The following is a list of Halley-type comets (HTCs), which are periodic comets with an orbital period between 20 and 200 years, often appearing only once or twice within one's lifetime. The majority come from between the orbits of Saturn and Neptune. Due to the nature of their orbits, they can be perturbed by the giant planets and sent into orbits too far from the Sun to outgas, and vice versa. Minor planets in comet-like orbits similar to HTCs that never come close enough to the Sun to outgas are called centaurs. HTCs are named after the first discovered member, and the first discovered periodic comet, Halley's Comet, which orbits the Sun in about 75 years, and passing as far as the orbit of Neptune.
Most of the comets that have a period between 20 and 200 years (making them HTCs based on the classical definition) are actually officially classified as either Jupiter-family comets (JFCs) or Chiron-type comets (CTCs), based on their Jupiter Tisserand's parameter (TJupiter). Although JFCs are classically defined by (P < 20 y), they're officially defined by (2 < TJupiter < 3). CTCs, on the other hand, are officially defined by (TJupiter > 3; a > aJupiter). Since they do not include any period-related constraints, some of the 20–200 year-period comets unfortunately match one of the classifications, making comet classifications even more vague.
For the 14 numbered HTCs, see the list of numbered comets, where they are labelled "HTC" in column "class".
This list contains only Halley-type comets which are not numbered yet because they have been observed only once. Comets that belong to a different comet classification based on its Jupiter Tisserand parameter are given its alternative classification next to the comets' name.
Comet designation | Name/ discoverer(s) | Period (years) | e | a (AU) | q (AU) | i (°) | Abs. mag (M1) | Last observed perihelion | Next perihelion | Ref |
---|---|---|---|---|---|---|---|---|---|---|
C/1917 F1 | Mellish | 145 | 0.993121 | 27.6473325 | 0.190186 | 32.6828 | 1917/04/11 | 2062 | MPC · JPL | |
C/1921 H1 | Dubiago | 70.8 | 0.9348 | 17.102 | 1.116 | 22.34 | 1921/05/04 | 2062 | MPC · JPL | |
C/1937 D1 | Wilk | 187 | 0.981098 | 32.7445244 | 0.618937 | 26.0205 | 1937/02/21 | 2124 | MPC · JPL | |
C/1942 EA | Väisälä | 85.4 | 0.933639 | 19.3951116 | 1.287079 | 37.9961 | 1942/02/15 | 2027/07/10 | MPC · JPL | |
C/1984 A1 | Bradfield 1 | 152.3 | 0.9524 | 28.5 | 1.35751 | 51.8005 | 9.6 | 1983/12/27 | 2136/04/01 | MPC · JPL |
C/1989 A3 | Bradfield | 81.9 | 0.977708 | 18.853 | 0.420271 | 83.0672 | 1988/12/05 | 2070/11/01 | MPC · JPL | |
C/1991 L3 | Levy | 51.28 | 0.928811 | 13.8018 | 0.982545 | 19.19031 | 8.8 | 1991/07/08 | 2042/10/19 | MPC · JPL |
C/1998 G1 | LINEAR | 42.08 | 0.8237 | 12.099 | 2.1333 | 109.714 | 10.8 | 1998/11/16 | 2040/12/15 | MPC · JPL |
C/1998 Y1 | LINEAR | 110 | 0.9239 | 22.956 | 1.74699 | 28.1082 | 14 | 1998/11/21 | 2108/11/15 | MPC · JPL |
C/1999 E1 | Li | 66.06 | 0.76011 | 16.341 | 3.92002 | 46.88108 | 8.3 | 1998/01/31 | 2065/02/21 | MPC · JPL |
C/1999 G1 | LINEAR | 149 | 0.856 | 28.1 | 4.048 | 76.55 | 8 | 1998/08/01 | 2150 | MPC · JPL |
C/1999 K4 | LINEAR | 70 | 0.92 | 20 | 1.442 | 120.8 | 18.5 | 1999/05/16 | 2069/06/08 | MPC · JPL |
C/1999 S3 | LINEAR | 82.43 | 0.89995 | 18.94 | 1.894939 | 70.5607 | 4.9 | 1999/11/09 | 2081/04/04 | MPC · JPL |
