Кометы галлеевского типа (также называются кометами семейства Нептуна) имеют период обращения вокруг Солнца P<200 лет, наклонение орбиты от 0° до 180°, инвариант Тиссерана <2. Многие из комет семейства Нептуна наблюдались всего лишь 1 или 2 раза с момента открытия. Орбиты комет семейства Нептуна более неустойчивы, чем орбиты комет семейства Юпитера, так как подвергаются гравитационным возмущениям со стороны планет-гигантов.
Кометы семейства Нептуна
В столбцах приводятся: обозначение кометы, точка перигелия кометы в астрономических единицах , эксцентриситет e, наклонение орбиты i, период обращения вокруг Солнца P и значение инварианта Тиссерана. В последнем столбце даются названия некоторых известных комет на русском языке.| Обозначение | q | e | i | P | TJ | Примечания |
|---|---|---|---|---|---|---|
| 1P/Halley | 0.575 | 0.968 | 162.2 | 75.9 | -0.598 | комета Галлея |
| 8P/Tuttle | 1.027 | 0.820 | 55.0 | 13.6 | 1.601 | комета Туттля |
| 12P/Pons-Brooks | 0.781 | 0.955 | 74.2 | 71.2 | 0.598 | комета Понса — Брукса |
| 13P/Olbers | 1.153 | 0.931 | 44.6 | 68.1 | 1.244 | комета Ольберса |
| 20D/Westphal | 1.254 | 0.920 | 40.9 | 61.9 | 1.361 | |
| 23P/Brorsen-Metcalf | 0.479 | 0.972 | 19.3 | 70.5 | 1.109 | |
| 27P/Crommelin | 0.734 | 0.919 | 29.2 | 27.4 | 1.481 | комета Кроммелина |
| 35P/Herschel-Rigollet | 0.748 | 0.974 | 64.2 | 154.9 | 0.644 | |
| 38P/Stephan-Oterma | 1.589 | 0.859 | 18.4 | 37.9 | 1.891 | |
| 55P/Tempel-Tuttle | 0.976 | 0.906 | 162.5 | 33.2 | -0.637 | комета Темпеля — Туттля |
| 96P/Machholz 1 | 0.124 | 0.959 | 58.1 | 5.3 | 1.942 | комета Макхольца |
| 109P/Swift-Tuttle | 0.960 | 0.963 | 113.5 | 133.3 | -0.280 | комета Свифта — Туттля |
| 122P/de Vico | 0.659 | 0.963 | 85.4 | 74.3 | 0.375 | |
| 126P/IRAS | 1.714 | 0.696 | 45.9 | 13.4 | 1.964 | |
| 161P/Hartley-IRAS | 1.275 | 0.835 | 95.7 | 21.5 | 0.540 | |
| 177P/Barnard | 1.107 | 0.954 | 31.2 | 119.8 | 1.317 | |
| 262P/McNaught-Russell | 1.280 | 0.815 | 29.1 | 18.3 | 1.918 | |
| 273P/Pons-Gambart | 0.810 | 0.975 | 136.4 | 188.1 | -0.645 | |
| 333P/LINEAR | 1.115 | 0.736 | 131.9 | 8.7 | 0.417 | |
| 342P/ SOHO | 0.053 | 0.983 | 13.3 | 5.3 | 1.986 | |
| 389/Siding Spring | 1.660 | 0.705 | 160.1 | 13.3 | -0.461 | комета Сайдинг-Спринг |
| C/1905 F1 (Giacobini) | 1.113 | 0.953 | 40.1 | 114.4 | 1.210 | |
| C/1914 S1 (Campbell) | 0.678 | 0.904 | 76.9 | 18.7 | 0.964 | |
| C/1917 F1 (Mellish) | 0.190 | 0.993 | 32.7 | 143.4 | 0.644 | |
| C/1921 H1 (Dubiago) | 1.116 | 0.935 | 22.3 | 70.7 | 1.496 | |
| C/1937 D1 (Wilk) | 0.619 | 0.981 | 26.0 | 180.8 | 1.035 | |
| C/1942 EA (Vaisala) | 1.287 | 0.934 | 38.0 | 85.4 | 1.358 | |
| C/1960 Y1 (Candy) | 1.047 | 0.930 | 151.2 | 58.2 | -0.746 | |
| C/1984 A1 (Bradfield 1) | 1.357 | 0.952 | 51.8 | 151.9 | 1.065 | |
| C/1989 A3 (Bradfield) | 0.421 | 0.978 | 83.1 | 84.1 | 0.368 | |
