
Periodisch heller 16m
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P=Periode; q=Periheldistanz; d=mögliche Erdnähe; i=Bahnneigung; T-=letztes Perihel; T+=nächstes Perihel; m=max. Helligkeit bei nächster Wiederkehr
Nr | Namen/Entdecker | Entdeckt | P | q | d |
i | T- | T+ | m |
1 |
Halley |
1705 |
76.01 |
0,59 |
0,12 |
162.2 |
1986 |
2061 |
2 |
2 |
Encke |
1819 |
3.30 |
0,34 |
0,22 |
11.8 |
2017 |
2023 |
6 |
4 |
Faye |
1843 |
7.55 |
1,67 |
0,62 |
9.1 |
2021 |
2029 |
12 |
6 |
d'Arrest |
1851 |
6.53 |
1,35 |
0,15 |
19.5 |
2021 |
2028 |
9 |
7 |
Pons-Winnecke |
1819 |
6.38 |
1,26 |
0,04 |
22.3 |
2021 |
2027 |
14 |
8 |
Tuttle |
1858 |
13.51 |
0,99 |
0,25 |
54.7 |
2021 |
2035 |
6 |
9 |
Tempel |
1867 |
5.51 |
1,50 |
0,57 |
10.5 |
2016 |
2022 |
11 |
10 |
Tempel |
1873 |
5.47 |
1,48 |
0,32 |
11.9 |
2021 |
2026 |
9 |
12 |
Pons-Brooks |
1812 |
70.92 |
0,77 |
0,63 |
74.9 |
1954 |
2024 |
10 |
13 |
Olbers |
1815 |
69.56 |
1,17 |
1,26 |
44.7 |
1956 |
2024 |
7 |
15 |
Finlay |
1886 |
6.75 |
1,03 |
0,18 |
3.7 |
2021 |
2028 |
12 |
16 |
Brooks |
1889 |
6.86 |
1,83 |
0,85 |
5.5 |
2021 |
2028 |
14 |
17 |
Holmes |
1892 |
6.88 |
2,05 |
1,62 |
19.1 |
2021 |
2028 |
2 |
19 |
Borrelly |
1904 |
6.86 |
1,36 |
0,41 |
30.3 |
2015 |
2022 |
9 |
21 |
Giacobini-Zinner |
1900 |
6.62 |
1,04 |
0,25 |
31.8 |
2018 |
2025 |
10 |
22 |
Kopff |
1906 |
6.46 |
1,58 |
0,56 |
4.7 |
2015 |
2022 |
10 |
23 |
Brorsen-Metcalf |
1847 |
70.52 |
0,47 |
0,62 |
19.3 |
1989 |
2059 |
6 |
24 |
Schaumasse |
1911 |
8.25 |
1,20 |
0,27 |
11.7 |
2017 |
2024 |
8 |
26 |
Grigg-Skjellerup |
1902 |
5.10 |
0,99 |
0,16 |
21.1 |
2018 |
2023 |
13 |
27 |
Crommelin |
1818 |
27.40 |
0,73 |
0,21 |
29.1 |
2011 |
2039 |
11 |
28 |
Neujmin |
1913 |
18.19 |
1,55 |
0,53 |
14.2 |
2021 |
2039 |
15 |
29 |
Schwassmann-Wachmann |
1927 |
14.65 |
5,72 |
4,46 |
9.4 |
2019 |
2035 |
11 |
30 |
Reinmuth |
1928 |
7.32 |
1,88 |
0,83 |
8.1 |
2017 |
2024 |
14 |
33 |
Daniel |
1909 |
8.10 |
2,16 |
0,42 |
22.4 |
2016 |
2024 |
14 |
35 |
Herschel-Rigollet |
1788 |
154.91 |
0,75 |
0,33 |
64.2 |
1939 |
2092 |
8 |
37 |
Forbes |
1929 |
14.65 |
1,57 |
0,54 |
8.9 |
2018 |
2024 |
15 |
38 |
Stephan-Oterma |
1867 |
37.71 |
1,57 |
0,59 |
17.9 |
2018 |
2056 |
11 |
40 |
Vaisala |
1939 |
10.83 |
1,79 |
0,77 |
11.5 |
2014 |
2025 |
15 |
41 |
Tuttle-Giacobini-Kresak |
1858 |
5.43 |
1,05 |
0,13 |
9.2 |
2017 |
2022 |
11 |
43 |
Wolf-Harrington |