C/1999 XS87 | LINEAR (*JFC) | 72.5 | 0.84057 | 17.386 | 2.7718 | 14.8464 | 10.9 | 1999/08/06 | 2072/02/04 | MPC · JPL |
C/2000 D2 | LINEAR | 72 | 0.867 | 17.2 | 2.2975 | 156.992 | 13.7 | 2000/03/08 | 2072 | MPC · JPL |
C/2000 G2 | LINEAR | 52 | 0.805 | 14 | 2.716 | 170.4785 | 12.8 | 2000/02/05 | 2052 | MPC · JPL |
C/2000 S3 | LONEOS (*JFC) | 39.97 | 0.7723 | 11.69 | 2.6622 | 25.164 | 6.4 | 2000/07/16 | 2040/07/10 | MPC · JPL |
C/2001 M10 | NEAT (*JFC) | 137.63 | 0.80107 | 26.657 | 5.30275 | 28.08349 | 9.4 | 2001/06/21 | 2139/02/01 | MPC · JPL |
C/2001 OG108 | LONEOS | 48.5 | 0.9252595 | 13.3 | 0.9940479 | 80.24505 | 13.2 | 2002/03/15 | 2050/09/13 | MPC · JPL |
P/2001 Q6 | NEAT | 22.61 | 0.82386 | 7.9946 | 1.408179 | 56.8553 | 13.3 | 2001/11/09 | 2024/06/20 | MPC · JPL |
C/2001 W2 | BATTeRS | 75.89 | 0.94136 | 17.925 | 1.051065 | 115.9131 | 12.1 | 2001/12/23 | 2077/11/15 | MPC · JPL |
C/2002 A1 | LINEAR (*JFC) | 70.04 | 0.72281 | 16.992 | 4.70996 | 14.03393 | 8.6 | 2001/11/26 | 2071/12/11 | MPC · JPL |
C/2002 A2 | LINEAR (*JFC) | 70.74 | 0.72482 | 17.103 | 4.70659 | 14.0386 | 7.5 | 2001/12/05 | 2072/09/01 | MPC · JPL |
C/2002 B1 | LINEAR | 31.24 | 0.77102 | 9.9183 | 2.27113 | 51.0214 | 6.3 | 2002/04/20 | 2032/06/17 | MPC · JPL |
C/2002 CE10 | LINEAR | 30.75 | 0.791486 | 9.81595 | 2.0467593 | 145.4587 | 10.8 | 2003/06/22 | 2034/03/23 | MPC · JPL |
C/2002 K4 | NEAT | 73.41 | 0.84232 | 17.532 | 2.76453 | 94.0632 | 11.4 | 2002/07/12 | 2075/12/01 | MPC · JPL |
C/2003 E1 | NEAT (*JFC) | 50.86 | 0.76359 | 13.7263 | 3.245004 | 33.53785 | 10.6 | 2004/02/13 | 2054/12/24 | MPC · JPL |
C/2003 F1 | LINEAR | 93.93 | 0.80605 | 20.664 | 4.007806 | 70.2216 | 8.3 | 2003/06/28 | 2097/06/02 | MPC · JPL |
P/2003 QX29 | NEAT (*JFC) | 22.74 | 0.4718 | 8.0255 | 4.239 | 11.3965 | 6.1 | 2002/10/26 | 2025/07/21 | MPC · JPL |
C/2003 R1 | LINEAR | 87.44 | 0.89331 | 19.7 | 2.10188 | 149.19563 | 12.7 | 2003/06/29 | 2090/12/15 | MPC · JPL |
C/2003 U1 | LINEAR | 109.6 | 0.9216 | 22.9 | 1.79572 | 164.4745 | 15.2 | 2003/11/03 | 2113 | MPC · JPL |
C/2003 W1 | LINEAR | 126.1 | 0.93429 | 25.15 | 1.65241 | 78.0756 | 13.5 | 2003/11/09 | 2130 | MPC · JPL |
C/2004 C1 | Larsen (*JFC) | 39.33 | 0.6231 | 11.566 | 4.3594 | 28.918 | 10 | 2003/03/19 | 2042/09/01 | MPC · JPL |
P/2004 DO29 | Spacewatch–LINEAR (*JFC) | 20.4 | 0.45151 | 7.4655 | 4.09475 | 14.5358 | 10.3 | 2004/10/11 | 2025/03/06 | MPC · JPL |
P/2004 V5-A | LINEAR–Hill (*JFC) | 22.42 | 0.445217 | 7.95059 | 4.410853 | 19.358136 | 8.8 | 2005/02/28 | 2027/07/31 | MPC · JPL |
P/2004 V5-B | LINEAR–Hill (*JFC) | 22.42 | 0.445233 | 7.95092 | 4.41091 | 19.35822 | 9.2 | 2005/03/01 | 2027/08/02 | MPC · JPL |
C/2005 N5 | Catalina | 153.65 | 0.94327 | 28.687 | 1.6274 | 21.37879 | 12.9 | 2005/08/22 | 2159/01/01 | MPC · JPL |
C/2005 O2 | Christensen | 115.43 | 0.85939 | 23.707 | 3.33358 | 148.89204 | 5.2 | 2005/09/08 | 2121/02/15 | MPC · JPL |
P/2005 S2 | Skiff (*CTC) | 22.48 | 0.1967 | 7.965 | 6.398 | 3.141 | 7.9 | 2006/06/30 | 2028/12/22 | MPC · JPL |
P/2005 T3 | Read (*CTC) | 20.58 | 0.174 | 7.509 | 6.202 | 6.26 | 9.2 | 2006/01/13 | 2026/08/15 | MPC · JPL |
P/2005 T4 | SWAN | 28.4 | 0.93 | 9.3 | 0.649399 | 160.0362 | 15.4 | 2005/10/10 | 2034 | MPC · JPL |
