Efemérides

SECCIÓN de COMETAS de la LIADA - Liga Iberoamericana de Astronomía - 
Web: https://rastreadoresdecometas.wordpress.com/
EFEMÉRIDES DE COMETAS DEL MES DE DICIEMBRE DE 2019
--~--------~--~----~--------~-------~--~----~--~--~--------~--~----~--------~------~--~----
2I/Borisov
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  11 15 36.1  -12 33 42   2.049   2.014   74.0   28.1  15.6
2019 12 02  000000  11 17 18.0  -13 18 59   2.040   2.012   74.3   28.2  15.6
2019 12 03  000000  11 18 59.7  -14 04 25   2.032   2.010   74.6   28.2  15.6
2019 12 04  000000  11 20 41.2  -14 50 01   2.025   2.009   75.0   28.3  15.6
2019 12 05  000000  11 22 22.3  -15 35 46   2.018   2.008   75.3   28.3  15.6
2019 12 06  000000  11 24 03.3  -16 21 38   2.011   2.007   75.6   28.4  15.5
2019 12 07  000000  11 25 43.9  -17 07 37   2.004   2.007   75.9   28.4  15.5
2019 12 08  000000  11 27 24.2  -17 53 41   1.998   2.007   76.3   28.5  15.5
2019 12 09  000000  11 29 04.3  -18 39 50   1.992   2.007   76.6   28.5  15.5
2019 12 10  000000  11 30 44.1  -19 26 03   1.986   2.007   76.9   28.6  15.5
2019 12 11  000000  11 32 23.5  -20 12 19   1.981   2.007   77.2   28.6  15.5
2019 12 12  000000  11 34 02.7  -20 58 37   1.976   2.008   77.5   28.6  15.5
2019 12 13  000000  11 35 41.6  -21 44 55   1.971   2.009   77.8   28.6  15.5
2019 12 14  000000  11 37 20.1  -22 31 13   1.966   2.010   78.2   28.6  15.5
2019 12 15  000000  11 38 58.3  -23 17 30   1.962   2.012   78.5   28.6  15.5
2019 12 16  000000  11 40 36.1  -24 03 44   1.958   2.013   78.8   28.6  15.5
2019 12 17  000000  11 42 13.6  -24 49 55   1.955   2.015   79.1   28.6  15.5
2019 12 18  000000  11 43 50.6  -25 36 02   1.952   2.018   79.4   28.6  15.5
2019 12 19  000000  11 45 27.4  -26 22 03   1.949   2.020   79.7   28.6  15.5
2019 12 20  000000  11 47 03.6  -27 07 58   1.946   2.023   80.0   28.6  15.5
2019 12 21  000000  11 48 39.5  -27 53 46   1.944   2.026   80.3   28.6  15.5
2019 12 22  000000  11 50 14.9  -28 39 25   1.942   2.029   80.6   28.6  15.5
2019 12 23  000000  11 51 49.9  -29 24 54   1.941   2.032   80.9   28.6  15.5
2019 12 24  000000  11 53 24.4  -30 10 13   1.939   2.036   81.2   28.5  15.5
2019 12 25  000000  11 54 58.4  -30 55 20   1.938   2.040   81.5   28.5  15.5
2019 12 26  000000  11 56 31.9  -31 40 15   1.937   2.044   81.8   28.4  15.5
2019 12 27  000000  11 58 04.9  -32 24 56   1.937   2.048   82.1   28.4  15.5
2019 12 28  000000  11 59 37.3  -33 09 22   1.937   2.053   82.4   28.4  15.6
2019 12 29  000000  12 01 09.1  -33 53 34   1.937   2.057   82.7   28.3  15.6
2019 12 30  000000  12 02 40.4  -34 37 29   1.937   2.062   83.0   28.2  15.6
2019 12 31  000000  12 04 11.1  -35 21 06   1.938   2.068   83.3   28.2  15.6
2020 01 01  000000  12 05 41.2  -36 04 26   1.939   2.073   83.6   28.1  15.6
2020 01 02  000000  12 07 10.6  -36 47 27   1.940   2.079   83.9   28.1  15.6
2020 01 03  000000  12 08 39.4  -37 30 09   1.941   2.085   84.1   28.0  15.6
2020 01 04  000000  12 10 07.5  -38 12 30   1.943   2.091   84.4   27.9  15.6
2020 01 05  000000  12 11 34.9  -38 54 30   1.945   2.097   84.7   27.8  15.7
2020 01 06  000000  12 13 01.5  -39 36 08   1.947   2.104   85.0   27.7  15.7
2020 01 07  000000  12 14 27.5  -40 17 24   1.950   2.111   85.3   27.7  15.7
2020 01 08  000000  12 15 52.7  -40 58 17   1.952   2.118   85.6   27.6  15.7
2020 01 09  000000  12 17 17.0  -41 38 46   1.955   2.125   85.9   27.5  15.7
2020 01 10  000000  12 18 40.6  -42 18 51   1.958   2.132   86.2   27.4  15.7
2020 01 11  000000  12 20 03.3  -42 58 32   1.962   2.140   86.5   27.3  15.8
2020 01 12  000000  12 21 25.2  -43 37 47   1.965   2.147   86.8   27.2  15.8
2020 01 13  000000  12 22 46.1  -44 16 37   1.969   2.155   87.1   27.1  15.8
2020 01 14  000000  12 24 06.2  -44 55 00   1.973   2.164   87.4   27.0  15.8
2020 01 15  000000  12 25 25.2  -45 32 57   1.977   2.172   87.6   26.9  15.8


C/2019 K1 (ATLAS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  16 15 36.0  -58 16 17   2.911   2.200   36.6   15.5  15.6
2019 12 02  000000  16 17 47.0  -58 35 55   2.904   2.195   36.8   15.6  15.6
2019 12 03  000000  16 20 01.1  -58 55 42   2.896   2.191   37.0   15.7  15.6
2019 12 04  000000  16 22 18.3  -59 15 39   2.888   2.186   37.2   15.8  15.6
2019 12 05  000000  16 24 38.9  -59 35 45   2.880   2.181   37.5   16.0  15.6
2019 12 06  000000  16 27 02.9  -59 56 00   2.871   2.177   37.7   16.1  15.6
2019 12 07  000000  16 29 30.5  -60 16 24   2.863   2.172   38.0   16.2  15.6
2019 12 08  000000  16 32 01.8  -60 36 57   2.854   2.168   38.2   16.3  15.5
2019 12 09  000000  16 34 37.1  -60 57 39   2.846   2.163   38.5   16.5  15.5
2019 12 10  000000  16 37 16.4  -61 18 29   2.837   2.159   38.8   16.6  15.5
2019 12 11  000000  16 40 00.1  -61 39 27   2.828   2.155   39.1   16.7  15.5
2019 12 12  000000  16 42 48.1  -62 00 33   2.819   2.151   39.3   16.9  15.5
2019 12 13  000000  16 45 40.9  -62 21 46   2.810   2.146   39.7   17.0  15.5
2019 12 14  000000  16 48 38.6  -62 43 06   2.801   2.142   40.0   17.2  15.4
2019 12 15  000000  16 51 41.4  -63 04 33   2.792   2.138   40.3   17.3  15.4
2019 12 16  000000  16 54 49.5  -63 26 06   2.783   2.134   40.6   17.5  15.4
2019 12 17  000000  16 58 03.4  -63 47 45   2.773   2.130   41.0   17.6  15.4
2019 12 18  000000  17 01 23.1  -64 09 29   2.764   2.126   41.3   17.8  15.4
2019 12 19  000000  17 04 49.1  -64 31 17   2.755   2.123   41.6   17.9  15.4
2019 12 20  000000  17 08 21.6  -64 53 09   2.745   2.119   42.0   18.1  15.4
2019 12 21  000000  17 12 01.0  -65 15 04   2.735   2.115   42.4   18.3  15.3
2019 12 22  000000  17 15 47.6  -65 37 02   2.726   2.111   42.7   18.4  15.3
2019 12 23  000000  17 19 41.7  -65 59 00   2.716   2.108   43.1   18.6  15.3
2019 12 24  000000  17 23 43.9  -66 21 00   2.706   2.104   43.5   18.8  15.3
2019 12 25  000000  17 27 54.4  -66 42 58   2.697   2.101   43.8   18.9  15.3
2019 12 26  000000  17 32 13.7  -67 04 54   2.687   2.097   44.2   19.1  15.3
2019 12 27  000000  17 36 42.3  -67 26 47   2.677   2.094   44.6   19.3  15.2
2019 12 28  000000  17 41 20.6  -67 48 36   2.667   2.091   45.0   19.4  15.2
2019 12 29  000000  17 46 09.1  -68 10 18   2.657   2.087   45.4   19.6  15.2
2019 12 30  000000  17 51 08.4  -68 31 51   2.647   2.084   45.8   19.8  15.2
2019 12 31  000000  17 56 19.0  -68 53 15   2.638   2.081   46.2   19.9  15.2
2020 01 01  000000  18 01 41.4  -69 14 27   2.628   2.078   46.6   20.1  15.2
2020 01 02  000000  18 07 16.3  -69 35 24   2.618   2.075   47.0   20.3  15.2
2020 01 03  000000  18 13 04.1  -69 56 04   2.608   2.072   47.4   20.4  15.1
2020 01 04  000000  18 19 05.6  -70 16 25   2.598   2.069   47.8   20.6  15.1
2020 01 05  000000  18 25 21.2  -70 36 24   2.588   2.067   48.2   20.8  15.1
2020 01 06  000000  18 31 51.6  -70 55 58   2.579   2.064   48.6   20.9  15.1
2020 01 07  000000  18 38 37.3  -71 15 03   2.569   2.061   48.9   21.1  15.1
2020 01 08  000000  18 45 38.9  -71 33 36   2.559   2.059   49.3   21.2  15.1
2020 01 09  000000  18 52 56.9  -71 51 33   2.550   2.056   49.7   21.4  15.1
2020 01 10  000000  19 00 31.8  -72 08 50   2.540   2.054   50.1   21.6  15.0
2020 01 11  000000  19 08 23.8  -72 25 23   2.531   2.051   50.5   21.7  15.0
2020 01 12  000000  19 16 33.3  -72 41 08   2.522   2.049   50.9   21.9  15.0
2020 01 13  000000  19 25 00.5  -72 56 00   2.512   2.047   51.3   22.0  15.0
2020 01 14  000000  19 33 45.3  -73 09 54   2.503   2.045   51.7   22.2  15.0
2020 01 15  000000  19 42 47.7  -73 22 45   2.494   2.043   52.1   22.3  15.0


C/2019 A9 (PANSTARRS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  17 15 44.4  -56 58 45   2.944   2.230   36.5   15.2  20.8
2019 12 02  000000  17 18 54.7  -56 46 48   2.960   2.239   36.1   15.0  20.9
2019 12 03  000000  17 22 01.6  -56 34 51   2.975   2.249   35.7   14.8  20.9
2019 12 04  000000  17 25 05.0  -56 22 55   2.990   2.259   35.3   14.6  20.9
2019 12 05  000000  17 28 05.2  -56 11 00   3.005   2.268   34.9   14.4  20.9
2019 12 06  000000  17 31 02.1  -55 59 07   3.020   2.278   34.6   14.2  21.0
2019 12 07  000000  17 33 55.9  -55 47 15   3.034   2.287   34.2   14.0  21.0
2019 12 08  000000  17 36 46.6  -55 35 25   3.049   2.297   33.8   13.8  21.0
2019 12 09  000000  17 39 34.4  -55 23 38   3.063   2.307   33.5   13.6  21.1
2019 12 10  000000  17 42 19.3  -55 11 53   3.078   2.316   33.1   13.4  21.1
2019 12 11  000000  17 45 01.4  -55 00 11   3.092   2.326   32.8   13.2  21.1
2019 12 12  000000  17 47 40.8  -54 48 32   3.106   2.336   32.4   13.1  21.1
2019 12 13  000000  17 50 17.5  -54 36 56   3.120   2.345   32.1   12.9  21.2
2019 12 14  000000  17 52 51.7  -54 25 23   3.134   2.355   31.8   12.7  21.2
2019 12 15  000000  17 55 23.3  -54 13 54   3.148   2.365   31.5   12.6  21.2
2019 12 16  000000  17 57 52.5  -54 02 28   3.161   2.375   31.2   12.4  21.3
2019 12 17  000000  18 00 19.3  -53 51 06   3.175   2.384   30.9   12.2  21.3
2019 12 18  000000  18 02 43.8  -53 39 49   3.188   2.394   30.6   12.1  21.3
2019 12 19  000000  18 05 06.0  -53 28 35   3.201   2.404   30.3   11.9  21.3
2019 12 20  000000  18 07 26.1  -53 17 25   3.214   2.414   30.1   11.8  21.4
2019 12 21  000000  18 09 43.9  -53 06 20   3.227   2.423   29.9   11.7  21.4
2019 12 22  000000  18 11 59.7  -52 55 19   3.239   2.433   29.6   11.5  21.4
2019 12 23  000000  18 14 13.4  -52 44 23   3.252   2.443   29.4   11.4  21.4
2019 12 24  000000  18 16 25.1  -52 33 31   3.264   2.453   29.2   11.3  21.5
2019 12 25  000000  18 18 34.8  -52 22 44   3.276   2.462   29.0   11.2  21.5
2019 12 26  000000  18 20 42.6  -52 12 02   3.288   2.472   28.8   11.1  21.5
2019 12 27  000000  18 22 48.6  -52 01 24   3.299   2.482   28.7   11.0  21.5
2019 12 28  000000  18 24 52.6  -51 50 52   3.311   2.492   28.5   10.9  21.6
2019 12 29  000000  18 26 54.9  -51 40 24   3.322   2.502   28.4   10.8  21.6
2019 12 30  000000  18 28 55.4  -51 30 01   3.333   2.512   28.3   10.7  21.6
2019 12 31  000000  18 30 54.1  -51 19 44   3.344   2.521   28.2   10.6  21.6
2020 01 01  000000  18 32 51.2  -51 09 31   3.355   2.531   28.2   10.6  21.7
2020 01 02  000000  18 34 46.5  -50 59 23   3.366   2.541   28.1   10.5  21.7
2020 01 03  000000  18 36 40.2  -50 49 20   3.376   2.551   28.1   10.4  21.7
2020 01 04  000000  18 38 32.4  -50 39 23   3.386   2.561   28.1   10.4  21.7
2020 01 05  000000  18 40 22.9  -50 29 30   3.396   2.571   28.1   10.4  21.8
2020 01 06  000000  18 42 11.8  -50 19 43   3.406   2.580   28.1   10.3  21.8
2020 01 07  000000  18 43 59.3  -50 10 00   3.416   2.590   28.1   10.3  21.8
2020 01 08  000000  18 45 45.2  -50 00 23   3.425   2.600   28.2   10.3  21.8
2020 01 09  000000  18 47 29.7  -49 50 51   3.434   2.610   28.3   10.3  21.8
2020 01 10  000000  18 49 12.7  -49 41 24   3.443   2.620   28.3   10.3  21.9
2020 01 11  000000  18 50 54.3  -49 32 02   3.452   2.630   28.5   10.3  21.9
2020 01 12  000000  18 52 34.5  -49 22 46   3.461   2.640   28.6   10.3  21.9
2020 01 13  000000  18 54 13.3  -49 13 34   3.469   2.650   28.8   10.3  21.9
2020 01 14  000000  18 55 50.8  -49 04 28   3.477   2.659   28.9   10.3  22.0
2020 01 15  000000  18 57 26.9  -48 55 27   3.485   2.669   29.1   10.3  22.0