1924 |
6.45 |
1,58 |
0,92 |
18.5 |
2016 |
2025 |
11 |
44 |
Reinmuth |
1947 |
6.63 |
1,89 |
0,89 |
6.9 |
2015 |
2022 |
15 |
45 |
Honda-Mrkos-Pajdusakova |
1948 |
5.25 |
0,52 |
0,06 |
4.2 |
2016 |
2022 |
8 |
46 |
Wirtanen |
1948 |
5.44 |
1,06 |
0,07 |
11.7 |
2018 |
2024 |
8 |
47 |
Ashbrook-Jackson |
1948 |
7.45 |
2,30 |
1,30 |
12.5 |
2017 |
2025 |
14 |
48 |
Johnson |
1949 |
6.96 |
2,31 |
1,01 |
13.6 |
2018 |
2025 |
15 |
49 |
Arend-Rigaux |
1951 |
6.61 |
1,37 |
0,43 |
18.3 |
2018 |
2025 |
14 |
50 |
Arend |
1951 |
8.24 |
1,92 |
0,88 |
19.2 |
2016 |
2024 |
14 |
52 |
Harrington-Abell |
1955 |
7.53 |
1,76 |
0,80 |
10.2 |
2021 |
2029 |
15 |
53 |
van Biesbroeck |
1954 |
12.52 |
2,41 |
1,40 |
6.6 |
2016 |
2028 |
13 |
55 |
Tempel-Tuttle |
1865 |
33.22 |
0,97 |
0,06 |
162.5 |
1998 |
2031 |
11 |
59 |
Kearns-Kwee |
1963 |
9.45 |
2,34 |
1,24 |
9.3 |
2018 |
2028 |
14 |
60 |
Tsuchinshan |
1965 |
6.78 |
1,76 |
0,66 |
6.7 |
2018 |
2025 |
16 |
61 |
Shajn-Schaldach |
1949 |
7.45 |
2,33 |
1,13 |
6.1 |
2015 |
2022 |
13 |
62 |
Tsuchinshan |
1965 |
6.62 |
1,49 |
0,49 |
10.5 |
2017 |
2023 |
8 |
63 |
Wild |
1960 |
13.24 |
1,96 |
0,95 |
19.9 |
2013 |
2026 |
13 |
64 |
Swift-Gehrels |
1889 |
9.18 |
1,34 |
0,44 |
8.4 |
2018 |
2028 |
10 |
65 |
Gunn |
1970 |
6.80 |
2,44 |
1,47 |
10.4 |
2017 |
2025 |
13 |
66 |
du Toit |
1944 |
14.70 |
1,27 |
0,49 |
18.7 |
2018 |
2033 |
12 |
67 |
Churyumov-Gerasimenko |
1969 |
6.57 |
1,29 |
0,39 |
7.1 |
2021 |
2028 |
12 |
68 |
Klemola |
1965 |
10.82 |
1,75 |
0,76 |
11.1 |
2019 |
2030 |
15 |
69 |
Taylor |
1915 |
6.95 |
1,94 |
0,64 |
20.5 |
2019 |
2026 |
15 |
71 |
Clark |
1973 |
5.51 |
1,56 |
0,58 |
9.5 |
2017 |
2023 |
11 |
72 |
Denning-Fujikawa |
1881 |
9.00 |
0,78 |
0,11 |
8.6 |
2014 |
2023 |
9 |
73 |
Schwassmann-Wachmann |
1930 |
5.35 |
0,94 |
0,08 |
11.4 |
2017 |
2022 |
11 |
74 |
Smirnova-Chernykh |
1975 |
8.52 |
3,56 |
3,50 |
6.6 |
2018 |
2026 |
15 |
76 |
West-Kohoutek-Ikemura |
1975 |
6.41 |
1,57 |
0,61 |
30.5 |
2019 |
2026 |
14 |
77 |
Longmore |
1975 |
6.82 |
2,31 |
2,30 |
24.4 |
2016 |
2023 |
15 |
78 |
Gehrels |
1973 |
7.22 |
2,01 |
1,31 |
6.5 |
2019 |
2026 |
11 |
81 |
Wild |
1978 |
6.40 |
1,59 |
0,65 |
3.2 |
2016 |
2022 |
9 |
84 |
Giclas |
1978 |
6.96 |
1,84 |
0,72 |
7.2 |
2020 |
2027 |
16 |
88 |
Howell |
1981 |
5.50 |
1,37 |
0,87 |
4.4 |
2020 |
2026 |
10 |
89 |
Russell |
1980 |
7.42 |
2,29 |
1,50 |
12.0 |
2016 |