C/2005 W2 | Christensen (*JFC) | 82.68 | 0.82446 | 18.979 | 3.33162 | 11.26403 | 10.8 | 2006/03/27 | 2096/12/01 | MPC · JPL |
C/2006 F2 | Christensen (*JFC) | 43.27 | 0.65138 | 12.324 | 4.2965 | 20.511 | 10.6 | 2006/05/30 | 2049/09/06 | MPC · JPL |
P/2006 HR30 | Siding Spring | 21.86 | 0.8431184 | 7.81754 | 1.2264277 | 31.884499 | 11.7 | 2007/01/02 | 2028/11/12 | MPC · JPL |
C/2006 U7 | Gibbs (*JFC) | 41.51 | 0.6309 | 11.99 | 4.425 | 57.762 | 11.6 | 2007/03/28 | 2048/10/01 | MPC · JPL |
C/2007 S2 | Lemmon (*JFC) | 44.45 | 0.557056 | 12.5477 | 5.557931 | 16.86305 | 9 | 2008/09/14 | 2053/02/25 | MPC · JPL |
C/2008 E1 | Catalina (*JFC) | 34.94 | 0.54815 | 10.687 | 4.82891 | 35.03769 | 9.1 | 2008/08/11 | 2043/07/31 | MPC · JPL |
P/2008 O3 | Boattini (*JFC) | 23.42 | 0.6949 | 8.186 | 2.4973 | 32.2699 | 5.1 | 2008/06/03 | 2031/11/03 | MPC · JPL |
C/2008 R3 | LINEAR | 79.11 | 0.89641 | 18.428 | 1.909035 | 43.23793 | 13.5 | 2008/11/22 | 2088/01/01 | MPC · JPL |
P/2008 Y3 | McNaught (*JFC) | 22.75 | 0.44766 | 8.0281 | 4.434241 | 38.81318 | 8.7 | 2009/01/11 | 2031/10/12 | MPC · JPL |
P/2009 O3 | Hill (*JFC) | 21.89 | 0.68688 | 7.8244 | 2.44999 | 16.2176 | 12 | 2009/05/18 | 2031/04/08 | MPC · JPL |
P/2009 Q5 | McNaught (*JFC) | 20.4 | 0.609061 | 7.4654 | 2.91851 | 40.9048 | 10.5 | 2009/09/08 | 2030/02/02 | MPC · JPL |
P/2009 T2 | La Sagra (*JFC) | 20.94 | 0.768991 | 7.596 | 1.75475 | 28.10639 | 14.2 | 2010/01/12 | 2030/12/21 | MPC · JPL |
P/2010 E2 | Jarnac (*JFC) | 25.4 | 0.72237 | 8.6402 | 2.39874 | 15.437 | 14.4 | 2010/04/07 | 2035/08/31 | MPC · JPL |
C/2010 E5 | Scotti (*JFC) | 122.96 | 0.84274 | 24.73 | 3.8884 | 18.9102 | 6.1 | 2009/11/21 | 2132/11/01 | MPC · JPL |
P/2010 J3 | McMillan (*JFC) | 26.94 | 0.72682 | 8.9871 | 2.45511 | 13.25507 | 11.6 | 2010/08/23 | 2037/08/01 | MPC · JPL |
P/2010 JC81 | WISE | 23.19 | 0.77735 | 8.13307 | 1.8108311 | 38.69025 | 10.3 | 2011/04/26 | 2034/07/04 | MPC · JPL |
C/2010 L5 | WISE | 23.6 | 0.904 | 8.2 | 0.7909 | 147.052 | 17.4 | 2010/04/23 | 2033 | MPC · JPL |
C/2011 J3 | LINEAR | 86.5 | 0.9258 | 19.56 | 1.451 | 114.7124 | 13.1 | 2011/01/24 | 2097 | MPC · JPL |
P/2011 JB15 | Spacewatch–Boattini | 20 | 0.31874 | 7.3668 | 5.01871 | 19.14127 | 5.5 | 2012/01/21 | 2032/01/21 | MPC · JPL |
C/2011 L1 | McNaught | 36.66 | 0.79678 | 11.034 | 2.24237 | 65.512 | 10.6 | 2010/12/18 | 2047/08/15 | MPC · JPL |
P/2011 P1 | McNaught (*JFC) | 21.54 | 0.3598 | 7.741 | 4.9556 | 6.1741 | 8.2 | 2010/07/22 | 2032/02/04 | MPC · JPL |
C/2011 P2 | PANSTARRS (*CTC) | 30.47 | 0.36982 | 9.7562 | 6.1481 | 8.98964 | 6.7 | 2010/09/13 | 2041/03/04 | MPC · JPL |
P/2011 S1 | Gibbs (*CTC) | 25.46 | 0.20305 | 8.6545 | 6.8972 | 2.6792 | 5.5 | 2014/08/20 | 2040/02/04 | MPC · JPL |
C/2011 S2 | Kowalski | 65.83 | 0.9316 | 16.304 | 1.115118 | 17.57253 | 14.8 | 2011/10/26 | 2077/08/25 | MPC · JPL |
C/2011 Y3 | Boattini (*JFC) | 40.82 | 0.705 | 11.85 | 3.4978 | 26.517 | 11.7 | 2011/08/22 | 2052/06/17 | MPC · JPL |
C/2012 BJ98 | Lemmon [1] (*JFC) | 70.52 | 0.87365 | 17.068 | 2.156577 | 2.6369 | 8.1 | 2012/09/20 | 2083/03/29 | MPC · JPL |
P/2012 C3 | PANSTARRS (*JFC) | 30.2 | 0.6264 | 9.7 | 3.625 | 9.19 | 13.5 | 2011/10/05 | 2042 | MPC · JPL |
C/2012 H2 | McNaught | 64.9 | 0.8936 | 16.14 | 1.71678 | 92.8355 | 15.7 | 2012/05/03 | 2077 | MPC · JPL |
P/2012 NJ | La Sagra | 24.79 | 0.848062 | 8.5027 | 1.2918901 | 84.37546 | 13.1 | 2012/06/13 | 2037/03/28 | MPC · JPL |