C/2018 W2 (Africano)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  21 53 51.7  -32 08 21   1.945   1.892   72.2   29.7  13.7
2019 12 02  000000  21 54 22.2  -32 21 29   1.970   1.899   71.3   29.5  13.8
2019 12 03  000000  21 54 54.0  -32 34 10   1.996   1.907   70.4   29.1  13.8
2019 12 04  000000  21 55 27.1  -32 46 24   2.022   1.914   69.5   28.8  13.8
2019 12 05  000000  21 56 01.5  -32 58 14   2.047   1.921   68.6   28.5  13.9
2019 12 06  000000  21 56 37.0  -33 09 41   2.072   1.928   67.7   28.2  13.9
2019 12 07  000000  21 57 13.7  -33 20 45   2.097   1.936   66.9   27.9  14.0
2019 12 08  000000  21 57 51.5  -33 31 27   2.122   1.943   66.0   27.6  14.0
2019 12 09  000000  21 58 30.4  -33 41 50   2.147   1.951   65.2   27.3  14.1
2019 12 10  000000  21 59 10.4  -33 51 52   2.172   1.958   64.3   27.0  14.1
2019 12 11  000000  21 59 51.4  -34 01 36   2.196   1.966   63.5   26.6  14.1
2019 12 12  000000  22 00 33.3  -34 11 02   2.220   1.973   62.7   26.3  14.2
2019 12 13  000000  22 01 16.3  -34 20 12   2.244   1.981   61.9   26.0  14.2
2019 12 14  000000  22 02 00.2  -34 29 04   2.268   1.989   61.1   25.7  14.3
2019 12 15  000000  22 02 45.0  -34 37 42   2.292   1.996   60.3   25.4  14.3
2019 12 16  000000  22 03 30.7  -34 46 04   2.315   2.004   59.5   25.0  14.3
2019 12 17  000000  22 04 17.3  -34 54 12   2.339   2.012   58.7   24.7  14.4
2019 12 18  000000  22 05 04.7  -35 02 07   2.362   2.020   57.9   24.4  14.4
2019 12 19  000000  22 05 53.0  -35 09 49   2.385   2.028   57.2   24.1  14.5
2019 12 20  000000  22 06 42.1  -35 17 18   2.408   2.036   56.4   23.7  14.5
2019 12 21  000000  22 07 32.0  -35 24 35   2.430   2.044   55.7   23.4  14.5
2019 12 22  000000  22 08 22.7  -35 31 41   2.453   2.052   54.9   23.1  14.6
2019 12 23  000000  22 09 14.1  -35 38 36   2.475   2.060   54.2   22.8  14.6
2019 12 24  000000  22 10 06.3  -35 45 21   2.497   2.068   53.5   22.5  14.6
2019 12 25  000000  22 10 59.1  -35 51 56   2.518   2.076   52.7   22.1  14.7
2019 12 26  000000  22 11 52.7  -35 58 21   2.540   2.084   52.0   21.8  14.7
2019 12 27  000000  22 12 47.0  -36 04 38   2.561   2.092   51.3   21.5  14.7
2019 12 28  000000  22 13 42.0  -36 10 46   2.582   2.101   50.6   21.2  14.8
2019 12 29  000000  22 14 37.6  -36 16 46   2.603   2.109   49.9   20.9  14.8
2019 12 30  000000  22 15 33.8  -36 22 39   2.624   2.117   49.3   20.6  14.9
2019 12 31  000000  22 16 30.7  -36 28 24   2.644   2.126   48.6   20.3  14.9
2020 01 01  000000  22 17 28.1  -36 34 02   2.664   2.134   47.9   20.0  14.9
2020 01 02  000000  22 18 26.1  -36 39 34   2.684   2.142   47.3   19.7  15.0
2020 01 03  000000  22 19 24.7  -36 45 00   2.704   2.151   46.6   19.4  15.0
2020 01 04  000000  22 20 23.9  -36 50 19   2.723   2.159   46.0   19.1  15.0
2020 01 05  000000  22 21 23.6  -36 55 34   2.743   2.168   45.4   18.8  15.1
2020 01 06  000000  22 22 23.8  -37 00 43   2.762   2.176   44.8   18.5  15.1
2020 01 07  000000  22 23 24.6  -37 05 47   2.780   2.185   44.2   18.3  15.1
2020 01 08  000000  22 24 25.8  -37 10 46   2.799   2.194   43.6   18.0  15.1
2020 01 09  000000  22 25 27.6  -37 15 41   2.817   2.202   43.0   17.7  15.2
2020 01 10  000000  22 26 29.8  -37 20 32   2.835   2.211   42.4   17.5  15.2
2020 01 11  000000  22 27 32.5  -37 25 19   2.853   2.220   41.8   17.2  15.2
2020 01 12  000000  22 28 35.6  -37 30 02   2.871   2.228   41.3   16.9  15.3
2020 01 13  000000  22 29 39.3  -37 34 42   2.888   2.237   40.8   16.7  15.3
2020 01 14  000000  22 30 43.3  -37 39 19   2.905   2.246   40.2   16.4  15.3
2020 01 15  000000  22 31 47.8  -37 43 53   2.922   2.254   39.7   16.2  15.4


C/2018 N2 (ASASSN)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  23 48 54.6  +39 09 56   2.528   3.131  119.3   16.0  13.0
2019 12 02  000000  23 47 43.5  +39 10 09   2.541   3.131  118.3   16.1  13.0
2019 12 03  000000  23 46 34.8  +39 10 21   2.555   3.132  117.3   16.2  13.0
2019 12 04  000000  23 45 28.7  +39 10 33   2.568   3.133  116.4   16.4  13.0
2019 12 05  000000  23 44 25.0  +39 10 46   2.582   3.133  115.4   16.5  13.0
2019 12 06  000000  23 43 23.8  +39 11 01   2.595   3.134  114.4   16.6  13.0
2019 12 07  000000  23 42 25.1  +39 11 16   2.609   3.135  113.5   16.8  13.0
2019 12 08  000000  23 41 28.7  +39 11 34   2.623   3.136  112.6   16.9  13.1
2019 12 09  000000  23 40 34.8  +39 11 55   2.637   3.137  111.6   17.0  13.1
2019 12 10  000000  23 39 43.2  +39 12 18   2.651   3.137  110.7   17.1  13.1
2019 12 11  000000  23 38 53.9  +39 12 44   2.666   3.138  109.8   17.2  13.1
2019 12 12  000000  23 38 06.9  +39 13 15   2.680   3.139  108.8   17.3  13.1
2019 12 13  000000  23 37 22.2  +39 13 49   2.694   3.140  107.9   17.4  13.1
2019 12 14  000000  23 36 39.7  +39 14 27   2.709   3.141  107.0   17.4  13.1
2019 12 15  000000  23 35 59.4  +39 15 10   2.723   3.142  106.1   17.5  13.1
2019 12 16  000000  23 35 21.3  +39 15 59   2.738   3.143  105.2   17.6  13.2
2019 12 17  000000  23 34 45.3  +39 16 52   2.753   3.144  104.3   17.7  13.2
2019 12 18  000000  23 34 11.5  +39 17 51   2.768   3.145  103.4   17.7  13.2
2019 12 19  000000  23 33 39.7  +39 18 55   2.782   3.146  102.6   17.8  13.2
2019 12 20  000000  23 33 10.0  +39 20 06   2.797   3.148  101.7   17.8  13.2
2019 12 21  000000  23 32 42.3  +39 21 23   2.812   3.149  100.8   17.9  13.2
2019 12 22  000000  23 32 16.5  +39 22 46   2.827   3.150  100.0   17.9  13.2
2019 12 23  000000  23 31 52.7  +39 24 17   2.842   3.151   99.1   18.0  13.3
2019 12 24  000000  23 31 30.9  +39 25 54   2.857   3.153   98.3   18.0  13.3
2019 12 25  000000  23 31 10.9  +39 27 38   2.872   3.154   97.4   18.0  13.3
2019 12 26  000000  23 30 52.8  +39 29 30   2.887   3.155   96.6   18.0  13.3
2019 12 27  000000  23 30 36.5  +39 31 30   2.903   3.157   95.8   18.1  13.3
2019 12 28  000000  23 30 22.0  +39 33 37   2.918   3.158   94.9   18.1  13.3
2019 12 29  000000  23 30 09.3  +39 35 52   2.933   3.159   94.1   18.1  13.3
2019 12 30  000000  23 29 58.2  +39 38 15   2.948   3.161   93.3   18.1  13.3
2019 12 31  000000  23 29 48.9  +39 40 46   2.963   3.162   92.5   18.1  13.4
2020 01 01  000000  23 29 41.2  +39 43 26   2.978   3.164   91.7   18.1  13.4
2020 01 02  000000  23 29 35.1  +39 46 14   2.993   3.165   90.9   18.1  13.4
2020 01 03  000000  23 29 30.6  +39 49 10   3.008   3.167   90.1   18.1  13.4
2020 01 04  000000  23 29 27.7  +39 52 15   3.023   3.168   89.4   18.1  13.4
2020 01 05  000000  23 29 26.3  +39 55 28   3.038   3.170   88.6   18.1  13.4
2020 01 06  000000  23 29 26.4  +39 58 50   3.053   3.172   87.8   18.0  13.4
2020 01 07  000000  23 29 27.9  +40 02 21   3.068   3.173   87.1   18.0  13.4
2020 01 08  000000  23 29 30.9  +40 06 01   3.083   3.175   86.3   18.0  13.5
2020 01 09  000000  23 29 35.2  +40 09 49   3.097   3.177   85.6   18.0  13.5
2020 01 10  000000  23 29 41.0  +40 13 46   3.112   3.179   84.9   17.9  13.5
2020 01 11  000000  23 29 48.1  +40 17 52   3.127   3.180   84.1   17.9  13.5
2020 01 12  000000  23 29 56.5  +40 22 07   3.142   3.182   83.4   17.9  13.5
2020 01 13  000000  23 30 06.2  +40 26 31   3.156   3.184   82.7   17.8  13.5
2020 01 14  000000  23 30 17.2  +40 31 04   3.171   3.186   82.0   17.8  13.5
2020 01 15  000000  23 30 29.5  +40 35 45   3.185   3.188   81.3   17.8  13.6


C/2018 F4 (PANSTARRS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  14 04 33.0  -81 59 32   3.793   3.440   61.9   14.6  17.5
2019 12 02  000000  14 11 08.9  -82 21 11   3.791   3.440   62.0   14.7  17.5
2019 12 03  000000  14 18 19.3  -82 42 37   3.790   3.440   62.0   14.7  17.5
2019 12 04  000000  14 26 09.3  -83 03 49   3.788   3.440   62.1   14.7  17.5
2019 12 05  000000  14 34 44.7  -83 24 42   3.787   3.440   62.2   14.7  17.5
2019 12 06  000000  14 44 12.2  -83 45 10   3.786   3.440   62.3   14.7  17.5
2019 12 07  000000  14 54 39.7  -84 05 10   3.784   3.440   62.4   14.7  17.5
2019 12 08  000000  15 06 16.1  -84 24 34   3.783   3.440   62.4   14.7  17.5
2019 12 09  000000  15 19 11.5  -84 43 15   3.782   3.440   62.5   14.7  17.5
2019 12 10  000000  15 33 36.9  -85 01 01   3.781   3.440   62.6   14.7  17.5
2019 12 11  000000  15 49 43.6  -85 17 43   3.780   3.440   62.7   14.7  17.5
2019 12 12  000000  16 07 42.6  -85 33 05   3.779   3.441   62.7   14.7  17.5
2019 12 13  000000  16 27 42.7  -85 46 52   3.778   3.441   62.8   14.7  17.5
2019 12 14  000000  16 49 48.3  -85 58 45   3.777   3.441   62.9   14.7  17.5
2019 12 15  000000  17 13 56.2  -86 08 27   3.776   3.441   62.9   14.8  17.5
2019 12 16  000000  17 39 53.0  -86 15 37   3.775   3.442   63.0   14.8  17.5
2019 12 17  000000  18 07 13.1  -86 19 59   3.774   3.442   63.0   14.8  17.5
2019 12 18  000000  18 35 19.4  -86 21 22   3.774   3.442   63.1   14.8  17.5
2019 12 19  000000  19 03 27.8  -86 19 41   3.773   3.443   63.2   14.8  17.5
2019 12 20  000000  19 30 53.9  -86 14 59   3.772   3.443   63.2   14.8  17.5
2019 12 21  000000  19 56 59.9  -86 07 26   3.772   3.443   63.3   14.8  17.5
2019 12 22  000000  20 21 18.9  -85 57 15   3.772   3.444   63.3   14.8  17.5
2019 12 23  000000  20 43 36.4  -85 44 46   3.771   3.444   63.4   14.8  17.5
2019 12 24  000000  21 03 48.6  -85 30 17   3.771   3.445   63.4   14.8  17.5
2019 12 25  000000  21 21 59.2  -85 14 05   3.771   3.445   63.4   14.8  17.5
2019 12 26  000000  21 38 16.8  -84 56 26   3.771   3.446   63.5   14.8  17.5
2019 12 27  000000  21 52 52.0  -84 37 34   3.771   3.446   63.5   14.8  17.5
2019 12 28  000000  22 05 56.5  -84 17 40   3.771   3.447   63.5   14.8  17.5
2019 12 29  000000  22 17 41.0  -83 56 55   3.771   3.448   63.6   14.8  17.5
2019 12 30  000000  22 28 15.9  -83 35 26   3.771   3.448   63.6   14.8  17.5
2019 12 31  000000  22 37 50.2  -83 13 20   3.772   3.449   63.6   14.8  17.5
2020 01 01  000000  22 46 31.8  -82 50 43   3.772   3.450   63.6   14.8  17.5
2020 01 02  000000  22 54 27.5  -82 27 40   3.773   3.450   63.6   14.8  17.5
2020 01 03  000000  23 01 43.2  -82 04 14   3.773   3.451   63.6   14.8  17.5
2020 01 04  000000  23 08 24.0  -81 40 28   3.774   3.452   63.6   14.8  17.5
2020 01 05  000000  23 14 34.3  -81 16 25   3.775   3.452   63.6   14.8  17.5
2020 01 06  000000  23 20 17.6  -80 52 08   3.775   3.453   63.6   14.8  17.5
2020 01 07  000000  23 25 37.1  -80 27 39   3.776   3.454   63.6   14.8  17.5
2020 01 08  000000  23 30 35.6  -80 02 59   3.777   3.455   63.6   14.8  17.5
2020 01 09  000000  23 35 15.5  -79 38 09   3.778   3.456   63.6   14.8  17.5
2020 01 10  000000  23 39 38.7  -79 13 12   3.780   3.457   63.6   14.8  17.5
2020 01 11  000000  23 43 47.1  -78 48 07   3.781   3.458   63.6   14.8  17.5
2020 01 12  000000  23 47 42.0  -78 22 57   3.782   3.459   63.6   14.8  17.5
2020 01 13  000000  23 51 25.0  -77 57 42   3.784   3.460   63.6   14.7  17.5
2020 01 14  000000  23 54 57.1  -77 32 22   3.785   3.461   63.5   14.7  17.5
2020 01 15  000000  23 58 19.4  -77 06 59   3.787   3.462   63.5   14.7  17.5


