0.00    -0.10
    19   4.1912      0.00    -0.11       0.00    -0.00
    20   4.1912      0.00     0.14       0.00     0.06
    21   4.1912      0.00    -0.23       0.00    -0.10
    22   4.1912      0.00    -0.13       0.00    -0.15
    23   4.1915      0.00     0.02       0.00     0.06
    24   4.1915      0.00     0.08       0.00    -0.08
    25   4.1915      0.00    -0.10       0.00     0.14
    26   4.1915      0.00    -0.08       0.00    -0.09
    27   4.1915      0.00    -0.27       0.00     0.35
    28   4.1916      0.00     0.36       0.00    -0.31
    29   4.1916      0.00    -0.18       0.00    -0.07
    30   4.1916      0.00     0.11       0.00     0.05
    31   4.2242      0.00     0.14       0.00     0.26
    32   4.2242      0.00     0.00       0.00    -0.22
    33   4.3279      0.00     0.00       0.00    -0.13
    34   4.3280      0.00    -0.17       0.00    -0.10
    35   4.3280      0.00     0.04       0.00    -0.04
    36   4.3280      0.00     0.28       0.00    -0.09
    37   4.4754      0.00    -0.03       0.00     0.13
    38   4.4755      0.00     0.12       0.00    -0.16
    39   4.4755      0.00    -0.08       0.00    -0.06
    40   4.4755      0.00     0.30       0.00     0.24
    41   5.0622      0.00     0.05       0.00    -0.23
    42   5.0622      0.00     0.01       0.00     0.53
    43   5.2044      0.00    -0.02       0.00    -0.03
    44   5.3052      0.00    -0.04       0.00    -0.00
    45   5.3052      0.00     0.00       0.00    -0.09
    46   5.3053      0.00     0.01       0.00    -0.13
    47   5.3053      0.00     0.07       0.00    -0.05
    48   5.4640      0.00     0.25       0.00     0.16
    49   6.0916      0.00     0.12       0.00    -0.17
    50   6.0916      0.00     0.07       0.00    -0.08
    51   6.0917      0.00    -0.27       0.00    -0.15
    52   6.0917      0.00     0.16       0.00    -0.09
    53   6.1136      0.00     0.01       0.00    -0.10
    54   6.1136      0.00     0.15       0.00    -0.01
    55   6.1137      0.00     0.00       0.00    -0.12
    56   6.1137      0.00     0.27       0.00     0.08
    57   6.1846      0.00     0.03       0.00    -0.16
    58   6.1846      0.00     0.02       0.00     0.07
    59   6.1847      0.00    -0.17       0.00     0.11
    60   6.1847      0.00    -0.03       0.00    -0.02
    61   6.2037      0.00    -0.02       0.00    -0.16
    62   6.2038      0.00     0.05       0.00    -0.18
    63   6.2038      0.00     0.14       0.00    -0.00
    64   6.2038      0.00    -0.02       0.00    -0.09
    65   6.2419      0.00     0.01       0.00     0.11
    66   6.2611      0.00     0.10       0.00    -0.12
    67   6.2612      0.00    -0.03       0.00    -0.02
    68   6.2612      0.00     0.08       0.00    -0.08
    69   6.2612      0.00    -0.09       0.00     0.06
    70   6.2804      0.00     0.03       0.00    -0.18
    71   6.3157      0.00    -0.35       0.00     0.28
    72   6.3376      0.00     0.24       0.00    -0.12
    73   6.3485      0.00    -0.01       0.00    -0.01
    74   6.3486      0.00     0.03       0.00     0.45
    75   6.3486      0.00     0.05       0.00    -0.19
    76   6.3486      0.00    -0.19       0.00    -0.03
    77   6.4113      0.00     0.32       0.00    -0.16
    78   7.0801      0.00    -0.09       0.00     0.08
    79   7.0801      0.00    -0.01       0.00    -0.00
    80   7.0801      0.00    -0.01       0.00     0.12
    81   7.0802      0.00     0.06       0.00    -0.19
    82   7.1403      0.00     0.22       0.00     0.21
    83   7.1783      0.00     0.15       0.00     0.25
    84   7.1838      0.00     0.02       0.00    -0.04
    85   7.2169      0.00     0.06       0.00     0.20
    86   7.2495      0.00     0.06       0.00    -0.24
    87   7.2496      0.00    -0.04       0.00     0.23
    88   7.3203      0.00    -0.14       0.00     0.05
    89   7.3204      0.00    -0.43       0.00     0.22
    90   7.3204      0.00    -0.06       0.00    -0.05
    91   7.3204      0.00     0.10       0.00     0.20
    92   8.2297      0.00    -0.25       0.00    -0.16
    93   8.2297      0.00     0.00       0.00    -0.09
    94   8.2298      0.00     0.06       0.00    -0.02
    95   8.2298      0.00    -0.10       0.00    -0.05
    96   8.2734      0.00    -0.03       0.00    -0.09
    97   8.2734      0.00    -0.15       0.00    -0.09
    98   8.2735      0.00     0.09       0.00     0.05
    99   8.2735      0.00    -0.01       0.00     0.16
   100   8.2925      0.00     0.07       0.00     0.02
   101   8.2925      0.00     0.01       0.00     0.18
   102   8.2925      0.00    -0.07       0.00     0.09
   103   8.2926      0.00    -0.05       0.00    -0.08
   104   8.3554      0.00    -0.12       0.00    -0.01
   105   8.3554      0.00    -0.13       0.00    -0.06
   106   8.3554      0.00    -0.04       0.00     0.09
   107   8.3555      0.00    -0.05       0.00     0.03
   108   8.4263      0.00     0.04       0.00     0.09
   109   8.4264      0.00    -0.00       0.00    -0.40
   110   8.4264      0.00     0.03       0.00     0.22
   111   8.4264      0.00    -0.13       0.00     0.05
   112   8.4536      0.00     0.16       0.00     0.05

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.

14JQ92    quality flag:3

Type:           3:2E      3:2E      3:2E
Type:          6:4II     6:4II     6:4II

axisobj        39.103    39.102    39.103
ecceobj         0.333     0.333     0.333
incobj         24.188    24.188    24.188
qmin           25.306    25.306    25.307
qmax           54.183    54.180    54.191
amean          39.453    39.453    39.453
amin           39.099    39.099    39.099
amax           39.927    39.928    39.931
emean           0.286     0.286     0.286
emin            0.165     0.165     0.165
emax            0.357     0.357     0.357
imean          25.228    25.228    25.229
imin           22.548    22.549    22.547
imax           28.851    28.851    28.851
excite_mean     0.517     0.517     0.517
fracstop        1.000     1.000     1.000
cjmean          2.743     2.743     2.743

libcent 0       178.7     178.7     178.7
libamp  0        31.4      31.4      31.3
libcent 1       179.2     179.2     178.9
libamp  1       165.5     165.7     164.8
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        94.4      94.4      94.4
kozaiamp         67.5      67.5      67.5