Weekly Information about Bright Comets (2026 Oct. 10: North)

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Updated on October 18, 2026
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Best time and the azimuth, altitude (A,h) are at lat. 35 deg in the Northern Hemisphere.
Azimuth indicates 0 for south, 90 for west, 180 for north, 270 for east.

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* 10P/Tempel 2

It brightened up to 6.9 mag in summer (Aug. 5, Juan Jose Gonzalez). Now it is 11.2 mag (Oct. 13, Yoshimi Nagai). It will fade out rapidly after this. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  22 56.79  -31 59.7   0.738   1.588   131   10.2  21:42 (  0, 23)  
Oct. 17  23  4.66  -30 23.9   0.804   1.621   127   10.5  21:22 (  0, 25)  

* 161P/Hartley-IRAS

Now it is 10.3 mag (Oct. 9, Toru Yusa). Fading gradually. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  21 51.83    2 15.5   0.548   1.429   132   10.4  20:32 (  0, 58)  
Oct. 17  20 58.02    7 27.3   0.644   1.388   113   10.5  19:12 (  0, 63)  

* P/2026 R2 ( Leonard )

New bright comet. It approached to Earth down to 0.3 a.u. in early October. Now it is 11.8 mag (Oct. 12, Mike Olason). It will fade out rapidly after this. It will be fainter than 18 mag in January. In the Northern Hemisphere, it will be unobservable soon. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  16 28.87  -14 35.4   0.327   0.837    51   12.3  18:56 ( 55, 16)  
Oct. 17  16 28.51  -40 37.8   0.418   0.804    51   12.7  18:47 ( 40, -5)  

* 169P/NEAT

It approached to Earth down to 0.17 a.u. mid August, and brightened up to 10.8 mag (Aug. 11, Thomas Lehmann). Now it is 12.5 mag (Oct. 8, Ken Harikae). Fading rapidly. It will be fainter than 18 mag in November. In the Northern Hemisphere, it will be getting higher gradually. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  10 15.03    1 59.3   0.949   0.701    42   12.6   4:37 (283, 21)  
Oct. 17  10 32.40    0 22.0   1.050   0.773    44   13.7   4:43 (287, 23)  

* C/2024 T5 ( ATLAS )

Now it is 13.0 mag (Oct. 14, Osamu Miyazaki). It stays 12 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   5 46.10  -13 34.3   3.857   4.247   106   12.7   4:33 (  0, 41)  
Oct. 17   5 46.26  -13 38.7   3.752   4.222   111   12.6   4:06 (  0, 41)  

* 252P/LINEAR

It has not been observed yet in this apparition. It has brightened up to 4 mag in 2016, and 10 mag in 2021. It brightens up to 11.5 mag, but it will turn to fade out rapidly after that. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it will be unobservable temporarily in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  11  5.52    0 39.5   1.831   1.080    29   13.4   4:37 (276, 10)  
Oct. 17  11 35.24   -1 48.5   1.810   1.048    28   12.8   4:43 (279,  9)  

* C/2026 A2 ( Bok )

Now it is 12.5 mag (Oct. 12, Thomas Lehmann). It stays 13 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will appear in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  18 36.92   65 45.9   1.828   2.136    93   13.6  18:56 (163, 56)  
Oct. 17  19  5.71   62 49.2   1.753   2.102    95   13.4  18:47 (161, 59)  

* 220P/McNaught

Major outburst of about 9 mag occured from May 31 to June 1, and it brightened up to 8.3 mag (June 3, Marco Goiato). Another major outburst occued on Aug. 5 and it brightened up to 6.4 mag (Aug. 6, Taras Prystavski). Now it is 12.4 mag (Oct. 14, Toru Yusa). Fading rapidly. It will be fainter than 18 mag in November. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   3 30.05    4 46.6   1.018   1.910   142   13.6   2:18 (  0, 60)  
Oct. 17   3 25.84    3 54.5   1.019   1.946   149   14.3   1:46 (  0, 59)  

* C/2024 J3 ( ATLAS )

Now it is 12.9 mag (Oct. 1, Osamu Miyazaki). It stays 14 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  18 26.49   41 35.4   3.791   3.887    88   13.6  18:56 (116, 69)  
Oct. 17  18 28.28   41 17.8   3.833   3.881    85   13.6  18:47 (114, 65)  

* 260P/McNaught

Now it is 13.8 mag (Oct. 7, Kunihiro Shima). It will fade out rapidly after this. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   6  1.32   44 54.7   1.013   1.595   104   13.6   4:37 (192, 80)  
Oct. 17   6 11.18   46 25.3   1.001   1.631   109   13.8   4:31 (180, 79)  

* 88P/Howell

It brightened up to 9.6 mag in the very low sky in spring (Apr. 14, Chris Wyatt). Now it is 13.5 mag (Oct. 14, Toru Yusa). It will fade out rapidly after this. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   3  1.44   14 24.5   1.498   2.411   149   13.7   1:49 (  0, 70)  
Oct. 17   2 54.22   14  3.3   1.504   2.456   157   13.9   1:15 (  0, 69)  

* 78P/Gehrels 2

Now it is 13.3 mag (Oct. 13, Thomas Lehmann). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 33.93   16  9.6   2.055   2.185    83   13.8   4:37 (303, 60)  
Oct. 17   7 42.92   15 24.6   1.997   2.207    88   13.8   4:43 (313, 63)  

* 29P/Schwassmann-Wachmann 1

Now it is 13.6 mag (Aug. 2, Andrew Pearce). Now it is not observable. It will appear soon in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  12 10.30   -8  3.0   7.289   6.318    12   14.3   4:37 (274, -9)  
Oct. 17  12 14.97   -8 37.2   7.261   6.318    17   14.3   4:43 (278, -3)  