C/2018 A6 (Gibbs)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  21 14 07.7  -71 18 35   3.572   3.259   63.8   15.8  16.9
2019 12 02  000000  21 16 18.6  -70 53 39   3.582   3.262   63.4   15.7  16.9
2019 12 03  000000  21 18 26.4  -70 28 49   3.592   3.265   63.0   15.6  16.9
2019 12 04  000000  21 20 31.3  -70 04 04   3.602   3.269   62.6   15.5  16.9
2019 12 05  000000  21 22 33.5  -69 39 26   3.613   3.272   62.2   15.5  16.9
2019 12 06  000000  21 24 33.1  -69 14 54   3.623   3.275   61.8   15.4  16.9
2019 12 07  000000  21 26 30.3  -68 50 28   3.634   3.279   61.4   15.3  17.0
2019 12 08  000000  21 28 25.3  -68 26 09   3.644   3.282   61.0   15.2  17.0
2019 12 09  000000  21 30 18.1  -68 01 56   3.655   3.285   60.6   15.1  17.0
2019 12 10  000000  21 32 08.9  -67 37 50   3.665   3.289   60.2   15.1  17.0
2019 12 11  000000  21 33 57.8  -67 13 51   3.676   3.292   59.8   15.0  17.0
2019 12 12  000000  21 35 45.0  -66 49 59   3.687   3.296   59.4   14.9  17.0
2019 12 13  000000  21 37 30.3  -66 26 14   3.697   3.299   59.0   14.8  17.0
2019 12 14  000000  21 39 14.1  -66 02 36   3.708   3.303   58.5   14.7  17.0
2019 12 15  000000  21 40 56.4  -65 39 05   3.719   3.306   58.1   14.6  17.0
2019 12 16  000000  21 42 37.1  -65 15 42   3.730   3.310   57.7   14.6  17.1
2019 12 17  000000  21 44 16.5  -64 52 27   3.740   3.313   57.3   14.5  17.1
2019 12 18  000000  21 45 54.6  -64 29 18   3.751   3.317   56.8   14.4  17.1
2019 12 19  000000  21 47 31.4  -64 06 18   3.762   3.321   56.4   14.3  17.1
2019 12 20  000000  21 49 07.0  -63 43 24   3.773   3.324   56.0   14.2  17.1
2019 12 21  000000  21 50 41.5  -63 20 39   3.784   3.328   55.6   14.1  17.1
2019 12 22  000000  21 52 14.9  -62 58 02   3.795   3.331   55.1   14.0  17.1
2019 12 23  000000  21 53 47.2  -62 35 32   3.805   3.335   54.7   13.9  17.1
2019 12 24  000000  21 55 18.5  -62 13 10   3.816   3.339   54.3   13.8  17.1
2019 12 25  000000  21 56 48.9  -61 50 56   3.827   3.342   53.8   13.7  17.2
2019 12 26  000000  21 58 18.3  -61 28 51   3.838   3.346   53.4   13.7  17.2
2019 12 27  000000  21 59 46.9  -61 06 53   3.849   3.350   53.0   13.6  17.2
2019 12 28  000000  22 01 14.6  -60 45 03   3.859   3.354   52.5   13.5  17.2
2019 12 29  000000  22 02 41.4  -60 23 22   3.870   3.357   52.1   13.4  17.2
2019 12 30  000000  22 04 07.4  -60 01 49   3.881   3.361   51.7   13.3  17.2
2019 12 31  000000  22 05 32.7  -59 40 24   3.892   3.365   51.3   13.2  17.2
2020 01 01  000000  22 06 57.2  -59 19 08   3.902   3.369   50.8   13.1  17.2
2020 01 02  000000  22 08 20.9  -58 57 59   3.913   3.372   50.4   13.0  17.2
2020 01 03  000000  22 09 44.0  -58 36 59   3.923   3.376   50.0   12.9  17.3
2020 01 04  000000  22 11 06.3  -58 16 08   3.934   3.380   49.6   12.8  17.3
2020 01 05  000000  22 12 28.0  -57 55 24   3.945   3.384   49.1   12.7  17.3
2020 01 06  000000  22 13 49.0  -57 34 49   3.955   3.388   48.7   12.6  17.3
2020 01 07  000000  22 15 09.4  -57 14 22   3.965   3.392   48.3   12.5  17.3
2020 01 08  000000  22 16 29.2  -56 54 04   3.976   3.396   47.9   12.4  17.3
2020 01 09  000000  22 17 48.4  -56 33 54   3.986   3.400   47.5   12.3  17.3
2020 01 10  000000  22 19 06.9  -56 13 52   3.996   3.403   47.1   12.2  17.3
2020 01 11  000000  22 20 24.9  -55 53 59   4.007   3.407   46.6   12.1  17.3
2020 01 12  000000  22 21 42.4  -55 34 14   4.017   3.411   46.2   12.0  17.3
2020 01 13  000000  22 22 59.3  -55 14 37   4.027   3.415   45.8   11.9  17.4
2020 01 14  000000  22 24 15.6  -54 55 08   4.037   3.419   45.4   11.8  17.4
2020 01 15  000000  22 25 31.5  -54 35 48   4.047   3.423   45.0   11.7  17.4


C/2017 T2 (PANSTARRS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  04 56 19.4  +46 18 59   1.650   2.576  154.6    9.5  10.2
2019 12 02  000000  04 54 03.4  +46 41 40   1.640   2.566  154.6    9.5  10.2
2019 12 03  000000  04 51 43.6  +47 04 11   1.631   2.557  154.7    9.5  10.1
2019 12 04  000000  04 49 20.0  +47 26 31   1.622   2.548  154.6    9.6  10.1
2019 12 05  000000  04 46 52.6  +47 48 38   1.614   2.539  154.4    9.6  10.1
2019 12 06  000000  04 44 21.6  +48 10 31   1.606   2.529  154.2    9.8  10.1
2019 12 07  000000  04 41 47.0  +48 32 08   1.598   2.520  153.9    9.9  10.0
2019 12 08  000000  04 39 08.9  +48 53 27   1.591   2.511  153.5   10.1  10.0
2019 12 09  000000  04 36 27.3  +49 14 28   1.584   2.502  153.0   10.3  10.0
2019 12 10  000000  04 33 42.5  +49 35 09   1.577   2.493  152.5   10.5  10.0
2019 12 11  000000  04 30 54.4  +49 55 29   1.571   2.484  152.0   10.7   9.9
2019 12 12  000000  04 28 03.3  +50 15 25   1.565   2.474  151.3   11.0   9.9
2019 12 13  000000  04 25 09.3  +50 34 58   1.560   2.465  150.6   11.3   9.9
2019 12 14  000000  04 22 12.6  +50 54 05   1.555   2.456  149.9   11.6   9.9
2019 12 15  000000  04 19 13.2  +51 12 46   1.550   2.447  149.1   11.9   9.8
2019 12 16  000000  04 16 11.5  +51 30 59   1.546   2.438  148.2   12.3   9.8
2019 12 17  000000  04 13 07.6  +51 48 44   1.542   2.429  147.4   12.6   9.8
2019 12 18  000000  04 10 01.6  +52 05 59   1.538   2.420  146.5   13.0   9.8
2019 12 19  000000  04 06 53.9  +52 22 44   1.535   2.411  145.5   13.4   9.8
2019 12 20  000000  04 03 44.7  +52 38 58   1.532   2.402  144.6   13.7   9.7
2019 12 21  000000  04 00 34.1  +52 54 41   1.529   2.393  143.6   14.1   9.7
2019 12 22  000000  03 57 22.5  +53 09 52   1.527   2.384  142.5   14.5   9.7
2019 12 23  000000  03 54 10.1  +53 24 30   1.525   2.375  141.5   14.9   9.7
2019 12 24  000000  03 50 57.2  +53 38 37   1.524   2.366  140.4   15.3   9.7
2019 12 25  000000  03 47 44.0  +53 52 10   1.522   2.357  139.4   15.8   9.6
2019 12 26  000000  03 44 30.8  +54 05 12   1.521   2.349  138.3   16.2   9.6
2019 12 27  000000  03 41 18.0  +54 17 41   1.521   2.340  137.2   16.6   9.6
2019 12 28  000000  03 38 05.6  +54 29 38   1.520   2.331  136.1   17.0   9.6
2019 12 29  000000  03 34 54.1  +54 41 04   1.520   2.322  135.0   17.4   9.6
2019 12 30  000000  03 31 43.7  +54 51 59   1.520   2.313  133.9   17.8   9.6
2019 12 31  000000  03 28 34.6  +55 02 24   1.521   2.304  132.8   18.3   9.5
2020 01 01  000000  03 25 27.1  +55 12 19   1.521   2.296  131.6   18.7   9.5
2020 01 02  000000  03 22 21.5  +55 21 45   1.522   2.287  130.5   19.1   9.5
2020 01 03  000000  03 19 17.8  +55 30 44   1.524   2.278  129.4   19.5   9.5
2020 01 04  000000  03 16 16.5  +55 39 16   1.525   2.270  128.3   19.9   9.5
2020 01 05  000000  03 13 17.7  +55 47 23   1.527   2.261  127.2   20.3   9.5
2020 01 06  000000  03 10 21.5  +55 55 04   1.529   2.252  126.1   20.7   9.4
2020 01 07  000000  03 07 28.3  +56 02 23   1.531   2.244  124.9   21.1   9.4
2020 01 08  000000  03 04 38.0  +56 09 19   1.533   2.235  123.8   21.4   9.4
2020 01 09  000000  03 01 51.0  +56 15 54   1.536   2.227  122.7   21.8   9.4
2020 01 10  000000  02 59 07.4  +56 22 09   1.538   2.218  121.6   22.2   9.4
2020 01 11  000000  02 56 27.3  +56 28 06   1.541   2.210  120.5   22.5   9.4
2020 01 12  000000  02 53 50.8  +56 33 45   1.544   2.201  119.4   22.9   9.4
2020 01 13  000000  02 51 18.0  +56 39 08   1.547   2.193  118.4   23.2   9.4
2020 01 14  000000  02 48 49.2  +56 44 17   1.551   2.184  117.3   23.6   9.3
2020 01 15  000000  02 46 24.2  +56 49 12   1.554   2.176  116.2   23.9   9.3


