SECCIÓN de COMETAS de la LIADA - Liga Iberoamericana de Astronomía -
Web: https://rastreadoresdecometas.wordpress.com/
EFEMÉRIDES DE COMETAS DEL 1 MAYO AL 15 DE JUNIO DE 2024
C/2023 V4 (Camarasa-Duszanowicz)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 03 35 07.4 +29 06 59 2.115 1.218 20.0 16.4 14.5
2024 05 02 000000 03 37 12.1 +29 43 29 2.110 1.212 19.9 16.4 14.5
2024 05 03 000000 03 39 19.2 +30 20 05 2.104 1.206 19.8 16.5 14.4
2024 05 04 000000 03 41 28.7 +30 56 47 2.099 1.200 19.8 16.5 14.4
2024 05 05 000000 03 43 40.8 +31 33 35 2.094 1.194 19.8 16.6 14.4
2024 05 06 000000 03 45 55.6 +32 10 28 2.088 1.189 19.8 16.7 14.4
2024 05 07 000000 03 48 13.2 +32 47 27 2.083 1.184 19.8 16.8 14.3
2024 05 08 000000 03 50 33.6 +33 24 32 2.077 1.179 19.8 16.9 14.3
2024 05 09 000000 03 52 56.9 +34 01 41 2.071 1.174 19.9 17.0 14.3
2024 05 10 000000 03 55 23.4 +34 38 55 2.066 1.169 20.0 17.2 14.3
2024 05 11 000000 03 57 53.1 +35 16 13 2.060 1.165 20.2 17.4 14.2
2024 05 12 000000 04 00 26.2 +35 53 36 2.054 1.161 20.3 17.6 14.2
2024 05 13 000000 04 03 02.7 +36 31 02 2.048 1.157 20.5 17.8 14.2
2024 05 14 000000 04 05 42.8 +37 08 31 2.042 1.153 20.7 18.0 14.2
2024 05 15 000000 04 08 26.8 +37 46 02 2.036 1.149 20.9 18.3 14.1
2024 05 16 000000 04 11 14.6 +38 23 36 2.029 1.146 21.1 18.5 14.1
2024 05 17 000000 04 14 06.6 +39 01 11 2.023 1.143 21.4 18.8 14.1
2024 05 18 000000 04 17 02.8 +39 38 47 2.017 1.140 21.7 19.1 14.1
2024 05 19 000000 04 20 03.5 +40 16 23 2.010 1.137 21.9 19.4 14.1
2024 05 20 000000 04 23 08.8 +40 53 58 2.004 1.134 22.3 19.7 14.1
2024 05 21 000000 04 26 19.0 +41 31 32 1.998 1.132 22.6 20.1 14.0
2024 05 22 000000 04 29 34.3 +42 09 02 1.991 1.130 22.9 20.4 14.0
2024 05 23 000000 04 32 54.8 +42 46 29 1.985 1.128 23.3 20.8 14.0
2024 05 24 000000 04 36 20.8 +43 23 52 1.978 1.127 23.6 21.1 14.0
2024 05 25 000000 04 39 52.6 +44 01 08 1.972 1.125 24.0 21.5 14.0
2024 05 26 000000 04 43 30.4 +44 38 17 1.965 1.124 24.4 21.9 14.0
2024 05 27 000000 04 47 14.5 +45 15 16 1.959 1.123 24.8 22.3 14.0
2024 05 28 000000 04 51 05.1 +45 52 06 1.953 1.122 25.2 22.6 14.0
2024 05 29 000000 04 55 02.5 +46 28 43 1.946 1.122 25.7 23.0 13.9
2024 05 30 000000 04 59 07.0 +47 05 07 1.940 1.122 26.1 23.4 13.9
2024 05 31 000000 05 03 18.8 +47 41 14 1.933 1.122 26.5 23.8 13.9
2024 06 01 000000 05 07 38.4 +48 17 04 1.927 1.122 27.0 24.2 13.9
2024 06 02 000000 05 12 05.9 +48 52 34 1.921 1.123 27.4 24.6 13.9
2024 06 03 000000 05 16 41.7 +49 27 41 1.915 1.123 27.9 25.0 13.9
2024 06 04 000000 05 21 26.0 +50 02 24 1.908 1.124 28.4 25.4 13.9
2024 06 05 000000 05 26 19.3 +50 36 38 1.902 1.125 28.8 25.8 13.9
2024 06 06 000000 05 31 21.7 +51 10 22 1.896 1.127 29.3 26.2 13.9
2024 06 07 000000 05 36 33.7 +51 43 32 1.891 1.129 29.8 26.5 13.9
2024 06 08 000000 05 41 55.4 +52 16 06 1.885 1.130 30.3 26.9 13.9
2024 06 09 000000 05 47 27.1 +52 47 59 1.879 1.133 30.8 27.3 13.9
2024 06 10 000000 05 53 09.2 +53 19 08 1.873 1.135 31.2 27.6 13.9
2024 06 11 000000 05 59 01.8 +53 49 29 1.868 1.138 31.7 28.0 13.9
2024 06 12 000000 06 05 05.1 +54 18 59 1.863 1.140 32.2 28.3 13.9
2024 06 13 000000 06 11 19.3 +54 47 33 1.858 1.143 32.7 28.7 13.9
2024 06 14 000000 06 17 44.6 +55 15 07 1.853 1.147 33.2 29.0 13.9
2024 06 15 000000 06 24 21.0 +55 41 37 1.848 1.150 33.7 29.3 13.9
C/2023 C2 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 16 53 48.7 -77 34 29 2.650 3.210 115.1 16.5 14.2
2024 05 02 000000 16 52 47.8 -77 38 29 2.638 3.203 115.5 16.5 14.2
2024 05 03 000000 16 51 41.9 -77 42 15 2.625 3.196 115.9 16.5 14.1
2024 05 04 000000 16 50 31.0 -77 45 45 2.612 3.189 116.3 16.5 14.1
2024 05 05 000000 16 49 15.1 -77 49 00 2.599 3.182 116.6 16.5 14.1
2024 05 06 000000 16 47 54.5 -77 51 58 2.587 3.175 117.0 16.4 14.1
2024 05 07 000000 16 46 29.0 -77 54 39 2.575 3.168 117.4 16.4 14.1
2024 05 08 000000 16 44 58.9 -77 57 02 2.562 3.161 117.8 16.4 14.0
2024 05 09 000000 16 43 24.3 -77 59 07 2.550 3.155 118.2 16.4 14.0
2024 05 10 000000 16 41 45.4 -78 00 54 2.538 3.148 118.5 16.4 14.0
2024 05 11 000000 16 40 02.3 -78 02 20 2.526 3.141 118.9 16.4 14.0