C/2012 Q1 | Kowalski (*JFC) | 133.63 | 0.63722 | 26.138 | 9.48222 | 45.181 | 4.7 | 2012/02/09 | 2145/10/01 | MPC · JPL |
C/2012 T6 | Kowalski | 54.38 | 0.87634 | 14.354 | 1.77509 | 33.2755 | 15.7 | 2012/08/26 | 2067/01/15 | MPC · JPL |
C/2012 X2 | PANSTARRS (*JFC) | 94.12 | 0.77052 | 20.69 | 4.74816 | 34.12389 | 9.6 | 2013/03/31 | 2107/05/14 | MPC · JPL |
C/2012 Y3 | McNaught | 159.3 | 0.93993 | 29.38 | 1.76482 | 73.2318 | 10.4 | 2012/08/25 | 2172 | MPC · JPL |
C/2013 C2 | Tenagra (*CTC) | 64.01 | 0.4293 | 16.001 | 9.1321 | 21.34426 | 4.4 | 2015/08/28 | 2080/09/01 | MPC · JPL |
C/2013 D1 | Holvorcem (*JFC) | 37.62 | 0.78088 | 11.227 | 2.46013 | 10.09356 | 13.5 | 2013/04/13 | 2050/11/25 | MPC · JPL |
P/2013 N3 | PANSTARRS (*JFC) | 20.26 | 0.5924 | 7.431 | 3.0289 | 2.17041 | 6.6 | 2014/02/11 | 2034/05/17 | MPC · JPL |
P/2013 P1 | PANSTARRS (*JFC) | 25.17 | 0.6053 | 8.588 | 3.3902 | 18.702 | 11.6 | 2013/02/26 | 2038/04/29 | MPC · JPL |
C/2013 P4 | PANSTARRS (*CTC) | 56.84 | 0.59636 | 14.783 | 5.96703 | 4.26425 | 5.1 | 2014/08/12 | 2071/06/15 | MPC · JPL |
C/2013 U1 | Catalina (*JFC) | 41.17 | 0.7971 | 11.92 | 2.4188 | 23.9415 | 13.9 | 2013/11/18 | 2055/01/01 | MPC · JPL |
C/2013 V3 | Nevsky | 45.36 | 0.89097 | 12.718 | 1.386693 | 32.1345 | 15.2 | 2013/10/29 | 2059/03/09 | MPC · JPL |
C/2013 W2 | PANSTARRS (*JFC) | 32.23 | 0.561 | 10.13 | 4.448 | 4.5436 | 5.8 | 2015/01/08 | 2047/03/15 | MPC · JPL |
C/2014 F3 | Sheppard–Trujillo (*JFC) | 66 | 0.65 | 16.3 | 5.7 | 6.48 | 6.1 | 2021/04/17 | 2087 | MPC · JPL |
C/2014 HU195 | Valdes–TOTAS (*JFC) | 102.25 | 0.76580 | 21.867 | 5.12113 | 5.82227 | 14.6 | 2015/05/18 | 2117/08/14 | MPC · JPL |
C/2014 J1 | Catalina | 25.4 | 0.802 | 8.64 | 1.7085 | 159.696 | 16.8 | 2014/06/20 | 2039 | MPC · JPL |
P/2014 L3 | Hill (*JFC) | 23.36 | 0.77309 | 8.1706 | 1.85396 | 6.264 | 13.7 | 2014/06/28 | 2037/11/06 | MPC · JPL |
P/2014 O3 | PANSTARRS (*JFC) | 20.72 | 0.3847 | 7.544 | 4.642 | 7.81 | 10.4 | 2014/04/16 | 2035/01/04 | MPC · JPL |
C/2014 Q3 | Borisov | 151.64 | 0.94207 | 28.436 | 1.647408 | 89.94888 | 8.8 | 2014/11/19 | 2166/07/10 | MPC · JPL |
C/2014 TG64 | Catalina (*JFC) | 22.283 | 0.7824 | 14.89 | 3.24 | 3.2391 | 6.4 | 2014/05/26 | 2072 | MPC · JPL |
C/2014 W7 | Christensen | 38 | 0.869 | 11.3 | 1.4881 | 98.314 | 16.3 | 2014/12/31 | 2052 | MPC · JPL |
C/2014 W9 | PANSTARRS | 37.28 | 0.8577 | 11.16 | 1.5874 | 10.6302 | 15.5 | 2015/02/15 | 2052/04/01 | MPC · JPL |
C/2014 W11 | PANSTARRS (*JFC) | 30.67 | 0.650255 | 9.7980 | 3.426805 | 12.70679 | 8.8 | 2015/06/17 | 2036/04/16 | MPC · JPL |
C/2015 A1 | PANSTARRS | 90.24 | 0.900816 | 20.119 | 1.995505 | 80.36576 | 6.9 | 2015/03/13 | 2105/06/09 | MPC · JPL |
P/2015 A3 | PANSTARRS | 21 | 0.85 | 7.6 | 1.154 | 172.51 | 20.2 | 2015/02/22 | 2036 | MPC · JPL |
P/2015 B1 | PANSTARRS (*JFC) | 30.10 | 0.38250 | 9.6772 | 5.97567 | 18.027 | 8.7 | 2015/09/19 | 2045/10/26 | MPC · JPL |
P/2015 B4 | Lemmon–PANSTARRS (*JFC) | 25.72 | 0.56894 | 8.7121 | 3.75540 | 1.74262 | 11.7 | 2015/02/17 | 2030/12/04 | MPC · JPL |
C/2015 D2 | PANSTARRS (*JFC) | 46.79 | 0.56826 | 12.985 | 5.6060 | 31.8339 | 6.3 | 2013/09/27 | 2060/07/13 | MPC · JPL |
C/2015 D5 | Kowalski (*JFC) | 27.66 | 0.4996 | 9.145 | 4.576 | 20.3990 | 6.0 | 2014/04/16 | 2041/12/12 | MPC · JPL |