2024 |
15 |
90 |
Gehrels |
1972 |
14.83 |
2,96 |
2,22 |
9.6 |
2017 |
2032 |
11 |
91 |
Russell |
1983 |
14.83 |
2,96 |
2,53 |
9.6 |
2020 |
2028 |
15 |
92 |
Sanguin |
1977 |
12.44 |
1,81 |
0,82 |
18.8 |
2015 |
2027 |
13 |
93 |
Lovas |
1980 |
9.14 |
1,69 |
0,83 |
12.2 |
2017 |
2026 |
13 |
94 |
Russell |
1984 |
6.58 |
2,23 |
1,26 |
6.2 |
2016 |
2023 |
15 |
95 |
Chiron |
1977 |
50.73 |
8,45 |
7,45 |
6.9 |
1996 |
2046 |
15 |
96 |
Machholz |
1986 |
5.23 |
0,12 |
0,32 |
60.1 |
2017 |
2023 |
6 |
97 |
Metcalf-Brewington |
1906 |
10.53 |
2,61 |
0,62 |
17.9 |
2011 |
2022 |
14 |
98 |
Takamizawa |
1984 |
7.21 |
1,58 |
0,69 |
9.5 |
2021 |
2028 |
15 |
101 |
Chernykh |
1977 |
13.92 |
2,35 |
1,81 |
5.1 |
2020 |
2034 |
15 |
102 |
Shoemaker |
1984 |
7.26 |
1,98 |
0,99 |
26.2 |
2021 |
2028 |
14 |
103 |
Hartley |
1986 |
6.40 |
1,03 |
0,12 |
13.6 |
2017 |
2023 |
6 |
104 |
Kowal |
1972 |
6.18 |
1,39 |
0,05 |
15.5 |
2016 |
2022 |
9 |
106 |
Schuster |
1977 |
7.29 |
1,54 |
0,77 |
20.1 |
2021 |
2028 |
15 |
108 |
Ciffreo |
1985 |
7.26 |
1,72 |
0,73 |
13.1 |
2021 |
2028 |
12 |
109 |
Swift-Tuttle |
1862 |
135.00 |
1,96 |
0,34 |
113.4 |
1992 |
2126 |
5 |
110 |
Hartley |
1988 |
6.87 |
2,48 |
1,81 |
11.6 |
2021 |
2028 |
14 |
114 |
Wiseman-Skiff |
1986 |
6.65 |
1,57 |
0,61 |
18.3 |
2020 |
2026 |
16 |
116 |
Wild |
1990 |
6.47 |
2,17 |
1,29 |
3.6 |
2016 |
2022 |
11 |
117 |
Helin-Roman-Alu |
1989 |
8.24 |
3,03 |
2,26 |
8.7 |
2014 |
2022 |
13 |
118 |
Shoemaker-Levy |
1991 |
6.49 |
2,01 |
0,87 |
8.5 |
2016 |
2022 |
11 |
119 |
Parker-Hartley |
1989 |
8.89 |
3,04 |
2,12 |
5.1 |
2014 |
2022 |
13 |
122 |
de Vico |
1846 |
74.41 |
0,65 |
0,32 |
85.4 |
1995 |
2069 |
8 |
123 |
West-Hartley |
1989 |
7.58 |
2,13 |
1,40 |
15.3 |
2019 |
2026 |
15 |
124 |
Mrkos |
1991 |
5.75 |
1,46 |
0,41 |
31.3 |
2020 |
2026 |
14 |
126 |
IRAS |
1983 |
13.29 |
1,70 |
0,78 |
45.9 |
2010 |
2023 |
13 |
128 |
Shoemaker-Holt |
1987 |
9.51 |
3,04 |
2,09 |
4.3 |
2017 |
2026 |
15 |
130 |
McNaught-Hughes |
1991 |
6.66 |
2,10 |
1,17 |
7.3 |
2018 |
2024 |
15 |
131 |
Mueller |
1990 |
7.35 |
2,42 |
1,47 |
7.3 |
2019 |
2026 |
16 |
134 |
Kowal-Vavrova |
1983 |
15.58 |
2,57 |
1,57 |
4.3 |
2014 |
2030 |
13 |
141 |
Machholz |
1994 |
5.23 |
0,75 |
0,12 |
12.8 |
2020 |
2026 |
12 |
144 |
Kushida |
1994 |
7.57 |
1,43 |
0,49 |
4.1 |
2016 |
2024 |
8 |
147 |
Kushida-Muramatsu |
1993 |
7.43 |
2,75 |
1,76 |
2.4 |