C/2017 M4 (ATLAS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  14 21 24.2  -55 17 11   5.081   4.383   40.8    8.5  15.9
2019 12 02  000000  14 21 55.3  -55 28 54   5.082   4.389   41.2    8.5  16.0
2019 12 03  000000  14 22 26.0  -55 40 42   5.083   4.395   41.6    8.6  16.0
2019 12 04  000000  14 22 56.3  -55 52 34   5.083   4.401   42.0    8.6  16.0
2019 12 05  000000  14 23 26.1  -56 04 31   5.083   4.407   42.5    8.7  16.0
2019 12 06  000000  14 23 55.4  -56 16 33   5.083   4.413   42.9    8.7  16.0
2019 12 07  000000  14 24 24.3  -56 28 39   5.083   4.419   43.3    8.8  16.0
2019 12 08  000000  14 24 52.6  -56 40 50   5.083   4.424   43.8    8.9  16.0
2019 12 09  000000  14 25 20.4  -56 53 05   5.082   4.430   44.3    8.9  16.0
2019 12 10  000000  14 25 47.7  -57 05 25   5.082   4.436   44.7    9.0  16.0
2019 12 11  000000  14 26 14.3  -57 17 49   5.081   4.442   45.2    9.1  16.0
2019 12 12  000000  14 26 40.4  -57 30 18   5.080   4.448   45.7    9.1  16.0
2019 12 13  000000  14 27 05.8  -57 42 51   5.079   4.454   46.2    9.2  16.0
2019 12 14  000000  14 27 30.6  -57 55 29   5.077   4.460   46.7    9.2  16.0
2019 12 15  000000  14 27 54.8  -58 08 11   5.076   4.466   47.2    9.3  16.0
2019 12 16  000000  14 28 18.2  -58 20 57   5.074   4.472   47.7    9.4  16.0
2019 12 17  000000  14 28 40.9  -58 33 48   5.073   4.478   48.3    9.4  16.0
2019 12 18  000000  14 29 02.8  -58 46 44   5.071   4.484   48.8    9.5  16.0
2019 12 19  000000  14 29 24.0  -58 59 44   5.069   4.490   49.4    9.6  16.0
2019 12 20  000000  14 29 44.3  -59 12 48   5.067   4.497   49.9    9.6  16.1
2019 12 21  000000  14 30 03.8  -59 25 56   5.064   4.503   50.5    9.7  16.1
2019 12 22  000000  14 30 22.4  -59 39 09   5.062   4.509   51.0    9.8  16.1
2019 12 23  000000  14 30 40.1  -59 52 26   5.060   4.515   51.6    9.8  16.1
2019 12 24  000000  14 30 56.9  -60 05 47   5.057   4.521   52.2    9.9  16.1
2019 12 25  000000  14 31 12.6  -60 19 12   5.054   4.527   52.7   10.0  16.1
2019 12 26  000000  14 31 27.4  -60 32 41   5.051   4.533   53.3   10.0  16.1
2019 12 27  000000  14 31 41.0  -60 46 14   5.048   4.539   53.9   10.1  16.1
2019 12 28  000000  14 31 53.5  -60 59 51   5.045   4.545   54.5   10.1  16.1
2019 12 29  000000  14 32 04.9  -61 13 32   5.042   4.551   55.1   10.2  16.1
2019 12 30  000000  14 32 15.1  -61 27 17   5.038   4.557   55.7   10.3  16.1
2019 12 31  000000  14 32 24.1  -61 41 05   5.035   4.563   56.3   10.3  16.1
2020 01 01  000000  14 32 31.8  -61 54 57   5.031   4.569   56.9   10.4  16.1
2020 01 02  000000  14 32 38.1  -62 08 52   5.028   4.576   57.5   10.4  16.1
2020 01 03  000000  14 32 43.1  -62 22 51   5.024   4.582   58.1   10.5  16.1
2020 01 04  000000  14 32 46.7  -62 36 53   5.020   4.588   58.8   10.6  16.1
2020 01 05  000000  14 32 48.8  -62 50 59   5.016   4.594   59.4   10.6  16.1
2020 01 06  000000  14 32 49.4  -63 05 07   5.012   4.600   60.0   10.7  16.1
2020 01 07  000000  14 32 48.4  -63 19 19   5.008   4.606   60.6   10.7  16.1
2020 01 08  000000  14 32 45.7  -63 33 33   5.004   4.612   61.3   10.8  16.1
2020 01 09  000000  14 32 41.4  -63 47 51   5.000   4.619   61.9   10.8  16.1
2020 01 10  000000  14 32 35.4  -64 02 10   4.995   4.625   62.5   10.9  16.1
2020 01 11  000000  14 32 27.5  -64 16 33   4.991   4.631   63.2   10.9  16.1
2020 01 12  000000  14 32 17.8  -64 30 58   4.986   4.637   63.8   11.0  16.2
2020 01 13  000000  14 32 06.1  -64 45 25   4.982   4.643   64.4   11.0  16.2
2020 01 14  000000  14 31 52.5  -64 59 55   4.977   4.649   65.1   11.1  16.2
2020 01 15  000000  14 31 36.7  -65 14 26   4.973   4.656   65.7   11.1  16.2


C/2017 K2 (PANSTARRS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  17 32 45.7  +46 07 08  10.642  10.337   69.4    5.1  16.8
2019 12 02  000000  17 33 17.3  +46 04 31  10.637  10.330   69.4    5.1  16.8
2019 12 03  000000  17 33 49.0  +46 01 58  10.631  10.324   69.3    5.1  16.8
2019 12 04  000000  17 34 20.8  +45 59 30  10.625  10.317   69.2    5.1  16.8
2019 12 05  000000  17 34 52.7  +45 57 07  10.619  10.310   69.2    5.1  16.8
2019 12 06  000000  17 35 24.7  +45 54 49  10.613  10.303   69.1    5.1  16.8
2019 12 07  000000  17 35 56.8  +45 52 35  10.606  10.296   69.1    5.1  16.8
2019 12 08  000000  17 36 29.0  +45 50 26  10.600  10.289   69.1    5.1  16.8
2019 12 09  000000  17 37 01.3  +45 48 21  10.594  10.282   69.0    5.1  16.7
2019 12 10  000000  17 37 33.7  +45 46 22  10.587  10.275   69.0    5.1  16.7
2019 12 11  000000  17 38 06.2  +45 44 27  10.581  10.268   69.0    5.1  16.7
2019 12 12  000000  17 38 38.7  +45 42 37  10.574  10.262   68.9    5.1  16.7
2019 12 13  000000  17 39 11.3  +45 40 51  10.568  10.255   68.9    5.1  16.7
2019 12 14  000000  17 39 43.9  +45 39 11  10.561  10.248   68.9    5.1  16.7
2019 12 15  000000  17 40 16.6  +45 37 35  10.554  10.241   68.9    5.1  16.7
2019 12 16  000000  17 40 49.3  +45 36 04  10.547  10.234   68.9    5.1  16.7
2019 12 17  000000  17 41 22.1  +45 34 38  10.540  10.227   68.9    5.1  16.7
2019 12 18  000000  17 41 54.9  +45 33 17  10.533  10.220   68.9    5.2  16.7
2019 12 19  000000  17 42 27.7  +45 32 00  10.526  10.213   68.9    5.2  16.7
2019 12 20  000000  17 43 00.6  +45 30 49  10.519  10.206   68.9    5.2  16.7
2019 12 21  000000  17 43 33.4  +45 29 42  10.511  10.199   68.9    5.2  16.7
2019 12 22  000000  17 44 06.3  +45 28 41  10.504  10.192   69.0    5.2  16.7
2019 12 23  000000  17 44 39.2  +45 27 44  10.497  10.185   69.0    5.2  16.7
2019 12 24  000000  17 45 12.0  +45 26 52  10.489  10.178   69.0    5.2  16.7
2019 12 25  000000  17 45 44.9  +45 26 05  10.481  10.172   69.1    5.2  16.7
2019 12 26  000000  17 46 17.7  +45 25 23  10.474  10.165   69.1    5.2  16.7
2019 12 27  000000  17 46 50.4  +45 24 47  10.466  10.158   69.2    5.2  16.7
2019 12 28  000000  17 47 23.2  +45 24 15  10.458  10.151   69.2    5.2  16.7
2019 12 29  000000  17 47 55.9  +45 23 48  10.450  10.144   69.3    5.2  16.7
2019 12 30  000000  17 48 28.5  +45 23 26  10.442  10.137   69.3    5.2  16.7
2019 12 31  000000  17 49 01.1  +45 23 09  10.434  10.130   69.4    5.2  16.6
2020 01 01  000000  17 49 33.6  +45 22 57  10.426  10.123   69.5    5.2  16.6
2020 01 02  000000  17 50 06.1  +45 22 50  10.417  10.116   69.6    5.2  16.6
2020 01 03  000000  17 50 38.4  +45 22 47  10.409  10.109   69.6    5.2  16.6
2020 01 04  000000  17 51 10.7  +45 22 50  10.400  10.102   69.7    5.2  16.6
2020 01 05  000000  17 51 42.9  +45 22 58  10.392  10.095   69.8    5.2  16.6
2020 01 06  000000  17 52 14.9  +45 23 10  10.383  10.088   69.9    5.3  16.6
2020 01 07  000000  17 52 46.9  +45 23 27  10.375  10.081   70.0    5.3  16.6
2020 01 08  000000  17 53 18.7  +45 23 50  10.366  10.074   70.1    5.3  16.6
2020 01 09  000000  17 53 50.5  +45 24 17  10.357  10.067   70.3    5.3  16.6
2020 01 10  000000  17 54 22.0  +45 24 49  10.348  10.060   70.4    5.3  16.6
2020 01 11  000000  17 54 53.5  +45 25 26  10.339  10.053   70.5    5.3  16.6
2020 01 12  000000  17 55 24.8  +45 26 07  10.330  10.046   70.6    5.3  16.6
2020 01 13  000000  17 55 56.0  +45 26 54  10.321  10.039   70.7    5.3  16.6
2020 01 14  000000  17 56 27.0  +45 27 45  10.311  10.033   70.9    5.3  16.6
2020 01 15  000000  17 56 57.9  +45 28 41  10.302  10.026   71.0    5.3  16.6


C/2017 B3 (LINEAR)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  22 52 58.2  -30 59 46   4.684   4.693   84.5   12.1  16.1
2019 12 02  000000  22 53 10.1  -30 47 31   4.703   4.697   83.7   12.0  16.1
2019 12 03  000000  22 53 22.8  -30 35 18   4.722   4.702   82.8   12.0  16.1
2019 12 04  000000  22 53 36.2  -30 23 05   4.741   4.707   82.0   12.0  16.1
2019 12 05  000000  22 53 50.5  -30 10 54   4.760   4.711   81.2   11.9  16.1
2019 12 06  000000  22 54 05.5  -29 58 44   4.779   4.716   80.4   11.9  16.1
2019 12 07  000000  22 54 21.2  -29 46 35   4.798   4.720   79.6   11.8  16.1
2019 12 08  000000  22 54 37.7  -29 34 28   4.818   4.725   78.7   11.8  16.2
2019 12 09  000000  22 54 54.8  -29 22 22   4.837   4.730   77.9   11.7  16.2
2019 12 10  000000  22 55 12.7  -29 10 17   4.856   4.734   77.1   11.7  16.2
2019 12 11  000000  22 55 31.2  -28 58 14   4.875   4.739   76.3   11.6  16.2
2019 12 12  000000  22 55 50.4  -28 46 13   4.894   4.744   75.5   11.6  16.2
2019 12 13  000000  22 56 10.3  -28 34 12   4.913   4.748   74.6   11.5  16.2
2019 12 14  000000  22 56 30.8  -28 22 14   4.932   4.753   73.8   11.5  16.2
2019 12 15  000000  22 56 52.0  -28 10 17   4.951   4.758   73.0   11.4  16.2
2019 12 16  000000  22 57 13.8  -27 58 22   4.970   4.762   72.2   11.3  16.3
2019 12 17  000000  22 57 36.1  -27 46 28   4.989   4.767   71.4   11.3  16.3
2019 12 18  000000  22 57 59.1  -27 34 36   5.008   4.772   70.6   11.2  16.3
2019 12 19  000000  22 58 22.7  -27 22 46   5.027   4.776   69.8   11.1  16.3
2019 12 20  000000  22 58 46.8  -27 10 57   5.046   4.781   68.9   11.1  16.3
2019 12 21  000000  22 59 11.5  -26 59 10   5.064   4.786   68.1   11.0  16.3
2019 12 22  000000  22 59 36.8  -26 47 25   5.083   4.790   67.3   10.9  16.3
2019 12 23  000000  23 00 02.6  -26 35 42   5.102   4.795   66.5   10.8  16.3
2019 12 24  000000  23 00 29.0  -26 24 00   5.120   4.800   65.7   10.8  16.4
2019 12 25  000000  23 00 55.8  -26 12 21   5.139   4.805   64.9   10.7  16.4
2019 12 26  000000  23 01 23.2  -26 00 43   5.157   4.810   64.1   10.6  16.4
2019 12 27  000000  23 01 51.1  -25 49 07   5.176   4.814   63.3   10.5  16.4
2019 12 28  000000  23 02 19.4  -25 37 33   5.194   4.819   62.5   10.4  16.4
2019 12 29  000000  23 02 48.3  -25 26 01   5.212   4.824   61.7   10.3  16.4
2019 12 30  000000  23 03 17.6  -25 14 30   5.230   4.829   60.9   10.2  16.4
2019 12 31  000000  23 03 47.3  -25 03 02   5.248   4.833   60.1   10.2  16.4
2020 01 01  000000  23 04 17.5  -24 51 36   5.266   4.838   59.3   10.1  16.5
2020 01 02  000000  23 04 48.1  -24 40 11   5.284   4.843   58.5   10.0  16.5
2020 01 03  000000  23 05 19.2  -24 28 49   5.302   4.848   57.7    9.9  16.5
2020 01 04  000000  23 05 50.6  -24 17 28   5.320   4.853   56.9    9.8  16.5
2020 01 05  000000  23 06 22.5  -24 06 10   5.337   4.858   56.1    9.7  16.5
2020 01 06  000000  23 06 54.7  -23 54 54   5.355   4.862   55.3    9.6  16.5
2020 01 07  000000  23 07 27.3  -23 43 39   5.372   4.867   54.5    9.5  16.5
2020 01 08  000000  23 08 00.3  -23 32 27   5.390   4.872   53.7    9.4  16.5
2020 01 09  000000  23 08 33.6  -23 21 17   5.407   4.877   52.9    9.3  16.5
2020 01 10  000000  23 09 07.3  -23 10 09   5.424   4.882   52.1    9.1  16.6
2020 01 11  000000  23 09 41.3  -22 59 03   5.441   4.887   51.3    9.0  16.6
2020 01 12  000000  23 10 15.7  -22 47 59   5.458   4.892   50.5    8.9  16.6
2020 01 13  000000  23 10 50.4  -22 36 57   5.474   4.897   49.7    8.8  16.6
2020 01 14  000000  23 11 25.3  -22 25 57   5.491   4.902   49.0    8.7  16.6
2020 01 15  000000  23 12 00.6  -22 14 59   5.507   4.907   48.2    8.6  16.6