| C/1991 L3 (Levy) | 0.983 | 0.929 | 19.2 | 51.3 | 1.517 | |
| C/1998 G1 (LINEAR) | 2.133 | 0.824 | 109.7 | 42.1 | -0.153 | |
| C/1998 Y1 (LINEAR) | 1.747 | 0.924 | 28.1 | 110.0 | 1.645 | |
| C/1999 E1 (Li) | 3.920 | 0.760 | 46.9 | 66.1 | 1.893 | |
| C/1999 G1 (LINEAR) | 4.049 | 0.857 | 76.6 | 150.3 | 0.742 | |
| P/1999 J6 (SOHO) | 0.049 | 0.984 | 26.6 | 5.5 | 1.923 | |
| C/1999 K4 (LINEAR) | 1.442 | 0.916 | 120.8 | 71.7 | -0.445 | |
| C/1999 S3 (LINEAR) | 1.895 | 0.900 | 70.6 | 82.4 | 0.828 | |
| C/2000 D2 (LINEAR) | 2.298 | 0.867 | 157.0 | 71.8 | -1.370 | |
| C/2000 G2 (LINEAR) | 2.717 | 0.810 | 170.5 | 53.9 | -1.553 | |
| C/2001 OG108 (LONEOS) | 0.994 | 0.925 | 80.2 | 48.5 | 0.597 | |
| P/2001 Q6 (NEAT) | 1.408 | 0.824 | 56.9 | 22.6 | 1.419 | |
| C/2001 W2 (BATTERS) | 1.051 | 0.941 | 115.9 | 75.9 | -0.257 | |
| C/2002 B1 (LINEAR) | 2.271 | 0.771 | 51.0 | 31.2 | 1.631 | |
| C/2002 CE10 (LINEAR) | 2.047 | 0.791 | 145.5 | 30.8 | -0.853 | |
| C/2002 K4 (NEAT) | 2.765 | 0.842 | 94.1 | 73.4 | 0.157 | |
| C/2002 R5 (SOHO) | 0.047 | 0.985 | 14.1 | 5.8 | 1.879 | |
| P/2002 S7 (SOHO) | 0.049 | 0.985 | 13.6 | 5.8 | 1.879 | |
| C/2003 F1 (LINEAR) | 4.008 | 0.806 | 70.2 | 93.9 | 1.050 | |
| C/2003 R1 (LINEAR) | 2.102 | 0.893 | 149.2 | 87.4 | -1.238 | |
| C/2003 U1 (LINEAR) | 1.796 | 0.922 | 164.5 | 109.6 | -1.342 | |
| C/2003 W1 (LINEAR) | 1.652 | 0.934 | 78.1 | 126.3 | 0.531 | |
| C/2005 N5 (Catalina) | 1.627 | 0.943 | 21.4 | 153.6 | 1.633 | |
| C/2005 O2 (Christensen) | 3.334 | 0.859 | 148.9 | 115.4 | -1.650 | |
| P/2005 T4 (SWAN) | 0.649 | 0.930 | 160.0 | 28.5 | -0.365 | |
| P/2006 HR30 (Siding Spring) | 1.226 | 0.843 | 31.9 | 21.9 | 1.785 | |
| C/2008 R3 (LINEAR) | 1.909 | 0.896 | 43.2 | 79.0 | 1.498 | |
| P/2008 Y12 (SOHO) | 0.065 | 0.979 | 23.3 | 5.4 | 1.980 | |
| P/2010 D2 (WISE) | 3.659 | 0.453 | 57.2 | 17.3 | 1.874 | |
| P/2010 JC81 (WISE) | 1.811 | 0.777 | 38.7 | 23.2 | 1.868 | |
| C/2010 L5 (WISE) | 0.791 | 0.904 | 147.0 | 23.7 | -0.273 | |
| C/2011 J3 (LINEAR) | 1.451 | 0.926 | 114.7 | 86.5 | -0.347 | |
| C/2011 L1 (McNaught) | 2.242 | 0.797 | 65.5 | 36.7 | 1.201 | |
| C/2011 S2 (Kowalski) | 1.115 | 0.932 | 17.6 | 65.8 | 1.546 | |
| C/2012 H2 (McNaught) | 1.717 | 0.894 | 92.8 | 64.8 | 0.244 | |
| P/2012 NJ (La Sagra) | 1.292 | 0.848 | 84.4 | 24.8 | 0.745 | |
| C/2012 T6 (Kowalski) | 1.775 | 0.876 | 33.3 | 54.4 | 1.700 | |
| C/2012 Y3 (McNaught) | 1.765 | 0.940 | 73.2 | 159.3 | 0.645 | |
| P/2013 AL76 (Catalina) | 2.047 | 0.684 | 144.9 | 16.5 | -0.528 | |
| C/2013 V3 (Nevski) | 1.387 | 0.891 | 32.1 | 45.4 | 1.611 | комета C/2013 V3 Невского |
| C/2014 J1 (Catalina) | 1.709 | 0.802 | 159.7 | 25.4 | -0.841 | |
| C/2014 Q3 (Borisov) | 1.647 | 0.942 | 89.9 | 151.6 | 0.184 | комета C/2014 Q3 Борисова |
| C/2014 W7 (Christensen) | 1.488 | 0.869 | 98.3 | 38.4 | 0.245 | |