2024 05 12 000000 16 38 15.2 -78 03 27 2.514 3.134 119.2 16.3 14.0
2024 05 13 000000 16 36 24.4 -78 04 12 2.503 3.127 119.6 16.3 13.9
2024 05 14 000000 16 34 30.1 -78 04 37 2.491 3.121 119.9 16.3 13.9
2024 05 15 000000 16 32 32.5 -78 04 40 2.480 3.114 120.3 16.3 13.9
2024 05 16 000000 16 30 31.9 -78 04 20 2.468 3.107 120.6 16.3 13.9
2024 05 17 000000 16 28 28.6 -78 03 37 2.457 3.100 120.9 16.3 13.9
2024 05 18 000000 16 26 22.9 -78 02 31 2.446 3.094 121.2 16.2 13.8
2024 05 19 000000 16 24 15.1 -78 01 01 2.435 3.087 121.5 16.2 13.8
2024 05 20 000000 16 22 05.6 -77 59 07 2.424 3.080 121.8 16.2 13.8
2024 05 21 000000 16 19 54.6 -77 56 49 2.414 3.074 122.1 16.2 13.8
2024 05 22 000000 16 17 42.5 -77 54 05 2.403 3.067 122.4 16.2 13.8
2024 05 23 000000 16 15 29.7 -77 50 56 2.393 3.060 122.7 16.2 13.8
2024 05 24 000000 16 13 16.4 -77 47 21 2.383 3.054 122.9 16.2 13.7
2024 05 25 000000 16 11 03.1 -77 43 20 2.372 3.047 123.2 16.1 13.7
2024 05 26 000000 16 08 50.0 -77 38 52 2.362 3.041 123.5 16.1 13.7
2024 05 27 000000 16 06 37.5 -77 33 58 2.353 3.034 123.7 16.1 13.7
2024 05 28 000000 16 04 26.0 -77 28 38 2.343 3.028 123.9 16.1 13.7
2024 05 29 000000 16 02 15.7 -77 22 51 2.333 3.021 124.2 16.1 13.6
2024 05 30 000000 16 00 07.1 -77 16 36 2.324 3.015 124.4 16.1 13.6
2024 05 31 000000 15 58 00.3 -77 09 55 2.315 3.008 124.6 16.1 13.6
2024 06 01 000000 15 55 55.7 -77 02 46 2.306 3.002 124.8 16.1 13.6
2024 06 02 000000 15 53 53.6 -76 55 11 2.297 2.995 124.9 16.1 13.6
2024 06 03 000000 15 51 54.3 -76 47 08 2.288 2.989 125.1 16.1 13.6
2024 06 04 000000 15 49 57.9 -76 38 39 2.279 2.982 125.3 16.1 13.5
2024 06 05 000000 15 48 04.9 -76 29 42 2.271 2.976 125.4 16.1 13.5
2024 06 06 000000 15 46 15.3 -76 20 19 2.262 2.970 125.6 16.1 13.5
2024 06 07 000000 15 44 29.4 -76 10 30 2.254 2.963 125.7 16.1 13.5
2024 06 08 000000 15 42 47.4 -76 00 14 2.246 2.957 125.8 16.2 13.5
2024 06 09 000000 15 41 09.4 -75 49 32 2.238 2.951 125.9 16.2 13.4
2024 06 10 000000 15 39 35.6 -75 38 25 2.231 2.944 126.0 16.2 13.4
2024 06 11 000000 15 38 06.0 -75 26 53 2.223 2.938 126.1 16.2 13.4
2024 06 12 000000 15 36 40.8 -75 14 56 2.216 2.932 126.2 16.2 13.4
2024 06 13 000000 15 35 20.0 -75 02 34 2.209 2.926 126.2 16.3 13.4
2024 06 14 000000 15 34 03.8 -74 49 49 2.202 2.920 126.2 16.3 13.4
2024 06 15 000000 15 32 52.1 -74 36 39 2.195 2.913 126.3 16.3 13.4
C/2023 A3 (Tsuchinshan-ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 13 22 48.4 -00 50 25 1.807 2.765 157.5 8.0 10.7
2024 05 02 000000 13 20 02.7 -00 41 34 1.800 2.751 155.9 8.6 10.7
2024 05 03 000000 13 17 16.5 -00 32 47 1.794 2.737 154.4 9.2 10.6
2024 05 04 000000 13 14 29.8 -00 24 04 1.788 2.724 152.8 9.7 10.6
2024 05 05 000000 13 11 42.9 -00 15 27 1.782 2.710 151.2 10.3 10.6
2024 05 06 000000 13 08 55.9 -00 06 55 1.778 2.696 149.6 10.9 10.6
2024 05 07 000000 13 06 08.9 +00 01 30 1.773 2.683 148.0 11.5 10.5
2024 05 08 000000 13 03 22.0 +00 09 48 1.769 2.669 146.4 12.1 10.5
2024 05 09 000000 13 00 35.5 +00 17 59 1.766 2.655 144.8 12.7 10.5
2024 05 10 000000 12 57 49.4 +00 26 02 1.763 2.641 143.2 13.2 10.4
2024 05 11 000000 12 55 03.9 +00 33 56 1.760 2.628 141.6 13.8 10.4
2024 05 12 000000 12 52 19.1 +00 41 41 1.758 2.614 140.0 14.4 10.4
2024 05 13 000000 12 49 35.2 +00 49 16 1.757 2.600 138.3 15.0 10.4
2024 05 14 000000 12 46 52.2 +00 56 41 1.755 2.586 136.7 15.5 10.3
2024 05 15 000000 12 44 10.3 +01 03 55 1.755 2.572 135.1 16.1 10.3
2024 05 16 000000 12 41 29.7 +01 10 59 1.754 2.558 133.5 16.7 10.3
2024 05 17 000000 12 38 50.4 +01 17 50 1.754 2.544 131.9 17.2 10.3
2024 05 18 000000 12 36 12.5 +01 24 30 1.755 2.530 130.3 17.7 10.3
2024 05 19 000000 12 33 36.1 +01 30 58 1.756 2.516 128.8 18.3 10.2
2024 05 20 000000 12 31 01.4 +01 37 14 1.757 2.502 127.2 18.8 10.2
2024 05 21 000000 12 28 28.4 +01 43 16 1.758 2.488 125.6 19.3 10.2
2024 05 22 000000 12 25 57.2 +01 49 06 1.760 2.473 124.0 19.8 10.2
2024 05 23 000000 12 23 27.9 +01 54 43 1.762 2.459 122.5 20.3 10.1
2024 05 24 000000 12 21 00.5 +02 00 07 1.765 2.445 120.9 20.8 10.1