C/2016 M1 (PANSTARRS)
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  06 32 46.0  -34 34 52   4.866   5.375  116.2    9.5  15.7
2019 12 02  000000  06 31 49.8  -34 33 59   4.868   5.383  116.6    9.4  15.7
2019 12 03  000000  06 30 53.3  -34 32 54   4.870   5.391  117.1    9.4  15.8
2019 12 04  000000  06 29 56.3  -34 31 38   4.872   5.399  117.5    9.3  15.8
2019 12 05  000000  06 28 59.0  -34 30 11   4.875   5.407  117.9    9.3  15.8
2019 12 06  000000  06 28 01.3  -34 28 31   4.877   5.415  118.3    9.2  15.8
2019 12 07  000000  06 27 03.4  -34 26 40   4.880   5.423  118.7    9.2  15.8
2019 12 08  000000  06 26 05.2  -34 24 38   4.883   5.431  119.1    9.1  15.8
2019 12 09  000000  06 25 06.7  -34 22 23   4.886   5.439  119.5    9.1  15.8
2019 12 10  000000  06 24 08.1  -34 19 57   4.890   5.447  119.8    9.0  15.8
2019 12 11  000000  06 23 09.3  -34 17 19   4.893   5.455  120.2    9.0  15.8
2019 12 12  000000  06 22 10.3  -34 14 29   4.897   5.463  120.5    8.9  15.8
2019 12 13  000000  06 21 11.2  -34 11 27   4.901   5.471  120.8    8.9  15.8
2019 12 14  000000  06 20 12.0  -34 08 13   4.905   5.479  121.1    8.8  15.8
2019 12 15  000000  06 19 12.8  -34 04 48   4.910   5.487  121.4    8.8  15.8
2019 12 16  000000  06 18 13.6  -34 01 10   4.915   5.495  121.7    8.8  15.9
2019 12 17  000000  06 17 14.3  -33 57 21   4.919   5.503  121.9    8.7  15.9
2019 12 18  000000  06 16 15.1  -33 53 19   4.925   5.511  122.1    8.7  15.9
2019 12 19  000000  06 15 16.0  -33 49 06   4.930   5.519  122.3    8.7  15.9
2019 12 20  000000  06 14 17.0  -33 44 41   4.935   5.527  122.5    8.6  15.9
2019 12 21  000000  06 13 18.1  -33 40 05   4.941   5.535  122.7    8.6  15.9
2019 12 22  000000  06 12 19.3  -33 35 16   4.947   5.543  122.9    8.6  15.9
2019 12 23  000000  06 11 20.8  -33 30 16   4.953   5.551  123.0    8.5  15.9
2019 12 24  000000  06 10 22.5  -33 25 04   4.960   5.559  123.2    8.5  15.9
2019 12 25  000000  06 09 24.4  -33 19 41   4.967   5.567  123.3    8.5  15.9
2019 12 26  000000  06 08 26.6  -33 14 07   4.974   5.575  123.4    8.5  15.9
2019 12 27  000000  06 07 29.1  -33 08 21   4.981   5.583  123.4    8.5  16.0
2019 12 28  000000  06 06 32.0  -33 02 24   4.988   5.591  123.5    8.4  16.0
2019 12 29  000000  06 05 35.3  -32 56 16   4.996   5.599  123.5    8.4  16.0
2019 12 30  000000  06 04 39.0  -32 49 57   5.004   5.607  123.6    8.4  16.0
2019 12 31  000000  06 03 43.1  -32 43 27   5.012   5.615  123.5    8.4  16.0
2020 01 01  000000  06 02 47.6  -32 36 47   5.020   5.623  123.5    8.4  16.0
2020 01 02  000000  06 01 52.7  -32 29 56   5.029   5.631  123.5    8.4  16.0
2020 01 03  000000  06 00 58.2  -32 22 55   5.037   5.639  123.4    8.4  16.0
2020 01 04  000000  06 00 04.3  -32 15 45   5.047   5.647  123.4    8.4  16.0
2020 01 05  000000  05 59 11.0  -32 08 24   5.056   5.655  123.3    8.4  16.0
2020 01 06  000000  05 58 18.2  -32 00 53   5.065   5.663  123.2    8.4  16.1
2020 01 07  000000  05 57 26.0  -31 53 14   5.075   5.671  123.0    8.4  16.1
2020 01 08  000000  05 56 34.5  -31 45 25   5.085   5.679  122.9    8.4  16.1
2020 01 09  000000  05 55 43.6  -31 37 27   5.095   5.687  122.7    8.4  16.1
2020 01 10  000000  05 54 53.4  -31 29 20   5.106   5.695  122.5    8.4  16.1
2020 01 11  000000  05 54 03.8  -31 21 04   5.116   5.703  122.3    8.4  16.1
2020 01 12  000000  05 53 15.0  -31 12 41   5.127   5.711  122.1    8.4  16.1
2020 01 13  000000  05 52 26.9  -31 04 09   5.139   5.719  121.9    8.4  16.1
2020 01 14  000000  05 51 39.4  -30 55 29   5.150   5.727  121.6    8.4  16.1
2020 01 15  000000  05 50 52.8  -30 46 41   5.162   5.735  121.3    8.4  16.1


260P/McNaught
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  02 23 42.7  +48 34 36   0.779   1.679  143.8   20.3  15.2
2019 12 02  000000  02 23 51.1  +48 26 00   0.787   1.685  143.4   20.4  15.2
2019 12 03  000000  02 24 02.4  +48 17 14   0.795   1.690  143.1   20.5  15.3
2019 12 04  000000  02 24 16.5  +48 08 17   0.803   1.696  142.7   20.6  15.3
2019 12 05  000000  02 24 33.5  +47 59 11   0.812   1.702  142.3   20.7  15.4
2019 12 06  000000  02 24 53.3  +47 49 58   0.820   1.708  141.9   20.9  15.4
2019 12 07  000000  02 25 15.9  +47 40 37   0.829   1.713  141.5   21.0  15.4
2019 12 08  000000  02 25 41.1  +47 31 10   0.838   1.719  141.0   21.1  15.5
2019 12 09  000000  02 26 09.0  +47 21 39   0.847   1.725  140.6   21.3  15.5
2019 12 10  000000  02 26 39.6  +47 12 03   0.856   1.731  140.1   21.4  15.5
2019 12 11  000000  02 27 12.7  +47 02 24   0.865   1.737  139.7   21.5  15.6
2019 12 12  000000  02 27 48.4  +46 52 42   0.875   1.743  139.2   21.7  15.6
2019 12 13  000000  02 28 26.5  +46 42 58   0.884   1.749  138.7   21.8  15.7
2019 12 14  000000  02 29 07.0  +46 33 13   0.894   1.755  138.2   22.0  15.7
2019 12 15  000000  02 29 49.8  +46 23 28   0.904   1.761  137.7   22.1  15.7
2019 12 16  000000  02 30 35.0  +46 13 42   0.914   1.767  137.1   22.3  15.8
2019 12 17  000000  02 31 22.4  +46 03 57   0.924   1.773  136.6   22.4  15.8
2019 12 18  000000  02 32 12.0  +45 54 14   0.934   1.779  136.1   22.6  15.9
2019 12 19  000000  02 33 03.8  +45 44 31   0.945   1.786  135.5   22.7  15.9
2019 12 20  000000  02 33 57.7  +45 34 51   0.956   1.792  135.0   22.9  15.9
2019 12 21  000000  02 34 53.6  +45 25 14   0.966   1.798  134.4   23.0  16.0
2019 12 22  000000  02 35 51.5  +45 15 40   0.977   1.804  133.9   23.1  16.0
2019 12 23  000000  02 36 51.5  +45 06 09   0.988   1.810  133.3   23.3  16.1
2019 12 24  000000  02 37 53.3  +44 56 42   1.000   1.817  132.7   23.4  16.1
2019 12 25  000000  02 38 57.0  +44 47 19   1.011   1.823  132.1   23.6  16.1
2019 12 26  000000  02 40 02.6  +44 38 01   1.022   1.829  131.6   23.7  16.2
2019 12 27  000000  02 41 09.9  +44 28 49   1.034   1.836  131.0   23.9  16.2
2019 12 28  000000  02 42 19.0  +44 19 41   1.046   1.842  130.4   24.0  16.3
2019 12 29  000000  02 43 29.8  +44 10 39   1.058   1.849  129.8   24.1  16.3
2019 12 30  000000  02 44 42.2  +44 01 43   1.070   1.855  129.2   24.3  16.3
2019 12 31  000000  02 45 56.2  +43 52 54   1.082   1.861  128.6   24.4  16.4
2020 01 01  000000  02 47 11.8  +43 44 10   1.094   1.868  128.0   24.5  16.4
2020 01 02  000000  02 48 28.9  +43 35 33   1.107   1.874  127.4   24.6  16.4
2020 01 03  000000  02 49 47.4  +43 27 03   1.119   1.881  126.8   24.8  16.5
2020 01 04  000000  02 51 07.3  +43 18 39   1.132   1.887  126.2   24.9  16.5
2020 01 05  000000  02 52 28.6  +43 10 22   1.145   1.894  125.5   25.0  16.6
2020 01 06  000000  02 53 51.2  +43 02 13   1.158   1.900  124.9   25.1  16.6
2020 01 07  000000  02 55 15.0  +42 54 10   1.171   1.907  124.3   25.2  16.6
2020 01 08  000000  02 56 40.1  +42 46 14   1.184   1.914  123.7   25.3  16.7
2020 01 09  000000  02 58 06.4  +42 38 25   1.198   1.920  123.1   25.4  16.7
2020 01 10  000000  02 59 33.8  +42 30 43   1.211   1.927  122.5   25.5  16.8
2020 01 11  000000  03 01 02.3  +42 23 07   1.225   1.933  121.8   25.6  16.8
2020 01 12  000000  03 02 31.8  +42 15 39   1.239   1.940  121.2   25.7  16.8
2020 01 13  000000  03 04 02.4  +42 08 18   1.253   1.947  120.6   25.8  16.9
2020 01 14  000000  03 05 34.0  +42 01 03   1.267   1.953  120.0   25.9  16.9
2020 01 15  000000  03 07 06.5  +41 53 55   1.281   1.960  119.3   25.9  17.0


289P/Blanpain
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  22 30 29.5  -15 58 11   0.275   1.002   85.2   78.9  16.2
2019 12 02  000000  22 31 23.2  -15 29 03   0.270   0.997   84.6   79.8  16.1
2019 12 03  000000  22 32 19.3  -14 58 44   0.265   0.994   84.0   80.6  16.1
2019 12 04  000000  22 33 17.5  -14 27 12   0.260   0.990   83.4   81.5  16.0
2019 12 05  000000  22 34 18.1  -13 54 22   0.255   0.986   82.8   82.4  16.0
2019 12 06  000000  22 35 20.8  -13 20 09   0.250   0.983   82.2   83.2  15.9
2019 12 07  000000  22 36 25.8  -12 44 28   0.245   0.980   81.7   84.0  15.9
2019 12 08  000000  22 37 33.0  -12 07 13   0.239   0.977   81.1   84.9  15.8
2019 12 09  000000  22 38 42.5  -11 28 19   0.234   0.975   80.6   85.7  15.7
2019 12 10  000000  22 39 54.2  -10 47 38   0.229   0.972   80.1   86.5  15.7
2019 12 11  000000  22 41 08.3  -10 05 02   0.223   0.970   79.7   87.3  15.6
2019 12 12  000000  22 42 24.7  -09 20 23   0.218   0.968   79.2   88.0  15.5
2019 12 13  000000  22 43 43.7  -08 33 32   0.212   0.966   78.8   88.8  15.5
2019 12 14  000000  22 45 05.3  -07 44 19   0.207   0.964   78.4   89.5  15.4
2019 12 15  000000  22 46 29.7  -06 52 32   0.201   0.963   78.0   90.2  15.4
2019 12 16  000000  22 47 57.1  -05 57 59   0.196   0.962   77.7   90.8  15.3
2019 12 17  000000  22 49 27.7  -05 00 26   0.190   0.961   77.4   91.5  15.2
2019 12 18  000000  22 51 01.8  -03 59 37   0.185   0.960   77.1   92.1  15.2
2019 12 19  000000  22 52 39.7  -02 55 16   0.179   0.959   76.9   92.6  15.1
2019 12 20  000000  22 54 22.0  -01 47 03   0.174   0.959   76.7   93.1  15.0
2019 12 21  000000  22 56 09.0  -00 34 38   0.169   0.959   76.6   93.5  15.0
2019 12 22  000000  22 58 01.2  +00 42 21   0.163   0.959   76.6   93.9  14.9
2019 12 23  000000  22 59 59.4  +02 04 21   0.158   0.959   76.6   94.2  14.8
2019 12 24  000000  23 02 04.2  +03 31 49   0.153   0.960   76.6   94.5  14.7
2019 12 25  000000  23 04 16.5  +05 05 15   0.147   0.961   76.8   94.6  14.7
2019 12 26  000000  23 06 37.4  +06 45 11   0.142   0.962   77.0   94.7  14.6
2019 12 27  000000  23 09 07.9  +08 32 12   0.137   0.963   77.4   94.6  14.5
2019 12 28  000000  23 11 49.5  +10 26 55   0.133   0.964   77.9   94.4  14.5
2019 12 29  000000  23 14 43.9  +12 29 58   0.128   0.966   78.4   94.1  14.4
2019 12 30  000000  23 17 53.0  +14 42 01   0.123   0.968   79.2   93.7  14.3
2019 12 31  000000  23 21 19.2  +17 03 42   0.119   0.970   80.0   93.0  14.2
2020 01 01  000000  23 25 05.4  +19 35 37   0.115   0.972   81.1   92.2  14.2
2020 01 02  000000  23 29 15.2  +22 18 17   0.111   0.975   82.3   91.3  14.1
2020 01 03  000000  23 33 52.8  +25 12 03   0.107   0.977   83.7   90.1  14.0
2020 01 04  000000  23 39 03.7  +28 17 03   0.104   0.980   85.3   88.7  14.0
2020 01 05  000000  23 44 54.6  +31 33 06   0.100   0.983   87.1   87.1  13.9
2020 01 06  000000  23 51 33.9  +34 59 36   0.098   0.987   89.1   85.2  13.9
2020 01 07  000000  23 59 12.4  +38 35 24   0.095   0.990   91.3   83.2  13.9
2020 01 08  000000  00 08 03.9  +42 18 45   0.094   0.994   93.7   80.9  13.8
2020 01 09  000000  00 18 26.1  +46 07 08   0.092   0.998   96.3   78.5  13.8
2020 01 10  000000  00 30 41.8  +49 57 20   0.091   1.002   99.0   75.9  13.8
2020 01 11  000000  00 45 20.4  +53 45 14   0.091   1.006  101.8   73.1  13.8
2020 01 12  000000  01 02 58.7  +57 26 00   0.091   1.010  104.6   70.4  13.8
2020 01 13  000000  01 24 21.6  +60 53 58   0.092   1.015  107.5   67.5  13.9
2020 01 14  000000  01 50 17.8  +64 02 44   0.093   1.020  110.4   64.7  13.9
2020 01 15  000000  02 21 30.1  +66 45 16   0.094   1.024  113.2   61.9  14.0