| C/2014 W9 (PANSTARRS) | 1.587 | 0.858 | 10.6 | 37.3 | 1.946 | |
| C/2015 A1 (PANSTARRS) | 1.996 | 0.901 | 80.4 | 90.2 | 0.544 | |
| P/2015 A3 (PANSTARRS) | 1.153 | 0.846 | 172.5 | 20.5 | -0.573 | |
| C/2015 D1 (SOHO) | 0.028 | 0.994 | 69.6 | 11.1 | 1.115 | |
| C/2015 F5 (SWAN-Xingming) | 0.346 | 0.978 | 149.3 | 61.3 | -0.289 | |
| C/2015 GX (PANSTARRS) | 1.972 | 0.878 | 90.3 | 65.1 | 0.314 | |
| C/2015 H1 (Bressi) | 1.926 | 0.941 | 140.7 | 185.6 | -1.151 | |
| P/2015 Q2 (Pimentel) | 1.819 | 0.754 | 146.2 | 20.2 | -0.599 | |
| C/2015 X2 (Catalina) | 1.905 | 0.879 | 72.5 | 62.5 | 0.830 | |
| C/2015 X8 (NEOWISE) | 1.190 | 0.939 | 155.3 | 86.4 | -0.944 | |
| C/2015 YG1 (NEOWISE) | 2.073 | 0.879 | 57.3 | 71.1 | 1.237 | |
| C/2016 S1 (PANSTARRS) | 2.412 | 0.709 | 94.7 | 23.8 | 0.483 | |
| P/2016 WM48 (Lemmon) | 1.748 | 0.787 | 117.5 | 23.5 | -0.082 | |
| C/2017 C1 (NEOWISE) | 1.502 | 0.928 | 65.8 | 94.9 | 0.863 | |
| C/2017 E2 (Tsuchinshan) | 2.353 | 0.891 | 79.2 | 100.1 | 0.589 | |
| P/2017 G2 (PANSTARRS) | 2.846 | 0.650 | 47.9 | 23.2 | 1.913 | |
| P/2017 TW13 (Lemmon) | 2.079 | 0.710 | 44.8 | 19.2 | 1.899 | |
| C/2017 W2 (Leonard) | 3.957 | 0.711 | 98.2 | 50.7 | 0.055 | |
| P/2017 Y3 (Leonard) | 1.275 | 0.871 | 27.6 | 31.0 | 1.728 | |
| C/2018 A1 (PANSTARRS) | 2.419 | 0.904 | 53.6 | 127.3 | 1.324 | |
| C/2018 A6 (Gibbs) | 3.018 | 0.803 | 77.0 | 60.2 | 0.801 | |
| C/2018 DO4 (Lemmon) | 2.406 | 0.907 | 160.5 | 131.5 | -1.569 | |
| C/2018 EN4 (NEOWISE) | 1.448 | 0.921 | 81.6 | 79.1 | 0.497 | |
| C/2018 K1 (Weiland) | 1.879 | 0.937 | 164.2 | 163.7 | -1.436 | |
| C/2018 M1 (Catalina) | 1.303 | 0.939 | 37.3 | 98.1 | 1.354 | |
| C/2018 O1 (ATLAS) | 1.558 | 0.944 | 154.0 | 147.2 | -1.185 | |
| C/2018 R5 (Lemmon) | 3.621 | 0.842 | 103.8 | 109.3 | -0.311 | |
| C/2018 V2 (ATLAS) | 2.475 | 0.903 | 159.1 | 128.6 | -1.574 | |
| C/2018 W1 (Catalina) | 1.360 | 0.938 | 83.3 | 101.9 | 0.405 | |
| C/2018 X3 (PANSTARRS) | 2.699 | 0.783 | 43.4 | 43.8 | 1.817 | |
| C/2019 L2 (NEOWISE) | 1.622 | 0.937 | 152.2 | 129.9 | -1.171 | |
| C/2019 T5 (ATLAS) | 1.529 | 0.809 | 33.4 | 22.7 | 1.866 | |
| C/2020 M3 (ATLAS) | 1.268 | 0.953 | 23.5 | 138.9 | 1.460 | |
| C/2020 S2 (PANSTARRS) | 1.756 | 0.827 | 22.4 | 32.5 | 1.963 | |
| C/2021 J1 (Maury-Attard) | 1.741 | 0.934 | 92.7 | 136.6 | 0.120 | |
| P/2021 U3 (Attard-Maury) | 1.887 | 0.550 | 70.0 | 8.6 | 1.755 | |
| C/2022 F2 (NEOWISE) | 1.585 | 0.934 | 97.3 | 117.1 | 0.022 | |
| C/2022 P1 (NEOWISE) | 1.595 | 0.913 | 154.6 | 79.1 | -1.102 | |
| C/2022 Q2 (ATLAS) | 1.644 | 0.950 | 151.5 | 187.9 | -1.221 | |
| C/2022 S5 (PANSTARRS) | 2.179 | 0.893 | 136.5 | 92.5 | -1.038 | |
| C/2022 Y2 (Lemmon) | 2.545 | 0.870 | 165.9 | 87.1 | -1.591 | |
| C/2023 E1 (ATLAS) | 1.027 | 0.947 | 38.3 | 85.0 | 1.242 | |
| C/2023 S3 (Lemmon) | 0.830 | 0.971 | 140.5 | 152.2 | -0.683 |