C/2015 F5 | SWAN–XingMing | 60.9 | 0.97764 | 15.47 | 0.345995 | 149.2590 | 17.6 | 2015/03/28 | 2075/02/01 | MPC · JPL |
C/2015 GX | PANSTARRS | 65.13 | 0.878198 | 16.1883 | 1.971753 | 90.25454 | 14.4 | 2015/08/26 | 2080/10/09 | MPC · JPL |
C/2015 H1 | Bressi | 185.5 | 0.94078 | 32.53 | 1.92636 | 140.65558 | 6.6 | 2015/03/28 | 2200/10/07 | MPC · JPL |
P/2015 Q2 | Pimentel | 20.16 | 0.7544 | 7.407 | 1.81912 | 146.2022 | 15.3 | 2015/09/10 | 2035/11/06 | MPC · JPL |
C/2015 T5 | Sheppard–Tholen (*CTC) | 147.9 | 0.6661 | 27.97 | 9.3383 | 11.0483 | 7.7 | 2016/01/24 | 2164 | MPC · JPL |
C/2015 V4 | PANSTARRS | 79.89 | 0.70567 | 18.550 | 5.45972 | 60.7513 | 8.7 | 2016/08/27 | 2096/07/19 | MPC · JPL |
C/2015 X2 | PANSTARRS | 62.5 | 0.8791 | 15.75 | 1.90456 | 72.458 | 16.1 | 2015/12/20 | 2078/06/25 | MPC · JPL |
C/2015 X4 | Elenin (*JFC) | 77.23 | 0.812807 | 18.1345 | 3.39466 | 29.50491 | 10.1 | 2015/11/03 | 2093/02/14 | MPC · JPL |
C/2015 X8 | NEOWISE | 86.9 | 0.9393 | 19.6 | 1.1903 | 155.2817 | 14.1 | 2015/10/23 | 2099/09/13 | MPC · JPL |
C/2015 YG1 | NEOWISE | 71.14 | 0.87924 | 17.169 | 2.07341 | 57.3360 | 12.3 | 2015/09/28 | 2086/11/17 | MPC · JPL |
P/2016 A3 | PANSTARRS (*JFC) | 21.36 | 0.3778 | 7.6979 | 4.7895 | 8.5929 | 5.4 | 2017/04/13 | 2038/08/22 | MPC · JPL |
C/2016 Q4 | Kowalski (*CTC) | 68.8 | 0.5781 | 16.79 | 7.084 | 7.2567 | 7.0 | 2018/01/28 | 2086 | MPC · JPL |
C/2016 S1 | PANSTARRS | 23.85 | 0.70887 | 8.285 | 2.41193 | 94.6898 | 7.5 | 2017/03/16 | 2041/01/20 | MPC · JPL |
P/2016 WM48 | Lemmon | 23.46 | 0.7867 | 8.1954 | 1.7480 | 117.5476 | 16.8 | 2017/02/26 | 2040 | MPC · JPL |
C/2017 C1 | NEOWISE | 92.08 | 0.9263697 | 20.7832 | 1.50172 | 65.73154 | 2017/01/19 | 2109 | MPC · JPL | |
P/2017 D4 | PANSTARRS (*JFC) | 20.23 | 0.62898 | 7.424 | 2.7545 | 10.3396 | 12.7 | 2016/09/06 | 2036/11/29 | MPC · JPL |
C/2017 E2 | Tsuchinshan | 100.09 | 0.89085 | 21.5567 | 2.35295 | 79.1686 | 11.3 | 2016/05/12 | 2116/06/14 | MPC · JPL |
P/2017 G1 | PANSTARRS (*JFC) | 21.53 | 0.66134 | 7.7387 | 2.621 | 3.534 | 13.1 | 2016/05/14 | 2037/11/23 | MPC · JPL |
P/2017 G2 | PANSTARRS | 23.22 | 0.65031 | 8.1394 | 2.846 | 47.90625 | 12.9 | 2017/06/13 | 2040/09/02 | MPC · JPL |
C/2017 K4 | ATLAS (*JFC) | 148.87 | 0.90571 | 28.0883 | 2.64824 | 16.67822 | 7.2 | 2018/01/08 | 2167 | MPC · JPL |
P/2017 P1 | PANSTARRS (*JFC) | 22.06 | 0.3088 | 7.86566 | 5.43665 | 7.7013 | 10.1 | 2018/06/18 | 2040/07/10 | MPC · JPL |
C/2017 S2 | PANSTARRS (*JFC) | 93.09 | 0.82406 | 20.5400 | 3.613 | 12.67723 | 13.2 | 2017/08/28 | 2110 | MPC · JPL |
C/2017 U5 | PANSTARRS (*JFC) | 69.72 | 0.74457 | 16.939 | 4.32676 | 18.9566 | 11.8 | 2017/12/19 | 2087/09/07 | MPC · JPL |
C/2017 W2 | Leonard | 50.81 | 0.7115 | 13.7176 | 3.958 | 98.1831 | 10.9 | 2017/11/02 | 2068 | MPC · JPL |
P/2017 W3 | Gibbs (*JFC) | 21.51 | 0.5039 | 7.734 | 3.8373 | 18.317 | 10.5 | 2018/02/25 | 2039/08/30 | MPC · JPL |
C/2017 X1 | PANSTARRS (*JFC) | 175.19 | 0.8511 | 31.3092 | 4.6624 | 31.3106 | 9.6 | 2018/06/14 | 2193 | MPC · JPL |
P/2017 Y3 | Leonard | 30.86 | 0.8703 | 9.838 | 1.2753 | 27.5859 | 13.6 | 2018/02/11 | 2049 | MPC · JPL |
C/2018 A1 | PANSTARRS | 131.18 | 0.9061 | 25.8169 | 2.4233 | 53.6213 | 13.1 | 2017/10/20 | 2148 | MPC · JPL |
C/2018 A6 | Gibbs | 72.80 | 0.8273 | 17.434 | 3.011 | 77.454 | 8.9 | 2019/07/08 | 2092 | MPC · JPL |