246P/NEAT
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  12 34 01.4  +12 28 08   3.915   3.633   66.3   14.4  19.1
2019 12 02  000000  12 35 00.5  +12 25 02   3.899   3.630   67.0   14.5  19.1
2019 12 03  000000  12 35 59.2  +12 22 01   3.883   3.627   67.8   14.6  19.0
2019 12 04  000000  12 36 57.5  +12 19 05   3.868   3.625   68.5   14.7  19.0
2019 12 05  000000  12 37 55.4  +12 16 14   3.852   3.622   69.3   14.7  19.0
2019 12 06  000000  12 38 52.8  +12 13 29   3.836   3.620   70.0   14.8  19.0
2019 12 07  000000  12 39 49.8  +12 10 49   3.820   3.617   70.8   14.9  19.0
2019 12 08  000000  12 40 46.4  +12 08 14   3.804   3.615   71.5   15.0  19.0
2019 12 09  000000  12 41 42.5  +12 05 45   3.788   3.612   72.3   15.1  19.0
2019 12 10  000000  12 42 38.1  +12 03 22   3.772   3.610   73.1   15.1  19.0
2019 12 11  000000  12 43 33.3  +12 01 04   3.755   3.607   73.8   15.2  18.9
2019 12 12  000000  12 44 27.9  +11 58 51   3.739   3.604   74.6   15.3  18.9
2019 12 13  000000  12 45 22.1  +11 56 45   3.723   3.602   75.3   15.3  18.9
2019 12 14  000000  12 46 15.8  +11 54 44   3.706   3.599   76.1   15.4  18.9
2019 12 15  000000  12 47 09.0  +11 52 49   3.690   3.597   76.9   15.5  18.9
2019 12 16  000000  12 48 01.7  +11 50 59   3.674   3.594   77.7   15.5  18.9
2019 12 17  000000  12 48 53.8  +11 49 16   3.657   3.592   78.4   15.6  18.9
2019 12 18  000000  12 49 45.4  +11 47 39   3.641   3.589   79.2   15.6  18.9
2019 12 19  000000  12 50 36.4  +11 46 08   3.624   3.586   80.0   15.7  18.8
2019 12 20  000000  12 51 26.9  +11 44 43   3.608   3.584   80.8   15.7  18.8
2019 12 21  000000  12 52 16.8  +11 43 24   3.591   3.581   81.6   15.8  18.8
2019 12 22  000000  12 53 06.1  +11 42 12   3.574   3.579   82.3   15.8  18.8
2019 12 23  000000  12 53 54.8  +11 41 06   3.558   3.576   83.1   15.8  18.8
2019 12 24  000000  12 54 42.9  +11 40 06   3.541   3.574   83.9   15.9  18.8
2019 12 25  000000  12 55 30.3  +11 39 13   3.525   3.571   84.7   15.9  18.8
2019 12 26  000000  12 56 17.2  +11 38 27   3.508   3.569   85.5   15.9  18.8
2019 12 27  000000  12 57 03.3  +11 37 47   3.491   3.566   86.3   16.0  18.7
2019 12 28  000000  12 57 48.8  +11 37 13   3.475   3.563   87.1   16.0  18.7
2019 12 29  000000  12 58 33.7  +11 36 47   3.458   3.561   87.9   16.0  18.7
2019 12 30  000000  12 59 17.8  +11 36 27   3.441   3.558   88.8   16.0  18.7
2019 12 31  000000  13 00 01.3  +11 36 13   3.425   3.556   89.6   16.1  18.7
2020 01 01  000000  13 00 44.0  +11 36 07   3.408   3.553   90.4   16.1  18.7
2020 01 02  000000  13 01 26.0  +11 36 07   3.391   3.551   91.2   16.1  18.7
2020 01 03  000000  13 02 07.3  +11 36 15   3.375   3.548   92.0   16.1  18.6
2020 01 04  000000  13 02 47.8  +11 36 29   3.358   3.546   92.9   16.1  18.6
2020 01 05  000000  13 03 27.6  +11 36 50   3.341   3.543   93.7   16.1  18.6
2020 01 06  000000  13 04 06.6  +11 37 17   3.325   3.541   94.5   16.1  18.6
2020 01 07  000000  13 04 44.9  +11 37 52   3.308   3.538   95.3   16.1  18.6
2020 01 08  000000  13 05 22.4  +11 38 34   3.292   3.535   96.2   16.1  18.6
2020 01 09  000000  13 05 59.0  +11 39 23   3.275   3.533   97.0   16.0  18.6
2020 01 10  000000  13 06 34.8  +11 40 19   3.259   3.530   97.9   16.0  18.5
2020 01 11  000000  13 07 09.9  +11 41 22   3.243   3.528   98.7   16.0  18.5
2020 01 12  000000  13 07 44.0  +11 42 31   3.226   3.525   99.5   16.0  18.5
2020 01 13  000000  13 08 17.4  +11 43 48   3.210   3.523  100.4   15.9  18.5
2020 01 14  000000  13 08 49.8  +11 45 12   3.194   3.520  101.3   15.9  18.5
2020 01 15  000000  13 09 21.4  +11 46 44   3.177   3.518  102.1   15.9  18.5


160P/LINEAR
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  21 04 25.5  -13 38 39   1.938   1.787   66.3   30.4  18.2
2019 12 02  000000  21 06 39.2  -13 21 55   1.946   1.787   65.9   30.2  18.2
2019 12 03  000000  21 08 53.1  -13 05 07   1.954   1.787   65.5   30.1  18.2
2019 12 04  000000  21 11 07.2  -12 48 15   1.962   1.787   65.1   30.0  18.2
2019 12 05  000000  21 13 21.4  -12 31 20   1.970   1.788   64.7   29.9  18.2
2019 12 06  000000  21 15 35.7  -12 14 21   1.979   1.788   64.3   29.8  18.2
2019 12 07  000000  21 17 50.2  -11 57 19   1.987   1.788   63.9   29.7  18.3
2019 12 08  000000  21 20 04.8  -11 40 13   1.995   1.788   63.5   29.5  18.3
2019 12 09  000000  21 22 19.5  -11 23 04   2.003   1.788   63.1   29.4  18.3
2019 12 10  000000  21 24 34.3  -11 05 52   2.011   1.789   62.7   29.3  18.3
2019 12 11  000000  21 26 49.2  -10 48 37   2.020   1.789   62.3   29.2  18.3
2019 12 12  000000  21 29 04.2  -10 31 18   2.028   1.790   61.9   29.0  18.3
2019 12 13  000000  21 31 19.3  -10 13 57   2.036   1.790   61.5   28.9  18.3
2019 12 14  000000  21 33 34.5  -09 56 32   2.045   1.791   61.1   28.8  18.3
2019 12 15  000000  21 35 49.7  -09 39 05   2.053   1.791   60.8   28.6  18.3
2019 12 16  000000  21 38 05.0  -09 21 34   2.061   1.792   60.4   28.5  18.3
2019 12 17  000000  21 40 20.4  -09 04 01   2.070   1.793   60.0   28.4  18.3
2019 12 18  000000  21 42 35.9  -08 46 25   2.078   1.793   59.6   28.2  18.4
2019 12 19  000000  21 44 51.4  -08 28 47   2.086   1.794   59.2   28.1  18.4
2019 12 20  000000  21 47 06.9  -08 11 05   2.095   1.795   58.8   28.0  18.4
2019 12 21  000000  21 49 22.6  -07 53 22   2.103   1.796   58.4   27.8  18.4
2019 12 22  000000  21 51 38.2  -07 35 35   2.112   1.797   58.1   27.7  18.4
2019 12 23  000000  21 53 54.0  -07 17 47   2.120   1.798   57.7   27.5  18.4
2019 12 24  000000  21 56 09.8  -06 59 56   2.128   1.799   57.3   27.4  18.4
2019 12 25  000000  21 58 25.6  -06 42 03   2.137   1.800   56.9   27.3  18.4
2019 12 26  000000  22 00 41.4  -06 24 08   2.145   1.801   56.5   27.1  18.4
2019 12 27  000000  22 02 57.3  -06 06 10   2.154   1.802   56.2   27.0  18.4
2019 12 28  000000  22 05 13.2  -05 48 11   2.162   1.803   55.8   26.8  18.5
2019 12 29  000000  22 07 29.2  -05 30 10   2.171   1.805   55.4   26.7  18.5
2019 12 30  000000  22 09 45.1  -05 12 07   2.180   1.806   55.0   26.5  18.5
2019 12 31  000000  22 12 01.1  -04 54 02   2.188   1.807   54.7   26.4  18.5
2020 01 01  000000  22 14 17.1  -04 35 56   2.197   1.809   54.3   26.2  18.5
2020 01 02  000000  22 16 33.1  -04 17 48   2.205   1.810   53.9   26.0  18.5
2020 01 03  000000  22 18 49.0  -03 59 39   2.214   1.812   53.6   25.9  18.5
2020 01 04  000000  22 21 05.0  -03 41 29   2.223   1.813   53.2   25.7  18.5
2020 01 05  000000  22 23 21.0  -03 23 18   2.231   1.815   52.8   25.6  18.5
2020 01 06  000000  22 25 36.9  -03 05 05   2.240   1.816   52.4   25.4  18.5
2020 01 07  000000  22 27 52.9  -02 46 51   2.248   1.818   52.1   25.3  18.6
2020 01 08  000000  22 30 08.8  -02 28 37   2.257   1.820   51.7   25.1  18.6
2020 01 09  000000  22 32 24.7  -02 10 22   2.266   1.821   51.3   24.9  18.6
2020 01 10  000000  22 34 40.6  -01 52 06   2.275   1.823   51.0   24.8  18.6
2020 01 11  000000  22 36 56.5  -01 33 50   2.283   1.825   50.6   24.6  18.6
2020 01 12  000000  22 39 12.4  -01 15 33   2.292   1.827   50.3   24.4  18.6
2020 01 13  000000  22 41 28.2  -00 57 16   2.301   1.829   49.9   24.3  18.6
2020 01 14  000000  22 43 44.1  -00 38 59   2.309   1.831   49.5   24.1  18.6
2020 01 15  000000  22 45 59.9  -00 20 41   2.318   1.833   49.2   24.0  18.6


155P/Shoemaker
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  10 25 06.0  +13 18 16   1.434   1.810   95.0   32.9  13.9
2019 12 02  000000  10 27 01.1  +13 12 53   1.427   1.811   95.6   32.8  13.9
2019 12 03  000000  10 28 55.0  +13 07 37   1.419   1.813   96.1   32.7  13.9
2019 12 04  000000  10 30 47.6  +13 02 28   1.412   1.814   96.7   32.7  13.9
2019 12 05  000000  10 32 38.9  +12 57 26   1.405   1.815   97.3   32.6  13.8
2019 12 06  000000  10 34 29.0  +12 52 32   1.398   1.816   97.8   32.5  13.8
2019 12 07  000000  10 36 17.6  +12 47 46   1.391   1.818   98.4   32.4  13.8
2019 12 08  000000  10 38 04.9  +12 43 08   1.384   1.819   99.0   32.3  13.8
2019 12 09  000000  10 39 50.9  +12 38 38   1.377   1.821   99.6   32.2  13.8
2019 12 10  000000  10 41 35.4  +12 34 16   1.370   1.822  100.1   32.1  13.8
2019 12 11  000000  10 43 18.5  +12 30 03   1.363   1.824  100.7   32.0  13.8
2019 12 12  000000  10 45 00.2  +12 25 59   1.356   1.826  101.3   31.9  13.8
2019 12 13  000000  10 46 40.4  +12 22 05   1.349   1.828  102.0   31.8  13.8
2019 12 14  000000  10 48 19.1  +12 18 19   1.342   1.829  102.6   31.7  13.8
2019 12 15  000000  10 49 56.3  +12 14 44   1.336   1.831  103.2   31.6  13.8
2019 12 16  000000  10 51 32.0  +12 11 18   1.329   1.833  103.8   31.4  13.8
2019 12 17  000000  10 53 06.0  +12 08 02   1.323   1.835  104.5   31.3  13.8
2019 12 18  000000  10 54 38.5  +12 04 56   1.316   1.837  105.1   31.1  13.8
2019 12 19  000000  10 56 09.4  +12 02 01   1.310   1.840  105.8   31.0  13.8
2019 12 20  000000  10 57 38.6  +11 59 17   1.304   1.842  106.4   30.8  13.8
2019 12 21  000000  10 59 06.2  +11 56 44   1.297   1.844  107.1   30.7  13.8
2019 12 22  000000  11 00 32.0  +11 54 22   1.291   1.846  107.8   30.5  13.8
2019 12 23  000000  11 01 56.1  +11 52 11   1.285   1.849  108.4   30.3  13.7
2019 12 24  000000  11 03 18.4  +11 50 12   1.279   1.851  109.1   30.1  13.7
2019 12 25  000000  11 04 39.0  +11 48 24   1.273   1.854  109.8   29.9  13.7
2019 12 26  000000  11 05 57.7  +11 46 49   1.267   1.856  110.5   29.7  13.7
2019 12 27  000000  11 07 14.6  +11 45 25   1.261   1.859  111.2   29.5  13.7
2019 12 28  000000  11 08 29.7  +11 44 14   1.255   1.862  112.0   29.3  13.7
2019 12 29  000000  11 09 42.9  +11 43 15   1.249   1.864  112.7   29.1  13.7
2019 12 30  000000  11 10 54.2  +11 42 28   1.244   1.867  113.4   28.9  13.7
2019 12 31  000000  11 12 03.5  +11 41 54   1.238   1.870  114.2   28.7  13.7
2020 01 01  000000  11 13 11.0  +11 41 32   1.233   1.873  114.9   28.4  13.7
2020 01 02  000000  11 14 16.5  +11 41 23   1.227   1.876  115.7   28.2  13.7
2020 01 03  000000  11 15 20.0  +11 41 26   1.222   1.879  116.4   27.9  13.7
2020 01 04  000000  11 16 21.5  +11 41 43   1.217   1.882  117.2   27.7  13.7
2020 01 05  000000  11 17 21.0  +11 42 12   1.212   1.885  118.0   27.4  13.7
2020 01 06  000000  11 18 18.5  +11 42 53   1.206   1.888  118.8   27.1  13.7
2020 01 07  000000  11 19 14.0  +11 43 48   1.202   1.891  119.6   26.9  13.7
2020 01 08  000000  11 20 07.4  +11 44 55   1.197   1.895  120.4   26.6  13.7
2020 01 09  000000  11 20 58.7  +11 46 15   1.192   1.898  121.2   26.3  13.7
2020 01 10  000000  11 21 48.0  +11 47 48   1.187   1.902  122.1   26.0  13.7
2020 01 11  000000  11 22 35.1  +11 49 34   1.183   1.905  122.9   25.7  13.7
2020 01 12  000000  11 23 20.1  +11 51 32   1.178   1.908  123.7   25.4  13.7
2020 01 13  000000  11 24 03.0  +11 53 43   1.174   1.912  124.6   25.1  13.7
2020 01 14  000000  11 24 43.8  +11 56 06   1.170   1.916  125.5   24.7  13.7
2020 01 15  000000  11 25 22.4  +11 58 42   1.166   1.919  126.3   24.4  13.7