2024 05 25 000000 12 18 35.2 +02 05 18 1.768 2.431 119.4 21.3 10.1
2024 05 26 000000 12 16 12.0 +02 10 14 1.771 2.416 117.9 21.8 10.1
2024 05 27 000000 12 13 50.9 +02 14 58 1.774 2.402 116.3 22.2 10.1
2024 05 28 000000 12 11 32.0 +02 19 27 1.778 2.388 114.8 22.7 10.0
2024 05 29 000000 12 09 15.4 +02 23 43 1.782 2.373 113.3 23.1 10.0
2024 05 30 000000 12 07 01.1 +02 27 46 1.786 2.359 111.8 23.5 10.0
2024 05 31 000000 12 04 49.2 +02 31 34 1.790 2.344 110.4 23.9 10.0
2024 06 01 000000 12 02 39.6 +02 35 09 1.795 2.330 108.9 24.3 9.9
2024 06 02 000000 12 00 32.4 +02 38 30 1.800 2.315 107.4 24.7 9.9
2024 06 03 000000 11 58 27.6 +02 41 37 1.805 2.301 106.0 25.1 9.9
2024 06 04 000000 11 56 25.3 +02 44 31 1.810 2.286 104.5 25.4 9.9
2024 06 05 000000 11 54 25.5 +02 47 11 1.815 2.271 103.1 25.8 9.9
2024 06 06 000000 11 52 28.2 +02 49 37 1.821 2.257 101.7 26.1 9.8
2024 06 07 000000 11 50 33.3 +02 51 50 1.826 2.242 100.3 26.5 9.8
2024 06 08 000000 11 48 40.9 +02 53 50 1.832 2.227 98.9 26.8 9.8
2024 06 09 000000 11 46 51.0 +02 55 37 1.838 2.212 97.5 27.1 9.8
2024 06 10 000000 11 45 03.5 +02 57 11 1.844 2.197 96.1 27.3 9.7
2024 06 11 000000 11 43 18.5 +02 58 32 1.850 2.182 94.7 27.6 9.7
2024 06 12 000000 11 41 36.0 +02 59 41 1.856 2.168 93.4 27.9 9.7
2024 06 13 000000 11 39 55.8 +03 00 37 1.862 2.153 92.0 28.1 9.7
2024 06 14 000000 11 38 18.1 +03 01 21 1.868 2.138 90.7 28.4 9.7
2024 06 15 000000 11 36 42.8 +03 01 53 1.875 2.122 89.4 28.6 9.6
C/2022 L2 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 10 49 19.6 -33 35 14 2.022 2.743 126.4 17.2 12.4
2024 05 02 000000 10 46 28.4 -33 17 46 2.037 2.745 125.2 17.5 12.4
2024 05 03 000000 10 43 42.7 -33 00 18 2.053 2.747 124.0 17.7 12.5
2024 05 04 000000 10 41 02.4 -32 42 52 2.069 2.749 122.8 18.0 12.5
2024 05 05 000000 10 38 27.4 -32 25 29 2.086 2.751 121.5 18.2 12.5
2024 05 06 000000 10 35 57.7 -32 08 11 2.102 2.753 120.3 18.4 12.5
2024 05 07 000000 10 33 33.1 -31 50 59 2.119 2.755 119.1 18.7 12.5
2024 05 08 000000 10 31 13.5 -31 33 56 2.137 2.757 117.9 18.9 12.6
2024 05 09 000000 10 28 58.9 -31 17 01 2.155 2.760 116.7 19.1 12.6
2024 05 10 000000 10 26 49.2 -31 00 17 2.173 2.762 115.5 19.3 12.6
2024 05 11 000000 10 24 44.1 -30 43 44 2.191 2.764 114.3 19.4 12.6
2024 05 12 000000 10 22 43.6 -30 27 23 2.209 2.767 113.1 19.6 12.6
2024 05 13 000000 10 20 47.6 -30 11 16 2.228 2.769 111.9 19.8 12.7
2024 05 14 000000 10 18 56.0 -29 55 23 2.247 2.772 110.8 19.9 12.7
2024 05 15 000000 10 17 08.6 -29 39 44 2.266 2.774 109.6 20.1 12.7
2024 05 16 000000 10 15 25.3 -29 24 21 2.286 2.777 108.4 20.2 12.7
2024 05 17 000000 10 13 46.1 -29 09 14 2.306 2.779 107.3 20.3 12.8
2024 05 18 000000 10 12 10.7 -28 54 23 2.325 2.782 106.1 20.4 12.8
2024 05 19 000000 10 10 39.1 -28 39 49 2.345 2.784 105.0 20.5 12.8
2024 05 20 000000 10 09 11.1 -28 25 31 2.365 2.787 103.9 20.6 12.8
2024 05 21 000000 10 07 46.7 -28 11 31 2.386 2.790 102.8 20.7 12.8
2024 05 22 000000 10 06 25.8 -27 57 49 2.406 2.792 101.6 20.8 12.9
2024 05 23 000000 10 05 08.2 -27 44 25 2.427 2.795 100.5 20.9 12.9
2024 05 24 000000 10 03 53.8 -27 31 18 2.447 2.798 99.5 20.9 12.9
2024 05 25 000000 10 02 42.5 -27 18 29 2.468 2.801 98.4 21.0 12.9
2024 05 26 000000 10 01 34.4 -27 05 59 2.489 2.804 97.3 21.0 13.0
2024 05 27 000000 10 00 29.1 -26 53 47 2.510 2.807 96.2 21.0 13.0
2024 05 28 000000 09 59 26.7 -26 41 52 2.531 2.810 95.2 21.1 13.0
2024 05 29 000000 09 58 27.1 -26 30 16 2.552 2.813 94.1 21.1 13.0
2024 05 30 000000 09 57 30.2 -26 18 58 2.573 2.816 93.1 21.1 13.0
2024 05 31 000000 09 56 35.8 -26 07 58 2.594 2.819 92.0 21.1 13.1
2024 06 01 000000 09 55 44.0 -25 57 16 2.616 2.822 91.0 21.1 13.1
2024 06 02 000000 09 54 54.6 -25 46 52 2.637 2.825 90.0 21.0 13.1
2024 06 03 000000 09 54 07.6 -25 36 46 2.658 2.828 89.0 21.0 13.1
2024 06 04 000000 09 53 22.9 -25 26 58 2.679 2.831 88.0 21.0 13.2
2024 06 05 000000 09 52 40.4 -25 17 27 2.700 2.834 87.0 20.9 13.2
2024 06 06 000000 09 52 00.0 -25 08 14 2.722 2.838 86.0 20.9 13.2
2024 06 07 000000 09 51 21.7 -24 59 18 2.743 2.841 85.0 20.8 13.2