2016 |
2023 |
16 |
154 |
Brewington |
1992 |
10.66 |
1,59 |
0,65 |
18.0 |
2013 |
2024 |
9 |
155 |
Shoemaker |
1994 |
17.10 |
1,81 |
0,87 |
6.4 |
2019 |
2036 |
14 |
157 |
Tritton |
1977 |
6.45 |
1,42 |
0,45 |
7.1 |
2016 |
2022 |
12 |
161 |
Hartley-IRAS |
1984 |
21.49 |
1,27 |
0,50 |
95.7 |
2005 |
2026 |
11 |
162 |
Siding Spring |
2004 |
5.32 |
1,23 |
0,44 |
27.8 |
2020 |
2026 |
13 |
164 |
Christensen |
2004 |
6.91 |
1,64 |
0,78 |
16.2 |
2018 |
2025 |
15 |
168 |
Hergenrother |
1998 |
6.92 |
1,42 |
0,42 |
4.1 |
2019 |
2026 |
15 |
169 |
NEAT |
2001 |
4.20 |
0,60 |
0,15 |
11.3 |
2018 |
2022 |
10 |
171 |
Spahr |
1999 |
6.62 |
1,73 |
0,84 |
21.9 |
2019 |
2025 |
15 |
174 |
Echeclus |
2000 |
35.30 |
5,86 |
4,85 |
4.3 |
2015 |
2050 |
14 |
181 |
Shoemaker-Levy |
1999 |
7.53 |
1,13 |
0,22 |
16.9 |
2014 |
2022 |
12 |
185 |
Petriew |
2001 |
5.47 |
0,94 |
0,82 |
13.9 |
2018 |
2023 |
11 |
192 |
Shoemaker-Levy |
1990 |
16.37 |
1,46 |
0,50 |
24.5 |
2007 |
2024 |
13 |
205 |
Giacobini |
1896 |
6.66 |
1,53 |
0,51 |
15.3 |
2015 |
2022 |
12 |
207 |
NEAT |
2001 |
7.66 |
0,94 |
0,22 |
10.1 |
2016 |
2024 |
12 |
209 |
LINEAR |
2003 |
5.09 |
0,97 |
0,05 |
21.2 |
2019 |
2024 |
12 |
210 |
Christensen |
2003 |
5.66 |
0,53 |
0,32 |
10.2 |
2020 |
2025 |
8 |
213 |
Van Ness |
2005 |
6.33 |
2,12 |
2,37 |
10.2 |
2017 |
2023 |
13 |
217 |
LINEAR |
2001 |
7.83 |
1,22 |
0,40 |
12.9 |
2017 |
2025 |
11 |
218 |
LINEAR |
2003 |
6.09 |
1,70 |
0,40 |
18.1 |
2020 |
2026 |
13 |
222 |
LINEAR |
2004 |
4.83 |
0,78 |
0,10 |
5.1 |
2019 |
2024 |
13 |
230 |
LINEAR |
1997 |
6.27 |
1,48 |
0,50 |
14.6 |
2015 |
2022 |
13 |
240 |
NEAT |
2002 |
7.59 |
2,12 |
2,10 |
23.5 |
2018 |
2025 |
13 |
249 |
LINEAR |
2006 |
4.62 |
0,51 |
0,10 |
4.6 |
2020 |
2025 |
11 |
252 |
LINEAR |
2000 |
5.34 |
1,00 |
0,03 |
10.4 |
2021 |
2026 |
10 |
255 |
Levy |
2006 |
5.29 |
1,00 |
0,10 |
18.2 |
2017 |
2022 |
13 |
260 |
McNaught |
2005 |
7.06 |
1,50 |
0,50 |
15.7 |
2019 |
2026 |
11 |
262 |
McNaught-Russell |
1994 |
18.25 |
1,28 |
0,80 |
29.1 |
2012 |
2030 |
11 |
284 |
McNaught |
2006 |
7.04 |
2,29 |
1,30 |
11.9 |
2021 |
2028 |
14 |
300 |
Catalina |
2005 |
4.42 |
0,82 |
0,05 |
5.7 |
2018 |
2023 |
14 |
315 |
LONEOS |
2005 |
11.22 |
2,42 |
1,50 |
17.9 |
2016 |
2027 |
13 |
333 |
LINEAR |
2007 |
8.63 |
1,10 |
0,18 |
132.4 |
2016 |
2024 |
10 |
355 |
LINEAR-NEAT |
2004 |
6.48 |
1,71 |
0,57 |
11.0 |
2017 |
2024 |
14 |