C/2018 DO4 | Lemmon | 131.40 | 0.9069 | 29.847 | 2.406 | 160.475 | 13.7 | 2019/08/18 | 2151 | MPC · JPL |
C/2018 K1 | Weiland | 163.42 | 0.9371 | 29.890 | 1.879 | 164.193 | 11.9 | 2018/04/06 | 2182 | MPC · JPL |
C/2018 M1 | CSS | 103.81 | 0.9409 | 22.087 | 1.304 | 37.265 | 15.9 | 2018/07/10 | 2122 | MPC · JPL |
C/2018 O1 | ATLAS | 147.09 | 0.944 | 27.864 | 1.558 | 154.041 | 12.6 | 2018/08/31 | 2165 | MPC · JPL |
C/2018 R5 | Lemmon | 109.55 | 0.8418 | 22.8947 | 3.6213 | 103.76 | 6 | 2019/01/09 | 2128 | MPC · JPL |
C/2018 S2 | TESS | 53.55 | 0.6149 | 14.206 | 5.471 | 64.220 | 6.7 | 2018/11/05 | 2072 | MPC · JPL |
C/2018 V2 | ATLAS | 129.65 | 0.9034 | 25.616 | 2.475 | 159.111 | 14.5 | 2018/11/26 | 2148 | MPC · JPL |
C/2018 W1 | CSS | 101.64 | 0.938 | 21.779 | 1.36 | 83.273 | 15.648 | 2019/05/11 | 2120 | MPC · JPL |
C/2018 X3 | PANSTARRS | 43.75 | 0.783 | 12.41686 | 2.69887 | 43.368 | 15.5 | 2018/12/30 | 2062 | MPC · JPL |
P/2018 Y2 | Africano (*JFC) | 20.72 | 0.4878 | 7.543 | 3.8635 | 11.48886 | 11 | 2018/12/13 | 2039 | MPC · JPL |
C/2019 A5 | PANSTARRS | 100.81 | 0.7080 | 21.6608 | 6.3242 | 67.5310 | 9.4 | 2019/06/09 | 2119 | MPC · JPL |
C/2019 L1 | PANSTARRS (*JFC) | 30.90 | 0.7065 | 9.8474 | 2.88986 | 9.993 | 13.6 | 2019/08/11 | 2050 | MPC · JPL |
C/2019 L2 | NEOWISE | 130.48 | 0.9370 | 25.72 | 1.622 | 152.19 | 10.3 | 2019/04/02 | 2149 | MPC · JPL |
C/2019 LB7 | Kleyna | 208.14 | 0.9293 | 35.1204 | 2.483 | 164.23 | 18.1 | 2019/03/27 | 2227 | MPC · JPL |
C/2019 T5 | ATLAS | 22.69 | 0.8092 | 8.014 | 1.5289 | 33.42 | 14.9 | 2019/08/01 | 2042 | MPC · JPL |
P/2019 V2 | Groeller (*JFC) | 20.63 | 0.333 | 7.523 | 5.0183 | 11.8 | 9.8 | 2020/10/21 | 2041 | MPC · JPL |
C/2019 Y4-D | ATLAS | 111.65 | 0.9888 | 23.187 | 0.2589 | 44.02 | 14.5 | 2020/05/31 | 2132 | MPC · JPL |
C/2019 Y4-E | ATLAS | 87.94 | 0.987 | 19.775 | 0.2525 | 45.085 | 16.3 | 2020/05/31 | 2108 | MPC · JPL |
P/2020 A4 | PANSTARRS-Lemmon (*JFC) | 23.52 | 0.6537 | 8.208 | 2.843 | 24.99 | 15.6 | 2019/11/22 | 2043 | MPC · JPL |
C/2020 M3 | ATLAS | 138.88 | 0.9527 | 26.817 | 1.268 | 23.474 | 14.6 | 2020/10/25 | 2159 | MPC · JPL |
C/2020 Q2 | PANSTARRS (*JFC) | 36.10 | 0.5055 | 10.9231 | 5.402 | 3.310 | 10.9 | 2020/02/07 | 2056 | MPC · JPL |
C/2020 S2 | PANSTARRS | 32.48 | 0.8275 | 10.1793 | 1.756 | 22.3978 | 16.3 | 2020/12/21 | 2052 | MPC · JPL |
P/2020 V3 | PANSTARRS (*JFC) | 24.17 | 0.2547 | 8.36 | 6.23 | 23.035 | 8.6 | 2021/02/07 | 2045 | MPC · JPL |
P/2020 V4 | Rankin (*JFC) | 28.52 | 0.4484 | 9.3336 | 5.15 | 14.245 | 6.9 | 2021/07/18 | 2050 | MPC · JPL |
P/2021 C2 | PANSTARRS (*JFC) | 29.47 | 0.4874 | 9.5408 | 4.890 | 21.927 | 11.4 | 2021/02/24 | 2050 | MPC · JPL |
C/2021 J1 | Maury-Attard | 134.85 | 0.9338 | 26.296 | 1.74 | 92.710 | 13.4 | 2021/02/19 | 2155 | MPC · JPL |
P/2021 J3 | ATLAS (*JFC) | 26.69 | 0.4507 | 8.931 | 4.890 | 14.573 | 6.9 | 2019/07/03 | 2046 | MPC · JPL |
C/2021 K1 | ATLAS (*JFC) | 45.50 | 0.8040 | 12.745 | 2.498 | 16.276 | 6.2 | 2021/05/04 | 2066 | MPC · JPL |
P/2021 R1 | PANSTARRS (*JFC) | 24.64 | 0.4229 | 8.467 | 4.886 | 5.520 | 7.4 | 2021/12/16 | 2046 | MPC · JPL |
P/2021 U1 | Wierzchos | 24.83 | 0.7127 | 8.511 | 2.445 | 30.560 | 16.1 | 2021/09/30 | 2046 | MPC · JPL |
P/2021 V2 | Fuls (*JFC) | 27.15 | 0.6130 | 9.034 | 3.500 | 12.696 | 7.0 | 2023/01/21 | 2050 | MPC · JPL |