114P/Wiseman-Skiff
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  02 13 08.5  +38 11 10   0.723   1.641  147.1   19.0  14.0
2019 12 02  000000  02 13 30.2  +37 47 27   0.723   1.639  146.6   19.3  14.0
2019 12 03  000000  02 13 54.8  +37 23 29   0.723   1.636  146.1   19.7  14.0
2019 12 04  000000  02 14 22.2  +36 59 20   0.723   1.633  145.5   20.0  14.0
2019 12 05  000000  02 14 52.4  +36 35 00   0.723   1.631  145.0   20.3  14.0
2019 12 06  000000  02 15 25.4  +36 10 32   0.723   1.628  144.4   20.6  14.0
2019 12 07  000000  02 16 01.2  +35 45 56   0.723   1.626  143.8   21.0  14.0
2019 12 08  000000  02 16 39.8  +35 21 15   0.724   1.624  143.1   21.3  14.0
2019 12 09  000000  02 17 21.2  +34 56 30   0.725   1.621  142.5   21.7  13.9
2019 12 10  000000  02 18 05.4  +34 31 42   0.726   1.619  141.9   22.1  13.9
2019 12 11  000000  02 18 52.2  +34 06 52   0.727   1.617  141.2   22.4  13.9
2019 12 12  000000  02 19 41.8  +33 42 04   0.728   1.615  140.5   22.8  13.9
2019 12 13  000000  02 20 34.1  +33 17 16   0.730   1.613  139.9   23.2  13.9
2019 12 14  000000  02 21 29.1  +32 52 32   0.732   1.611  139.2   23.5  13.9
2019 12 15  000000  02 22 26.6  +32 27 51   0.734   1.609  138.5   23.9  13.9
2019 12 16  000000  02 23 26.7  +32 03 16   0.736   1.607  137.8   24.3  13.9
2019 12 17  000000  02 24 29.4  +31 38 48   0.738   1.605  137.1   24.7  13.9
2019 12 18  000000  02 25 34.6  +31 14 28   0.740   1.603  136.4   25.1  13.9
2019 12 19  000000  02 26 42.2  +30 50 16   0.743   1.602  135.7   25.4  13.9
2019 12 20  000000  02 27 52.3  +30 26 14   0.745   1.600  134.9   25.8  13.9
2019 12 21  000000  02 29 04.9  +30 02 24   0.748   1.598  134.2   26.2  13.9
2019 12 22  000000  02 30 19.8  +29 38 45   0.751   1.597  133.5   26.5  13.9
2019 12 23  000000  02 31 37.0  +29 15 20   0.754   1.595  132.8   26.9  13.9
2019 12 24  000000  02 32 56.5  +28 52 09   0.758   1.594  132.1   27.3  13.9
2019 12 25  000000  02 34 18.3  +28 29 12   0.761   1.593  131.3   27.6  13.9
2019 12 26  000000  02 35 42.3  +28 06 31   0.765   1.591  130.6   28.0  13.9
2019 12 27  000000  02 37 08.5  +27 44 07   0.769   1.590  129.9   28.3  14.0
2019 12 28  000000  02 38 36.8  +27 22 00   0.773   1.589  129.2   28.7  14.0
2019 12 29  000000  02 40 07.2  +27 00 10   0.777   1.588  128.5   29.0  14.0
2019 12 30  000000  02 41 39.7  +26 38 39   0.781   1.587  127.8   29.3  14.0
2019 12 31  000000  02 43 14.1  +26 17 26   0.786   1.586  127.1   29.7  14.0
2020 01 01  000000  02 44 50.4  +25 56 33   0.790   1.585  126.4   30.0  14.0
2020 01 02  000000  02 46 28.7  +25 35 59   0.795   1.584  125.7   30.3  14.0
2020 01 03  000000  02 48 08.8  +25 15 46   0.800   1.583  125.0   30.6  14.0
2020 01 04  000000  02 49 50.6  +24 55 52   0.805   1.583  124.3   30.9  14.0
2020 01 05  000000  02 51 34.2  +24 36 19   0.810   1.582  123.6   31.2  14.0
2020 01 06  000000  02 53 19.4  +24 17 07   0.815   1.582  122.9   31.5  14.0
2020 01 07  000000  02 55 06.3  +23 58 15   0.820   1.581  122.2   31.7  14.1
2020 01 08  000000  02 56 54.8  +23 39 44   0.826   1.581  121.5   32.0  14.1
2020 01 09  000000  02 58 44.8  +23 21 34   0.831   1.580  120.9   32.3  14.1
2020 01 10  000000  03 00 36.2  +23 03 45   0.837   1.580  120.2   32.5  14.1
2020 01 11  000000  03 02 29.1  +22 46 16   0.843   1.580  119.6   32.8  14.1
2020 01 12  000000  03 04 23.4  +22 29 08   0.849   1.580  118.9   33.0  14.1
2020 01 13  000000  03 06 18.9  +22 12 21   0.855   1.579  118.3   33.3  14.1
2020 01 14  000000  03 08 15.8  +21 55 54   0.861   1.579  117.6   33.5  14.2
2020 01 15  000000  03 10 14.0  +21 39 48   0.868   1.579  117.0   33.7  14.2


101P/Chernykh
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  23 54 08.9  -07 31 18   1.886   2.374  107.3   23.4  15.9
2019 12 02  000000  23 54 55.3  -07 24 12   1.896   2.373  106.6   23.5  15.9
2019 12 03  000000  23 55 43.0  -07 16 56   1.906   2.372  105.8   23.6  15.9
2019 12 04  000000  23 56 31.9  -07 09 33   1.916   2.371  105.0   23.7  15.9
2019 12 05  000000  23 57 22.1  -07 02 01   1.926   2.369  104.2   23.8  15.9
2019 12 06  000000  23 58 13.4  -06 54 21   1.936   2.368  103.5   23.9  15.9
2019 12 07  000000  23 59 06.0  -06 46 33   1.946   2.367  102.7   24.0  15.9
2019 12 08  000000  23 59 59.8  -06 38 38   1.956   2.366  102.0   24.0  15.9
2019 12 09  000000  00 00 54.8  -06 30 34   1.967   2.365  101.2   24.1  16.0
2019 12 10  000000  00 01 50.9  -06 22 24   1.977   2.364  100.5   24.2  16.0
2019 12 11  000000  00 02 48.2  -06 14 06   1.987   2.362   99.7   24.3  16.0
2019 12 12  000000  00 03 46.6  -06 05 41   1.998   2.361   99.0   24.3  16.0
2019 12 13  000000  00 04 46.0  -05 57 09   2.008   2.360   98.3   24.4  16.0
2019 12 14  000000  00 05 46.6  -05 48 30   2.019   2.359   97.6   24.4  16.0
2019 12 15  000000  00 06 48.3  -05 39 44   2.029   2.359   96.8   24.5  16.0
2019 12 16  000000  00 07 51.0  -05 30 52   2.040   2.358   96.1   24.5  16.0
2019 12 17  000000  00 08 54.7  -05 21 54   2.051   2.357   95.4   24.6  16.0
2019 12 18  000000  00 09 59.5  -05 12 49   2.061   2.356   94.7   24.6  16.0
2019 12 19  000000  00 11 05.2  -05 03 38   2.072   2.355   94.0   24.6  16.0
2019 12 20  000000  00 12 12.0  -04 54 20   2.083   2.354   93.3   24.7  16.1
2019 12 21  000000  00 13 19.8  -04 44 57   2.094   2.354   92.6   24.7  16.1
2019 12 22  000000  00 14 28.5  -04 35 28   2.104   2.353   91.9   24.7  16.1
2019 12 23  000000  00 15 38.2  -04 25 53   2.115   2.352   91.2   24.7  16.1
2019 12 24  000000  00 16 48.9  -04 16 13   2.126   2.351   90.6   24.7  16.1
2019 12 25  000000  00 18 00.5  -04 06 27   2.137   2.351   89.9   24.7  16.1
2019 12 26  000000  00 19 13.0  -03 56 36   2.148   2.350   89.2   24.7  16.1
2019 12 27  000000  00 20 26.4  -03 46 40   2.159   2.350   88.6   24.7  16.1
2019 12 28  000000  00 21 40.7  -03 36 38   2.170   2.349   87.9   24.7  16.1
2019 12 29  000000  00 22 55.9  -03 26 32   2.181   2.349   87.2   24.7  16.1
2019 12 30  000000  00 24 11.9  -03 16 21   2.192   2.348   86.6   24.7  16.2
2019 12 31  000000  00 25 28.8  -03 06 05   2.203   2.348   85.9   24.7  16.2
2020 01 01  000000  00 26 46.5  -02 55 45   2.214   2.347   85.3   24.7  16.2
2020 01 02  000000  00 28 05.0  -02 45 20   2.225   2.347   84.6   24.7  16.2
2020 01 03  000000  00 29 24.3  -02 34 51   2.236   2.347   84.0   24.6  16.2
2020 01 04  000000  00 30 44.4  -02 24 18   2.248   2.346   83.3   24.6  16.2
2020 01 05  000000  00 32 05.3  -02 13 41   2.259   2.346   82.7   24.6  16.2
2020 01 06  000000  00 33 27.0  -02 03 00   2.270   2.346   82.1   24.5  16.2
2020 01 07  000000  00 34 49.3  -01 52 16   2.281   2.346   81.4   24.5  16.2
2020 01 08  000000  00 36 12.4  -01 41 28   2.292   2.345   80.8   24.4  16.2
2020 01 09  000000  00 37 36.3  -01 30 36   2.303   2.345   80.2   24.4  16.3
2020 01 10  000000  00 39 00.8  -01 19 41   2.315   2.345   79.6   24.4  16.3
2020 01 11  000000  00 40 26.0  -01 08 43   2.326   2.345   79.0   24.3  16.3
2020 01 12  000000  00 41 51.9  -00 57 42   2.337   2.345   78.3   24.2  16.3
2020 01 13  000000  00 43 18.5  -00 46 38   2.348   2.345   77.7   24.2  16.3
2020 01 14  000000  00 44 45.7  -00 35 32   2.359   2.345   77.1   24.1  16.3
2020 01 15  000000  00 46 13.6  -00 24 22   2.371   2.345   76.5   24.1  16.3


68P/Klemola
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  20 50 17.2  -14 59 12   2.034   1.808   62.7   29.0  14.1
2019 12 02  000000  20 52 57.6  -14 54 11   2.043   1.809   62.3   28.9  14.1
2019 12 03  000000  20 55 38.1  -14 48 58   2.052   1.811   61.9   28.7  14.1
2019 12 04  000000  20 58 18.6  -14 43 35   2.060   1.812   61.6   28.6  14.2
2019 12 05  000000  21 00 59.0  -14 38 00   2.069   1.813   61.2   28.4  14.2
2019 12 06  000000  21 03 39.3  -14 32 15   2.078   1.815   60.8   28.3  14.2
2019 12 07  000000  21 06 19.6  -14 26 20   2.087   1.817   60.5   28.2  14.2
2019 12 08  000000  21 08 59.8  -14 20 13   2.096   1.818   60.1   28.0  14.2
2019 12 09  000000  21 11 39.9  -14 13 57   2.105   1.820   59.7   27.9  14.2
2019 12 10  000000  21 14 19.8  -14 07 31   2.114   1.822   59.4   27.7  14.2
2019 12 11  000000  21 16 59.6  -14 00 54   2.124   1.823   59.0   27.6  14.2
2019 12 12  000000  21 19 39.3  -13 54 08   2.133   1.825   58.6   27.4  14.3
2019 12 13  000000  21 22 18.8  -13 47 12   2.142   1.827   58.3   27.3  14.3
2019 12 14  000000  21 24 58.1  -13 40 06   2.151   1.829   57.9   27.1  14.3
2019 12 15  000000  21 27 37.2  -13 32 51   2.161   1.831   57.5   27.0  14.3
2019 12 16  000000  21 30 16.2  -13 25 27   2.170   1.833   57.2   26.8  14.3
2019 12 17  000000  21 32 54.9  -13 17 54   2.179   1.835   56.8   26.7  14.3
2019 12 18  000000  21 35 33.5  -13 10 11   2.189   1.838   56.4   26.5  14.3
2019 12 19  000000  21 38 11.8  -13 02 20   2.198   1.840   56.1   26.3  14.4
2019 12 20  000000  21 40 49.8  -12 54 21   2.208   1.842   55.7   26.2  14.4
2019 12 21  000000  21 43 27.7  -12 46 12   2.217   1.844   55.3   26.0  14.4
2019 12 22  000000  21 46 05.3  -12 37 56   2.227   1.847   54.9   25.9  14.4
2019 12 23  000000  21 48 42.6  -12 29 31   2.237   1.849   54.6   25.7  14.4
2019 12 24  000000  21 51 19.6  -12 20 58   2.246   1.852   54.2   25.5  14.4
2019 12 25  000000  21 53 56.4  -12 12 17   2.256   1.854   53.8   25.4  14.4
2019 12 26  000000  21 56 32.9  -12 03 29   2.266   1.857   53.5   25.2  14.5
2019 12 27  000000  21 59 09.1  -11 54 33   2.275   1.859   53.1   25.0  14.5
2019 12 28  000000  22 01 45.1  -11 45 30   2.285   1.862   52.7   24.9  14.5
2019 12 29  000000  22 04 20.6  -11 36 19   2.295   1.865   52.4   24.7  14.5
2019 12 30  000000  22 06 55.9  -11 27 02   2.305   1.868   52.0   24.5  14.5
2019 12 31  000000  22 09 30.9  -11 17 38   2.315   1.870   51.6   24.3  14.5
2020 01 01  000000  22 12 05.5  -11 08 07   2.325   1.873   51.2   24.2  14.6
2020 01 02  000000  22 14 39.7  -10 58 30   2.335   1.876   50.9   24.0  14.6
2020 01 03  000000  22 17 13.7  -10 48 46   2.345   1.879   50.5   23.8  14.6
2020 01 04  000000  22 19 47.2  -10 38 57   2.355   1.882   50.1   23.6  14.6
2020 01 05  000000  22 22 20.4  -10 29 01   2.365   1.885   49.7   23.5  14.6
2020 01 06  000000  22 24 53.2  -10 19 00   2.375   1.888   49.4   23.3  14.6
2020 01 07  000000  22 27 25.7  -10 08 54   2.385   1.892   49.0   23.1  14.7
2020 01 08  000000  22 29 57.8  -09 58 42   2.395   1.895   48.6   22.9  14.7
2020 01 09  000000  22 32 29.4  -09 48 25   2.405   1.898   48.2   22.7  14.7
2020 01 10  000000  22 35 00.8  -09 38 03   2.416   1.901   47.9   22.6  14.7
2020 01 11  000000  22 37 31.7  -09 27 36   2.426   1.905   47.5   22.4  14.7
2020 01 12  000000  22 40 02.2  -09 17 04   2.436   1.908   47.1   22.2  14.7
2020 01 13  000000  22 42 32.3  -09 06 28   2.446   1.912   46.7   22.0  14.8
2020 01 14  000000  22 45 02.1  -08 55 48   2.457   1.915   46.4   21.8  14.8
2020 01 15  000000  22 47 31.5  -08 45 03   2.467   1.919   46.0   21.6  14.8