2024 06 08 000000 09 50 45.4 -24 50 40 2.764 2.844 84.1 20.8 13.2
2024 06 09 000000 09 50 11.1 -24 42 19 2.785 2.848 83.1 20.7 13.3
2024 06 10 000000 09 49 38.6 -24 34 14 2.806 2.851 82.2 20.7 13.3
2024 06 11 000000 09 49 08.0 -24 26 27 2.827 2.854 81.2 20.6 13.3
2024 06 12 000000 09 48 39.1 -24 18 56 2.848 2.858 80.3 20.5 13.3
2024 06 13 000000 09 48 11.9 -24 11 41 2.869 2.861 79.3 20.4 13.4
2024 06 14 000000 09 47 46.3 -24 04 42 2.890 2.865 78.4 20.3 13.4
2024 06 15 000000 09 47 22.3 -23 58 00 2.911 2.868 77.5 20.2 13.4
C/2022 E2 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 06 49 26.4 +32 32 29 4.263 3.863 60.2 13.1 14.0
2024 05 02 000000 06 49 23.4 +32 36 42 4.277 3.860 59.3 13.0 14.0
2024 05 03 000000 06 49 21.4 +32 40 54 4.291 3.858 58.3 12.8 14.0
2024 05 04 000000 06 49 20.4 +32 45 05 4.304 3.855 57.4 12.7 14.0
2024 05 05 000000 06 49 20.2 +32 49 14 4.318 3.852 56.4 12.6 14.0
2024 05 06 000000 06 49 21.0 +32 53 22 4.331 3.850 55.5 12.5 14.0
2024 05 07 000000 06 49 22.7 +32 57 29 4.344 3.847 54.5 12.3 14.0
2024 05 08 000000 06 49 25.2 +33 01 35 4.356 3.844 53.6 12.2 14.0
2024 05 09 000000 06 49 28.6 +33 05 40 4.369 3.841 52.7 12.1 14.0
2024 05 10 000000 06 49 32.9 +33 09 44 4.381 3.839 51.7 11.9 14.1
2024 05 11 000000 06 49 37.9 +33 13 48 4.394 3.836 50.8 11.8 14.1
2024 05 12 000000 06 49 43.8 +33 17 50 4.406 3.834 49.9 11.6 14.1
2024 05 13 000000 06 49 50.4 +33 21 52 4.417 3.831 49.0 11.5 14.1
2024 05 14 000000 06 49 57.8 +33 25 54 4.429 3.828 48.1 11.3 14.1
2024 05 15 000000 06 50 06.0 +33 29 55 4.440 3.826 47.2 11.2 14.1
2024 05 16 000000 06 50 14.9 +33 33 55 4.452 3.823 46.3 11.0 14.1
2024 05 17 000000 06 50 24.6 +33 37 55 4.463 3.821 45.4 10.9 14.1
2024 05 18 000000 06 50 34.9 +33 41 55 4.473 3.818 44.5 10.7 14.1
2024 05 19 000000 06 50 45.9 +33 45 55 4.484 3.816 43.6 10.5 14.1
2024 05 20 000000 06 50 57.6 +33 49 54 4.494 3.813 42.7 10.4 14.1
2024 05 21 000000 06 51 10.0 +33 53 54 4.504 3.811 41.9 10.2 14.1
2024 05 22 000000 06 51 23.0 +33 57 53 4.514 3.809 41.0 10.0 14.1
2024 05 23 000000 06 51 36.7 +34 01 53 4.524 3.806 40.1 9.9 14.1
2024 05 24 000000 06 51 51.0 +34 05 52 4.533 3.804 39.3 9.7 14.1
2024 05 25 000000 06 52 05.8 +34 09 52 4.542 3.801 38.4 9.5 14.1
2024 05 26 000000 06 52 21.3 +34 13 51 4.551 3.799 37.6 9.4 14.1
2024 05 27 000000 06 52 37.4 +34 17 51 4.560 3.797 36.7 9.2 14.1
2024 05 28 000000 06 52 54.0 +34 21 52 4.568 3.794 35.9 9.0 14.1
2024 05 29 000000 06 53 11.2 +34 25 53 4.577 3.792 35.1 8.8 14.1
2024 05 30 000000 06 53 29.0 +34 29 54 4.585 3.790 34.3 8.7 14.1
2024 05 31 000000 06 53 47.3 +34 33 56 4.592 3.788 33.4 8.5 14.1
2024 06 01 000000 06 54 06.1 +34 37 58 4.600 3.785 32.6 8.3 14.1
2024 06 02 000000 06 54 25.4 +34 42 01 4.607 3.783 31.8 8.1 14.1
2024 06 03 000000 06 54 45.2 +34 46 04 4.614 3.781 31.0 7.9 14.1
2024 06 04 000000 06 55 05.5 +34 50 09 4.621 3.779 30.2 7.8 14.1
2024 06 05 000000 06 55 26.3 +34 54 14 4.627 3.777 29.4 7.6 14.1
2024 06 06 000000 06 55 47.6 +34 58 20 4.633 3.775 28.7 7.4 14.1
2024 06 07 000000 06 56 09.3 +35 02 27 4.639 3.772 27.9 7.2 14.1
2024 06 08 000000 06 56 31.4 +35 06 34 4.645 3.770 27.1 7.1 14.1
2024 06 09 000000 06 56 54.0 +35 10 43 4.650 3.768 26.4 6.9 14.1
2024 06 10 000000 06 57 17.0 +35 14 53 4.656 3.766 25.7 6.7 14.1
2024 06 11 000000 06 57 40.4 +35 19 05 4.660 3.764 24.9 6.5 14.1
2024 06 12 000000 06 58 04.1 +35 23 17 4.665 3.762 24.2 6.4 14.1
2024 06 13 000000 06 58 28.3 +35 27 31 4.669 3.760 23.5 6.2 14.1
2024 06 14 000000 06 58 52.8 +35 31 46 4.674 3.758 22.8 6.0 14.1
2024 06 15 000000 06 59 17.6 +35 36 02 4.677 3.756 22.2 5.9 14.1
C/2021 S3 (PANSTARRS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 20 18 58.2 +42 59 42 1.542 1.727 82.4 35.3 8.8
2024 05 02 000000 20 20 09.2 +43 33 32 1.551 1.736 82.5 35.1 8.8
2024 05 03 000000 20 21 18.0 +44 06 50 1.559 1.745 82.6 35.0 8.9
2024 05 04 000000 20 22 24.6 +44 39 36 1.568 1.754 82.8 34.8 8.9
2024 05 05 000000 20 23 28.8 +45 11 50 1.576 1.763 82.9 34.6 9.0
2024 05 06 000000 20 24 30.7 +45 43 33 1.585 1.772 83.0 34.4 9.0