C/2022 F2 | NEOWISE | 117.13 | 0.934 | 23.939 | 1.585 | 97.293 | 15.8 | 2022/03/23 | 2139 | MPC · JPL |
C/2022 P1 | NEOWISE | 79.30 | 0.9136 | 18.458 | 1.595 | 154.607 | 10.0 | 2022/11/28 | 2102 | MPC · JPL |
C/2022 Q2 | ATLAS | 187.51 | 0.9498 | 32.760 | 1.644 | 151.49 | 13.9 | 2023/01/31 | 2210 | MPC · JPL |
C/2022 S5 | PANSTARRS | 92.51 | 0.8935 | 20.454 | 2.179 | 136.53 | 12.8 | 2022/11/27 | 2115 | MPC · JPL |
P/2022 Y1 | Hogan | 44.43 | 0.764 | 12.545 | 2.958 | 18.859 | 13.3 | 2022/11/27 | 2067 | MPC · JPL |
C/2022 Y2 | Lemmon | 87.14 | 0.871 | 19.655 | 2.545 | 165.907 | 7.5 | 2023/03/22 | 2110 | MPC · JPL |
C/2023 E1 | ATLAS | 85.02 | 0.947 | 19.334 | 1.027 | 38.313 | 16.2 | 2023/07/01 | 2108 | MPC · JPL |
C/2023 H3 | PANSTARRS | 50.39 | 0.616 | 13.642 | 5.233 | 2.489 | 7.2 | 2024/02/19 | 2074 | MPC · JPL |
C/2023 S3 | Lemmon | 152.38 | 0.971 | 28.529 | 0.83 | 140.498 | 16.7 | 2024/01/19 | 2164 | MPC · JPL |
C/2023 V3 | PANSTARRS | 48.17 | 0.662 | 13.239 | 4.472 | 40.259 | 11.6 | 2023/08/06 | 2071 | MPC · JPL |
A comet is an icy, small Solar System body that warms and begins to release gases when passing close to the Sun, a process called outgassing. This produces an extended, gravitationally unbound atmosphere or coma surrounding the nucleus, and sometimes a tail of gas and dust gas blown out from the coma. These phenomena are due to the effects of solar radiation and the outstreaming solar wind plasma acting upon the nucleus of the comet. Comet nuclei range from a few hundred meters to tens of kilometers across and are composed of loose collections of ice, dust, and small rocky particles. The coma may be up to 15 times Earth's diameter, while the tail may stretch beyond one astronomical unit. If sufficiently close and bright, a comet may be seen from Earth without the aid of a telescope and can subtend an arc of up to 30° across the sky. Comets have been observed and recorded since ancient times by many cultures and religions.
In planetary astronomy, a centaur is a small Solar System body that orbits the Sun between Jupiter and Neptune and crosses the orbits of one or more of the giant planets. Centaurs generally have unstable orbits because they cross or have crossed the orbits of the giant planets; almost all their orbits have dynamic lifetimes of only a few million years, but there is one known centaur, 514107 Kaʻepaokaʻawela, which may be in a stable orbit. Centaurs typically exhibit the characteristics of both asteroids and comets. They are named after the mythological centaurs that were a mixture of horse and human. Observational bias toward large objects makes determination of the total centaur population difficult. Estimates for the number of centaurs in the Solar System more than 1 km in diameter range from as low as 44,000 to more than 10,000,000.
12P/Pons–Brooks is a periodic comet with an orbital period of 71 years. It fits the classical definition of a Halley-type comet with an orbital period between 20 and 200 years, and is also one of the brightest known periodic comets, reaching an absolute visual magnitude ~5 in its approach to perihelion. Comet Pons-Brooks was discovered at Marseilles Observatory in July 1812 by Jean-Louis Pons, and then later recovered in 1883 by William Robert Brooks.