29P/Schwassmann-Wachmann
   T.U.      H M S         J2000.0         DELTA     R     ELON   FASE   M1
------------------  ---------------------  ------  ------  -----  -----  ----
2019 12 01  000000  00 25 06.8  +13 11 42   5.193   5.780  122.3    8.3  15.2
2019 12 02  000000  00 25 03.9  +13 10 04   5.207   5.781  121.3    8.4  15.2
2019 12 03  000000  00 25 01.7  +13 08 29   5.221   5.781  120.3    8.5  15.2
2019 12 04  000000  00 25 00.2  +13 06 59   5.235   5.781  119.3    8.6  15.2
2019 12 05  000000  00 24 59.4  +13 05 32   5.249   5.781  118.3    8.6  15.2
2019 12 06  000000  00 24 59.2  +13 04 09   5.263   5.781  117.2    8.7  15.2
2019 12 07  000000  00 24 59.7  +13 02 49   5.277   5.781  116.2    8.8  15.2
2019 12 08  000000  00 25 01.0  +13 01 34   5.292   5.781  115.2    8.9  15.2
2019 12 09  000000  00 25 02.9  +13 00 23   5.307   5.781  114.2    8.9  15.2
2019 12 10  000000  00 25 05.4  +12 59 15   5.321   5.781  113.3    9.0  15.3
2019 12 11  000000  00 25 08.7  +12 58 11   5.336   5.782  112.3    9.1  15.3
2019 12 12  000000  00 25 12.6  +12 57 12   5.351   5.782  111.3    9.1  15.3
2019 12 13  000000  00 25 17.2  +12 56 16   5.366   5.782  110.3    9.2  15.3
2019 12 14  000000  00 25 22.5  +12 55 25   5.381   5.782  109.3    9.2  15.3
2019 12 15  000000  00 25 28.4  +12 54 37   5.397   5.782  108.3    9.3  15.3
2019 12 16  000000  00 25 35.0  +12 53 54   5.412   5.782  107.3    9.4  15.3
2019 12 17  000000  00 25 42.3  +12 53 15   5.428   5.782  106.4    9.4  15.3
2019 12 18  000000  00 25 50.2  +12 52 40   5.443   5.782  105.4    9.4  15.3
2019 12 19  000000  00 25 58.8  +12 52 09   5.459   5.782  104.4    9.5  15.3
2019 12 20  000000  00 26 08.1  +12 51 42   5.474   5.782  103.4    9.5  15.3
2019 12 21  000000  00 26 18.0  +12 51 19   5.490   5.783  102.5    9.6  15.3
2019 12 22  000000  00 26 28.6  +12 51 01   5.506   5.783  101.5    9.6  15.3
2019 12 23  000000  00 26 39.8  +12 50 46   5.522   5.783  100.5    9.6  15.3
2019 12 24  000000  00 26 51.6  +12 50 36   5.538   5.783   99.6    9.7  15.3
2019 12 25  000000  00 27 04.1  +12 50 30   5.554   5.783   98.6    9.7  15.3
2019 12 26  000000  00 27 17.2  +12 50 29   5.570   5.783   97.6    9.7  15.4
2019 12 27  000000  00 27 31.0  +12 50 31   5.586   5.783   96.7    9.7  15.4
2019 12 28  000000  00 27 45.4  +12 50 38   5.602   5.783   95.7    9.7  15.4
2019 12 29  000000  00 28 00.4  +12 50 49   5.618   5.783   94.8    9.8  15.4
2019 12 30  000000  00 28 16.0  +12 51 04   5.634   5.784   93.8    9.8  15.4
2019 12 31  000000  00 28 32.3  +12 51 24   5.650   5.784   92.9    9.8  15.4
2020 01 01  000000  00 28 49.1  +12 51 47   5.666   5.784   92.0    9.8  15.4
2020 01 02  000000  00 29 06.6  +12 52 15   5.682   5.784   91.0    9.8  15.4
2020 01 03  000000  00 29 24.6  +12 52 47   5.698   5.784   90.1    9.8  15.4
2020 01 04  000000  00 29 43.3  +12 53 23   5.715   5.784   89.2    9.8  15.4
2020 01 05  000000  00 30 02.5  +12 54 03   5.731   5.784   88.2    9.8  15.4
2020 01 06  000000  00 30 22.3  +12 54 48   5.747   5.784   87.3    9.8  15.4
2020 01 07  000000  00 30 42.7  +12 55 36   5.763   5.784   86.4    9.8  15.4
2020 01 08  000000  00 31 03.6  +12 56 28   5.779   5.785   85.4    9.8  15.4
2020 01 09  000000  00 31 25.1  +12 57 25   5.795   5.785   84.5    9.7  15.4
2020 01 10  000000  00 31 47.1  +12 58 25   5.811   5.785   83.6    9.7  15.4
2020 01 11  000000  00 32 09.7  +12 59 30   5.827   5.785   82.7    9.7  15.5
2020 01 12  000000  00 32 32.8  +13 00 38   5.843   5.785   81.8    9.7  15.5
2020 01 13  000000  00 32 56.5  +13 01 50   5.859   5.785   80.9    9.7  15.5
2020 01 14  000000  00 33 20.6  +13 03 06   5.875   5.785   80.0    9.6  15.5
2020 01 15  000000  00 33 45.3  +13 04 26   5.891   5.785   79.0    9.6  15.5

M1: es un valor teórico estimado (mag absoluta) de la magnitud total de la coma. 
No es necesariamente la magnitud que será observada la "coma" del cometa.
M2: es el valor de la magnitud nuclear (de la condensación central de la coma).
Las Magnitudes CCD suelen estar cerca de 2 magnitudes por debajo de la visual; entonces 
no es de esperar coincidencia entre la observación visual (m1=--) con la CCD (m1=-- CCD; 
debe tenerse en cuenta en la toma y medición el de cubrir la totalidad de la coma visible.
Se aconseja utilizar aberturas pequeñas (concentración) y con filtro V.

–~——–~–~—-~——–~——-~–~—-~–~–~——–~–~—-~——–~——~–~—-

  1. b.tardes. .
    ¿ pregunto…..cuando habrá un cometa menor de mag. 10???…
    por qué son tan poco frecuentes? ?..

    • Estimo que para Septiembre tendremos uno nuevo, que sea más brillante que magnitud 10. Será C/2018 W2 (Africano). Y en Noviembre-Diciembre C/2017 T2 (PanSTARRS) aproximadamente en 8va. Veremos sus evoluciones en estos próximos meses. La mayor o menor frecuencia es relativo a los pasos de los periódicos si son o no favorables por sus distancia con la Tierra. Y de los no-periódicos: dependerá mucho de los próximos descubrimientos y de sus distancia al perihelio y a su vez si estén cercanos a la Tierra. El 1P/Halley pasó el perihelio en 1986 con la Tierra del otro lado de nuestra órbita (muy desfavorable). En 1910 pasamos por entre la cola del cometa. Y en la próxima pasaremos demasiado cerca del Halley y mejor que en 1910. Es bastante azaroso todo.

  2. Juan Araujo

    Señor
    Luis Mansilla.
    Tengo una inquietud: ¿por qué en las tablas de coordenadas de los cometas se invirtió la posición de las letras ( H M S ) correspondientes a la Ascensión Recta?
    Saludos.

    • C/2018 V1 (Machholz-Fujikawa-Iwamoto)
      T.U. H M S J2000.0 DELTA R ELON FASE M1
      —————— ——————— —— —— —– —– —-
      2018 11 12 000000 12 41 44.8 -01 38 14 1.034 0.679 39.1 66.9 10.4
      Explico la primera línea
      Año Mes Día Hora Min Seg TU – J2000.0 – AR 12 41 44.8 DEC -01 38 14
      J2000.0 coordenadas del cometa para el año 2000, primer grupo es AR (RA) y el segundo grupo la declinación.
      Espero se entienda

  3. Gracias por datos de mi pasión: COMETAS
    Abrazos Eduardo.

  4. Buen dia! Espero avistar a C2015 V2 JHONSON si el clima ayuda…para junio’17.
    Abrazo a todos Amantes como yo de la Astronomía.. en especial los Cometas,

  5. Siempre. Busco algún cometa razonablemente brillante de al menos de mag 10 o menor. Pero nada😞, es mi observación favorita: la de Cometas, pero desde la zona donde vivo el cielo es de hasta mag.3
    Y con mi telescopio Newton 800mm f4 es difícil ver cometas débiles. Mmm 😠

    • Hola Eduardo, por cierto para ver cometas es aconsejable cambiar de sitio, pero esto no siempre se puede 😦
      Corregí en parte el texto. Si es un Newtoniano de una focal de 800 mm y f/4 la abertura es de 200 mm o 20 cm.
      Lo que indicaría que podrías ver menospreciado y con dificultad -por las condiciones de tu cielo- cometas de hasta magnitud 11 casi seguro.
      Algo muy importante de aclarar a todos aquellos que consultan las efemérides cuando se fijan en la última columna de datos está el llamado “m1” ese valor es teórico y orientativo (tomar como pronóstico por decirlo de otra forma) y el fijado por el organismo competente (MPC) conforme la magnitud absoluta en el momento del descubrimiento y confirmación.
      No significa que lo veremos con esos brillos en el futuro. Deben fijarse luego de ver las efemérides, en Cometas Observables los datos orientativos de las observaciones reales y en la páginas últimas Observaciones para ver el brillo que está siendo registrado para cada cometa. Suelen ser en muchos casos de 2 a más magnitudes más brillantes al pronóstico.
      Contame ¿donde es tu residencia (ciudad y país)? para ver que es lo que tenes disponible este mes o ver en los siguientes si se te favorece en algo la tan ansiada observación cometaria.

      • Hola Luis. Recien veo tu nensaje…poco frecuento internet x falta tiempo…
        Gracias!
        Mi long Oeste 57,59°
        Lat Sur 37,9614°
        Hace 30 años soy aficionado a Astronomía la AMO ! *(el clima No me ayuda)
        Mar del Plata .prov. Buenos Aires
        Argentina
        Un abrazo.

  6. Eduardo jorge

    Gracias por datos de mi preferencia como astrónomo aficionado.
    siempre espero un cometa mag. 2 durante luna nueva…y q.esté despejado…abrazo a tod@s !

  7. Nuevamente ¡gracias LIADA x la info. AMO la Astronomia, especialmente los COMETAS.
    Desde Mar del Plata, Buenos Aires, Argentina. Abrazo!

  8. Bronny Sanchez

    Desde Barquisimeto, Venezuela, le envío un saludo efusivo al compañero Luis Mansilla! Soy miembro de ALDA…Hace ya cierto tiempo te envié un reporte de mi observación! Después de una larga ausencia, espero ya comenzar con los reportes de forma progresiva!

    • OK, Bienvenido al grupo de Rastreadores de Cometas. Esperamos tu reportes e invitamos a muchos aficionados que observan cometas se animen a reportar. Estamos a vuestra disposición para guiarlos y ayudarle a confeccionar estos, que luego publicaremos con cada cometa. Ya te he incluido en el listado de Membresía. Saludos y un fuerte abrazo para los hermanos venezolanos y para quienes leen nuestra -“por que es de todos”- web de la Sección Cometas de la LIADA.

      • Excelente Luis! Ya vi mi nombre en el listado, junto a muchos grandes y experimentados observadores de cometas (Michael Matiazzo, Chris Wyatt, tu persona, por nombrar unos pocos) y es un honor estar, dando ese pequeño aporte, y para mi, muy grande, ya que la observación de cometas es por la cual me he inclinado, en definitiva, en lo que astronomía observacional se refiere.. Mucha preparación, Dedicación, Perseverancia, y nutrirse día a día, con los aportes, sugerencias y el apoyo invaluable de tu persona, dada la amplia experiencia que posees.. Un saludo muy efusivo Luis y… manos a la obra!

        Bronny Sánchez
        Asociación Larénse de Astronomía
        Barquisimeto, Venezuela.

  9. Gracias x informacion(de Cometas)excelente! Ojala lleguen cometas mas brillantes.o mas cerca,o mas Grandes..o la sumatoria d.todo.

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