2024 05 07 000000 20 25 30.3 +46 14 45 1.593 1.781 83.1 34.2 9.0
2024 05 08 000000 20 26 27.5 +46 45 26 1.602 1.791 83.3 34.0 9.1
2024 05 09 000000 20 27 22.3 +47 15 35 1.611 1.800 83.4 33.9 9.1
2024 05 10 000000 20 28 14.7 +47 45 14 1.620 1.810 83.5 33.7 9.1
2024 05 11 000000 20 29 04.7 +48 14 23 1.628 1.819 83.7 33.5 9.2
2024 05 12 000000 20 29 52.1 +48 43 01 1.637 1.828 83.8 33.3 9.2
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C/2021 G2 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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C/2020 V2 (ZTF)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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2024 05 05 000000 00 27 03.5 -43 58 24 4.713 4.441 68.4 12.2 14.7
2024 05 06 000000 00 27 35.3 -44 07 22 4.708 4.449 69.1 12.2 14.7
2024 05 07 000000 00 28 06.7 -44 16 30 4.703 4.457 69.8 12.3 14.8
2024 05 08 000000 00 28 37.7 -44 25 48 4.699 4.466 70.6 12.3 14.8
2024 05 09 000000 00 29 08.2 -44 35 16 4.694 4.474 71.3 12.3 14.8
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2024 06 15 000000 00 40 00.4 -52 19 57 4.512 4.775 98.9 12.1 15.0
C/2020 K1 (PANSTARRS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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C/2019 U5 (PANSTARRS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 07 21 12.3 -35 10 58 5.022 5.027 84.6 11.5 15.0
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2024 05 05 000000 07 20 56.7 -34 43 08 5.087 5.050 82.2 11.4 15.1
2024 05 06 000000 07 20 55.1 -34 36 30 5.104 5.056 81.6 11.4 15.1
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2024 05 09 000000 07 20 55.0 -34 17 21 5.152 5.073 79.9 11.3 15.1
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2024 05 11 000000 07 20 59.0 -34 05 14 5.185 5.085 78.7 11.2 15.1
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2024 05 19 000000 07 21 43.7 -33 22 11 5.312 5.131 74.3 10.9 15.2
2024 05 20 000000 07 21 52.2 -33 17 24 5.327 5.137 73.8 10.9 15.2
2024 05 21 000000 07 22 01.3 -33 12 46 5.343 5.143 73.2 10.9 15.3
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2024 06 12 000000 07 27 25.1 -32 05 15 5.657 5.272 62.9 9.9 15.5
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2024 06 15 000000 07 28 23.3 -32 01 09 5.695 5.290 61.7 9.7 15.5
C/2019 T4 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 17 45 17.8 +30 12 26 6.426 6.918 115.4 7.6 17.4
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2024 05 05 000000 17 44 19.5 +30 37 07 6.425 6.940 117.0 7.4 17.5
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2024 05 09 000000 17 43 13.0 +31 00 17 6.426 6.963 118.4 7.3 17.5
2024 05 10 000000 17 42 55.2 +31 05 50 6.427 6.969 118.8 7.3 17.5
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C/2019 L3 (ATLAS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 10 36 24.8 -51 12 18 7.247 7.811 120.8 6.4 17.7
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C/2017 K2 (PANSTARRS)
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 05 23 37.9 +12 09 38 6.377 5.661 41.4 6.8 13.1
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2024 05 05 000000 05 25 40.8 +12 27 43 6.454 5.695 38.2 6.3 13.1
2024 05 06 000000 05 26 12.2 +12 32 07 6.472 5.703 37.3 6.2 13.1
2024 05 07 000000 05 26 43.7 +12 36 29 6.491 5.711 36.5 6.0 13.1
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2024 05 09 000000 05 27 47.4 +12 45 03 6.527 5.728 34.9 5.8 13.2
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2024 06 09 000000 05 45 18.5 +14 36 12 6.977 5.988 12.0 2.0 13.5
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2024 06 15 000000 05 48 46.7 +14 53 28 7.038 6.038 9.2 1.5 13.5
479P/Elenin
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 08 46 24.0 -14 55 37 0.621 1.245 96.9 53.5 14.9
2024 05 02 000000 08 49 14.1 -15 15 01 0.621 1.244 96.8 53.5 14.9
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2024 05 05 000000 08 58 05.9 -16 13 31 0.621 1.244 96.6 53.7 14.9
2024 05 06 000000 09 01 10.4 -16 33 04 0.621 1.244 96.6 53.7 14.9