Damocloids are a class of minor planets such as 5335 Damocles and 1996 PW that have Halley-type or long-period highly eccentric orbits typical of periodic comets such as Halley's Comet, but without showing a cometary coma or tail. David Jewitt defines a damocloid as an object with a Jupiter Tisserand invariant (TJ) of 2 or less, while Akimasa Nakamura defines this group with the following orbital elements:
In astrodynamics, the orbital eccentricity of an astronomical object is a dimensionless parameter that determines the amount by which its orbit around another body deviates from a perfect circle. A value of 0 is a circular orbit, values between 0 and 1 form an elliptic orbit, 1 is a parabolic escape orbit, and greater than 1 is a hyperbola. The term derives its name from the parameters of conic sections, as every Kepler orbit is a conic section. It is normally used for the isolated two-body problem, but extensions exist for objects following a rosette orbit through the Galaxy.
The scattered disc (or scattered disk) is a distant circumstellar disc in the Solar System that is sparsely populated by icy small Solar System bodies, which are a subset of the broader family of trans-Neptunian objects. The scattered-disc objects (SDOs) have orbital eccentricities ranging as high as 0.8, inclinations as high as 40°, and perihelia greater than 30 astronomical units (4.5×109 km; 2.8×109 mi). These extreme orbits are thought to be the result of gravitational "scattering" by the gas giants, and the objects continue to be subject to perturbation by the planet Neptune.
167P/CINEOS (P/2004 PY42) is a large periodic comet and active, grey centaur, approximately 66 kilometers (41 miles) in diameter, orbiting the Sun outside the orbit of Saturn. It was discovered on August 10, 2004, by astronomers with the CINEOS survey at Gran Sasso in Italy. It is one of only a handful known Chiron-type comets.
Tisserand's parameter is a number calculated from several orbital elements of a relatively small object and a larger "perturbing body". It is used to distinguish different kinds of orbits. The term is named after French astronomer Félix Tisserand who derived it, and applies to restricted three-body problems in which the three objects all differ greatly in mass.
20898 Fountainhills, provisional designation 2000 WE147, is a dark asteroid in a cometary orbit (ACO) from the outermost regions of the asteroid belt, approximately 37 kilometers (23 miles) in diameter. It was discovered on 30 November 2000, by American amateur astronomer Charles W. Juels at the Fountain Hills Observatory in Arizona, United States. The D-type asteroid has a rotation period of 12.84 hours. It was named for the city of Fountain Hills, Arizona, in the United States.
An extinct comet is a comet that has expelled most of its volatile ice and has little left to form a tail and coma. In a dormant comet, rather than being depleted, any remaining volatile components have been sealed beneath an inactive surface layer.
38P/Stephan–Oterma is a periodic comet with an orbital period of 38 years. It fits the classical definition of a Halley-type comet with. It was discovered on 22.9 January 1867, by Jérôme Eugène Coggia at Marseilles Observatory, France. On 25.86 January Édouard Stephan confirmed it was a comet. It was recovered in 6 November 1942 by the Finnish astronomer Liisi Oterma.
2005 VX3 is trans-Neptunian object and retrograde damocloid on a highly eccentric, cometary-like orbit. It was first observed on 1 November 2005, by astronomers with the Mount Lemmon Survey at the Mount Lemmon Observatory in Arizona, United States. The unusual object measures approximately 7 kilometers (4 miles) in diameter. It has the 3rd largest known heliocentric semi-major axis and aphelion. Additionally its perihelion lies within the orbit of Jupiter, which means it also has the largest orbital eccentricity of any known minor planet.
2002 RN109 is a trans-Neptunian astronomical object and damocloid on a highly eccentric, cometary-like orbit. It was first observed on 6 September 2002, by astronomers of the Lincoln Near-Earth Asteroid Research project at its ETS near Socorro, New Mexico, United States. The unusual object is approximately 4 kilometers (2 miles) in diameter. It has the second-highest orbital eccentricity of any known minor planet, after 2005 VX3.
(127546) 2002 XU93, provisional designation 2002 XU93, is a trans-Neptunian object and centaur on highly inclined and eccentric orbit in the outer region of the Solar System. It measures approximately 170 kilometers (110 mi) in diameter and is one of few objects with such an unusual orbit. It was discovered on 4 December 2002, by American astronomer Marc Buie at the Kitt Peak National Observatory in Arizona, United States.
In planetary science, the term unusual minor planet, or unusual object, is used for a minor planet that possesses an unusual physical or orbital characteristic. For the Minor Planet Center (MPC), which operates under the auspices of the International Astronomical Union, any non-classical main-belt asteroid, which account for the vast majority of all minor planets, is an unusual minor planet. These include the near-Earth objects and Trojans as well as the distant minor planets such as centaurs and trans-Neptunian objects. In a narrower sense, the term is used for a group of bodies – including main-belt asteroids, Mars-crossers, centaurs and otherwise non-classifiable minor planets – that show a high orbital eccentricity, typically above 0.5 and/or a perihelion of less than 6 AU. Similarly, an unusual asteroid (UA) is an inner Solar System object with a high eccentricity and/or inclination but with a perihelion larger than 1.3 AU, which does exclude the near-Earth objects.
A Chiron-type comet (CTC) is a member of a small family of comets defined as having a semi-major axis larger than that of Jupiter (5.2 AU) and a Tisserand's parameter with respect to Jupiter (TJupiter) of more than 3.