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2024 05 08 000000 09 07 30.4 -17 12 15 0.621 1.244 96.6 53.7 14.9
2024 05 09 000000 09 10 45.8 -17 31 51 0.621 1.245 96.6 53.7 14.9
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2024 05 30 000000 10 32 10.9 -24 00 55 0.644 1.288 99.5 50.9 15.1
2024 05 31 000000 10 36 35.8 -24 17 00 0.647 1.292 99.8 50.7 15.2
2024 06 01 000000 10 41 03.0 -24 32 45 0.649 1.295 100.0 50.4 15.2
2024 06 02 000000 10 45 32.4 -24 48 08 0.652 1.299 100.2 50.2 15.2
2024 06 03 000000 10 50 03.8 -25 03 09 0.655 1.303 100.4 49.9 15.2
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2024 06 05 000000 10 59 12.2 -25 31 59 0.661 1.312 100.9 49.4 15.3
2024 06 06 000000 11 03 48.9 -25 45 48 0.665 1.316 101.1 49.2 15.3
2024 06 07 000000 11 08 27.1 -25 59 12 0.668 1.320 101.3 48.9 15.3
2024 06 08 000000 11 13 06.6 -26 12 10 0.672 1.325 101.6 48.6 15.4
2024 06 09 000000 11 17 47.3 -26 24 42 0.676 1.329 101.8 48.4 15.4
2024 06 10 000000 11 22 29.1 -26 36 48 0.680 1.334 102.0 48.1 15.4
2024 06 11 000000 11 27 11.6 -26 48 26 0.684 1.339 102.2 47.8 15.4
2024 06 12 000000 11 31 54.9 -26 59 37 0.689 1.344 102.4 47.6 15.5
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2024 06 15 000000 11 46 07.1 -27 30 23 0.703 1.360 103.0 46.7 15.6
473P/NEAT
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 04 07 35.1 +63 15 31 2.073 1.637 50.9 28.5 17.2
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2024 05 09 000000 05 05 44.4 +64 54 30 2.118 1.690 51.7 28.0 17.4
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2024 05 30 000000 07 39 16.8 +63 05 38 2.283 1.845 52.2 25.7 18.0
2024 05 31 000000 07 45 32.7 +62 49 10 2.293 1.853 52.2 25.6 18.0
2024 06 01 000000 07 51 40.6 +62 31 56 2.303 1.861 52.1 25.5 18.0
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2024 06 03 000000 08 03 32.2 +61 55 26 2.323 1.876 52.0 25.2 18.1
2024 06 04 000000 08 09 16.0 +61 36 13 2.333 1.884 51.9 25.1 18.1
2024 06 05 000000 08 14 51.7 +61 16 26 2.343 1.892 51.8 24.9 18.1
2024 06 06 000000 08 20 19.6 +60 56 06 2.354 1.900 51.7 24.8 18.1
2024 06 07 000000 08 25 39.7 +60 35 15 2.364 1.908 51.6 24.6 18.2
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2024 06 09 000000 08 35 57.1 +59 52 09 2.386 1.925 51.4 24.4 18.2
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2024 06 11 000000 08 45 44.9 +59 07 26 2.408 1.941 51.2 24.1 18.3
2024 06 12 000000 08 50 28.2 +58 44 33 2.420 1.949 51.1 23.9 18.3
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2024 06 15 000000 09 03 57.7 +57 34 05 2.454 1.974 50.7 23.5 18.4
227P/Catalina-LINEAR
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 09 27 21.0 +22 20 27 1.270 1.706 96.3 36.0 18.2
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154P/Brewington
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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144P/Kushida
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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103P/Hartley
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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62P/Tsuchinshan
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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32P/Comas Sola
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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29P/Schwassmann-Wachmann
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
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2024 05 28 000000 08 22 29.5 +19 37 04 6.707 6.205 56.4 7.8 16.1
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2024 06 01 000000 08 24 44.9 +19 27 00 6.760 6.206 53.2 7.5 16.1
2024 06 02 000000 08 25 19.6 +19 24 26 6.773 6.206 52.3 7.4 16.1
2024 06 03 000000 08 25 54.6 +19 21 50 6.786 6.206 51.5 7.4 16.1
2024 06 04 000000 08 26 29.9 +19 19 12 6.799 6.207 50.7 7.3 16.1
2024 06 05 000000 08 27 05.6 +19 16 33 6.811 6.207 49.9 7.2 16.1
2024 06 06 000000 08 27 41.5 +19 13 53 6.824 6.207 49.1 7.1 16.1
2024 06 07 000000 08 28 17.8 +19 11 11 6.836 6.207 48.3 7.0 16.1
2024 06 08 000000 08 28 54.3 +19 08 28 6.848 6.208 47.5 6.9 16.1
2024 06 09 000000 08 29 31.2 +19 05 44 6.860 6.208 46.7 6.8 16.1
2024 06 10 000000 08 30 08.3 +19 02 58 6.872 6.208 45.9 6.7 16.1
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13P/Olbers
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 04 38 48.5 +26 32 03 2.243 1.479 31.4 20.8 9.0
2024 05 02 000000 04 41 12.4 +26 54 15 2.239 1.470 31.0 20.7 8.9
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2024 05 04 000000 04 46 06.8 +27 38 34 2.231 1.453 30.3 20.5 8.8
2024 05 05 000000 04 48 37.3 +28 00 40 2.227 1.445 30.0 20.4 8.8
2024 05 06 000000 04 51 10.1 +28 22 43 2.223 1.437 29.7 20.4 8.7
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2024 05 08 000000 04 56 22.6 +29 06 40 2.214 1.420 29.1 20.3 8.6
2024 05 09 000000 04 59 02.4 +29 28 34 2.209 1.412 28.9 20.2 8.5
2024 05 10 000000 05 01 44.7 +29 50 23 2.205 1.404 28.6 20.1 8.5
2024 05 11 000000 05 04 29.5 +30 12 08 2.200 1.396 28.4 20.1 8.4
2024 05 12 000000 05 07 16.8 +30 33 48 2.195 1.388 28.1 20.1 8.3
2024 05 13 000000 05 10 06.6 +30 55 22 2.190 1.381 27.9 20.0 8.3
2024 05 14 000000 05 12 59.0 +31 16 52 2.185 1.373 27.7 20.0 8.2
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2024 05 16 000000 05 18 51.9 +31 59 31 2.175 1.358 27.3 19.9 8.1
2024 05 17 000000 05 21 52.5 +32 20 41 2.170 1.351 27.1 19.9 8.1
2024 05 18 000000 05 24 55.8 +32 41 43 2.165 1.343 26.9 19.9 8.0
2024 05 19 000000 05 28 02.0 +33 02 36 2.160 1.336 26.8 19.9 7.9
2024 05 20 000000 05 31 11.1 +33 23 21 2.155 1.329 26.6 19.9 7.9
2024 05 21 000000 05 34 23.1 +33 43 57 2.149 1.323 26.5 19.9 7.8
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2024 05 23 000000 05 40 56.2 +34 24 38 2.138 1.309 26.2 20.0 7.7
2024 05 24 000000 05 44 17.4 +34 44 42 2.133 1.303 26.1 20.0 7.7
2024 05 25 000000 05 47 41.7 +35 04 33 2.127 1.296 26.1 20.1 7.6
2024 05 26 000000 05 51 09.2 +35 24 12 2.122 1.290 26.0 20.1 7.6
2024 05 27 000000 05 54 39.9 +35 43 38 2.116 1.284 25.9 20.2 7.5
2024 05 28 000000 05 58 13.9 +36 02 49 2.111 1.278 25.9 20.3 7.5
2024 05 29 000000 06 01 51.3 +36 21 44 2.105 1.272 25.9 20.3 7.4
2024 05 30 000000 06 05 32.1 +36 40 24 2.100 1.267 25.8 20.4 7.4
2024 05 31 000000 06 09 16.3 +36 58 46 2.094 1.261 25.8 20.5 7.3
2024 06 01 000000 06 13 03.9 +37 16 51 2.088 1.256 25.8 20.6 7.3
2024 06 02 000000 06 16 55.1 +37 34 36 2.083 1.251 25.8 20.7 7.2
2024 06 03 000000 06 20 49.8 +37 52 02 2.077 1.246 25.9 20.8 7.2
2024 06 04 000000 06 24 48.1 +38 09 07 2.071 1.241 25.9 20.9 7.1
2024 06 05 000000 06 28 50.0 +38 25 49 2.066 1.236 26.0 21.1 7.1
2024 06 06 000000 06 32 55.5 +38 42 08 2.060 1.231 26.0 21.2 7.1
2024 06 07 000000 06 37 04.6 +38 58 03 2.054 1.227 26.1 21.3 7.0
2024 06 08 000000 06 41 17.4 +39 13 32 2.049 1.223 26.2 21.5 7.0
2024 06 09 000000 06 45 33.8 +39 28 35 2.043 1.219 26.3 21.6 6.9
2024 06 10 000000 06 49 53.8 +39 43 10 2.037 1.215 26.4 21.8 6.9
2024 06 11 000000 06 54 17.5 +39 57 15 2.032 1.211 26.5 22.0 6.9
2024 06 12 000000 06 58 44.8 +40 10 51 2.026 1.207 26.6 22.1 6.8
2024 06 13 000000 07 03 15.7 +40 23 54 2.021 1.204 26.7 22.3 6.8
2024 06 14 000000 07 07 50.2 +40 36 24 2.015 1.201 26.9 22.5 6.8
2024 06 15 000000 07 12 28.3 +40 48 21 2.010 1.198 27.0 22.7 6.7
12P/Pons-Brooks
Posiciones para -30º 00' 00" +060º 00' 00"
T.U. H M S J2000.0 DELTA R ELON FASE M1
------------------ --------------------- ------ ------ ----- ----- ----
2024 05 01 000000 04 01 47.9 +02 48 45 1.594 0.803 25.0 32.0 3.8
2024 05 02 000000 04 05 06.7 +02 05 57 1.593 0.808 25.4 32.4 3.9
2024 05 03 000000 04 08 24.9 +01 23 10 1.591 0.813 25.8 32.7 3.9
2024 05 04 000000 04 11 42.6 +00 40 25 1.589 0.818 26.3 33.1 3.9
2024 05 05 000000 04 14 59.8 -00 02 16 1.588 0.824 26.8 33.5 4.0
2024 05 06 000000 04 18 16.8 -00 44 55 1.586 0.830 27.3 33.9 4.0
2024 05 07 000000 04 21 33.6 -01 27 30 1.584 0.836 27.8 34.2 4.0
2024 05 08 000000 04 24 50.4 -02 10 01 1.582 0.843 28.4 34.6 4.1
2024 05 09 000000 04 28 07.1 -02 52 28 1.580 0.851 28.9 35.0 4.1
2024 05 10 000000 04 31 24.1 -03 34 51 1.578 0.858 29.5 35.4 4.2
2024 05 11 000000 04 34 41.2 -04 17 08 1.576 0.866 30.1 35.8 4.2
2024 05 12 000000 04 37 58.8 -04 59 21 1.574 0.874 30.7 36.2 4.3
2024 05 13 000000 04 41 16.7 -05 41 28 1.572 0.883 31.3 36.5 4.3
2024 05 14 000000 04 44 35.3 -06 23 30 1.570 0.891 32.0 36.9 4.4
2024 05 15 000000 04 47 54.4 -07 05 27 1.568 0.900 32.6 37.2 4.4
2024 05 16 000000 04 51 14.4 -07 47 17 1.567 0.909 33.2 37.6 4.5
2024 05 17 000000 04 54 35.1 -08 29 02 1.565 0.919 33.9 37.9 4.5
2024 05 18 000000 04 57 56.8 -09 10 40 1.563 0.929 34.6 38.2 4.6
2024 05 19 000000 05 01 19.5 -09 52 12 1.561 0.939 35.3 38.5 4.6
2024 05 20 000000 05 04 43.3 -10 33 37 1.559 0.949 35.9 38.7 4.7
2024 05 21 000000 05 08 08.2 -11 14 56 1.558 0.959 36.6 39.0 4.7
2024 05 22 000000 05 11 34.5 -11 56 07 1.556 0.970 37.3 39.3 4.8
2024 05 23 000000 05 15 02.1 -12 37 11 1.554 0.980 38.0 39.5 4.8
2024 05 24 000000 05 18 31.1 -13 18 07 1.553 0.991 38.7 39.7 4.9
2024 05 25 000000 05 22 01.6 -13 58 55 1.552 1.002 39.4 39.9 5.0
2024 05 26 000000 05 25 33.6 -14 39 35 1.550 1.013 40.1 40.1 5.0
2024 05 27 000000 05 29 07.3 -15 20 06 1.549 1.025 40.8 40.2 5.1
2024 05 28 000000 05 32 42.7 -16 00 29 1.548 1.036 41.5 40.4 5.1
2024 05 29 000000 05 36 19.8 -16 40 41 1.548 1.048 42.2 40.5 5.2
2024 05 30 000000 05 39 58.8 -17 20 44 1.547 1.060 42.9 40.6 5.3
2024 05 31 000000 05 43 39.6 -18 00 37 1.547 1.071 43.6 40.7 5.3
2024 06 01 000000 05 47 22.3 -18 40 18 1.546 1.083 44.3 40.8 5.4
2024 06 02 000000 05 51 07.0 -19 19 48 1.546 1.095 45.0 40.9 5.4
2024 06 03 000000 05 54 53.8 -19 59 06 1.546 1.108 45.7 40.9 5.5
2024 06 04 000000 05 58 42.5 -20 38 12 1.546 1.120 46.3 40.9 5.6
2024 06 05 000000 06 02 33.3 -21 17 04 1.547 1.132 47.0 41.0 5.6
2024 06 06 000000 06 06 26.3 -21 55 42 1.547 1.145 47.7 41.0 5.7
2024 06 07 000000 06 10 21.3 -22 34 05 1.548 1.157 48.4 41.0 5.7
2024 06 08 000000 06 14 18.5 -23 12 13 1.549 1.170 49.0 40.9 5.8
2024 06 09 000000 06 18 17.8 -23 50 04 1.551 1.182 49.7 40.9 5.9
2024 06 10 000000 06 22 19.3 -24 27 38 1.552 1.195 50.3 40.8 5.9
2024 06 11 000000 06 26 23.0 -25 04 54 1.554 1.208 51.0 40.8 6.0
2024 06 12 000000 06 30 28.9 -25 41 51 1.556 1.221 51.6 40.7 6.0
2024 06 13 000000 06 34 36.9 -26 18 27 1.558 1.233 52.2 40.6 6.1
2024 06 14 000000 06 38 47.1 -26 54 43 1.561 1.246 52.9 40.5 6.2
2024 06 15 000000 06 42 59.4 -27 30 36 1.564 1.259 53.5 40.4 6.2
--~--------~--~----~--------~-------~--~----~--~--~--------~--~-
M1: No es necesariamente la magnitud que será observada de 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 en la medición el de cubrir la totalidad de la coma visible.
Se aconseja utilizar aberturas pequeñas (generar concentración) y con la utilización del filtro "V".
-esto último aproxima el m1=-- CCD a los valores visuales-
--~--------~--~----~--------~-------~--~----~--~--~--------~--~-
--~--------~--~----~--------~-------~--~----~--~--~--------~--~-
M1: No es necesariamente la magnitud que será observada de 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 en la medición el de cubrir la totalidad de la coma visible.
Se aconseja utilizar aberturas pequeñas (generar concentración) y con la utilización del filtro "V".
-esto último aproxima el m1=-- CCD a los valores visuales-
--~--------~--~----~--------~-------~--~----~--~--~--------~--~-
Observación de Cometas @Rastreadores de Cometas 
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.
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
Gracias por datos de mi pasión: COMETAS
Abrazos Eduardo.
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,
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.
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 !
Todos sostenemos esta esperanza 🙂
Nuevamente ¡gracias LIADA x la info. AMO la Astronomia, especialmente los COMETAS.
Desde Mar del Plata, Buenos Aires, Argentina. Abrazo!
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.
Gracias x informacion(de Cometas)excelente! Ojala lleguen cometas mas brillantes.o mas cerca,o mas Grandes..o la sumatoria d.todo.
La esperanza es lo último que se pierde 🙂