* 11P/Tempel-Swift-LINEAR

Now it is 15.0 mag (Oct. 12, D. Buczynski). It brightens up to 13 mag, but it will turn to fade out rapidly after that. It will be fainter than 18 mag in February. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   2  8.96   38 57.5   0.495   1.429   143   15.2   0:56 (180, 86)  
Oct. 17   2 18.51   37 33.5   0.461   1.413   149   14.3   0:39 (180, 87)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. Now it is 14.2 mag (Oct. 4, Andrew Pearce). It stays 14 mag for a while. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition. In the Northern Hemisphere, it is not observable until 2030.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 39.24  -72 18.6  13.668  13.546    80   14.5   4:37 (352,-19)  
Oct. 17   7 41.87  -72 46.3  13.660  13.526    80   14.5   4:43 (354,-19)  

* C/2024 R4 ( PanSTARRS )

Now it is 14.5 mag (Oct. 15, Toru Yusa). It stays 14 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  19 51.61   46 20.7   5.053   5.375   103   14.5  18:56 (163, 78)  
Oct. 17  19 47.25   45 33.0   5.077   5.344   100   14.5  18:47 (145, 77)  

* (3200) Phaethon

Parent object of Geminids meteor shower. It approached to Sun down to 0.14 a.u. on Sept. 2. Now it is 14.5 mag (Oct. 12, Katsumi Yoshimoto). It will fade out rapidly after this. It will be fainter than 18 mag in December. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will be observable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  16 44.62   55 42.9   0.368   0.986    77   14.9  18:56 (138, 51)  
Oct. 17  19  1.75   53 10.7   0.404   1.099    93   14.8  18:47 (147, 67)  

* C/2023 R1 ( PanSTARRS )

Now it is 14.7 mag (Sept. 19, Mike Olason). It stays 15 mag for a while. It will be unobservable soon in the Northern Hemisphere, or in November in the Southern Hemisphere. But it will be observable again in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  15 28.25  -18 28.6   4.661   3.922    37   14.9  18:56 ( 64,  4)  
Oct. 17  15 29.44  -19  4.4   4.764   3.948    31   15.0  18:47 ( 66,  1)  

* 123P/West-Hartley

Now it is 15.9 mag (Oct. 12, M. Jaeger, G. Rhemann, E. Prosperi). It stays 15 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  11 38.16   13 34.8   2.987   2.163    28   14.9   4:37 (261, 10)  
Oct. 17  11 52.47   11 58.7   2.956   2.168    31   14.9   4:43 (265, 13)  

* C/2025 V2 ( Rankin )

It is expected to brighten up to 12.5 mag in 2027 spring. Brightening gradually. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. In the Southern Hemisphere, it is not observable now, but it will appear in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  12 14.52   16  6.6   3.629   2.759    25   15.7   4:37 (253,  4)  
Oct. 17  12 27.69   15 32.1   3.537   2.704    28   15.6   4:43 (257,  8)  

* C/2022 QE78 ( ATLAS )

Now it is 15.5 mag (June 14, Alfons Diepvens). It stays 16 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  11 18.73   26 21.9   6.897   6.178    40   15.6   4:37 (252, 21)  
Oct. 17  11 24.58   26 17.4   6.852   6.201    46   15.6   4:43 (255, 26)  

* 63P/Wild 1

It brightened up to 13.0 mag in early summer (July 3, Thomas Lehmann). It will fade out rapidly after this. It will be fainter than 18 mag in December. Now it is not observable. It will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  13 14.44  -14 58.1   3.164   2.184     9   15.6  18:56 ( 85,-20)  
Oct. 17  13 28.59  -16 55.7   3.197   2.214     7   15.8  18:47 ( 84,-22)  

* C/2025 Y1 ( ATLAS )

Now it is 16.1 mag (Aug. 5, Ken-ichi Kadota). Brightening slowly. Now it is not observable. It will appear in November in the Northern Hemisphere, or in December in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  13 49.58   -2 36.2   5.488   4.520    12   15.7  18:56 ( 91, -6)  
Oct. 17  13 56.70   -3 11.2   5.447   4.468     9   15.7  18:47 ( 92, -9)  

* C/2022 N2 ( PanSTARRS )

Now it is 15.9 mag (Sept. 23, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 29.60   25 28.5   5.300   5.327    86   15.9   4:37 (287, 67)  
Oct. 17   7 32.15   25 24.6   5.230   5.367    92   15.9   4:43 (298, 72)  

* C/2025 M2 ( PanSTARRS )

It is expected to brighten up to 12 mag from 2027 to 2028. Now it is 15.9 mag (Aug. 28, Jean-Claude Merlin). Brightening slowly. It will be unobservable in December. But it will be observable again in February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  18 42.24  -21 27.0   4.849   4.839    83   16.0  18:56 ( 24, 30)  
Oct. 17  18 40.03  -21 27.1   4.929   4.788    76   15.9  18:47 ( 29, 28)  

* 112P/Urata-Niijima

Now it is 16.5 mag (Oct. 14, Toru Yusa). Fading gradually. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 33.89   39 50.8   1.099   1.455    87   16.2   4:37 (249, 69)  
Oct. 17   7 59.36   41 47.7   1.079   1.467    89   16.1   4:43 (243, 70)  

* 114P/Wiseman-Skiff

Now it is 16.6 mag (Oct. 9, Ken-ichi Kadota). Fading slowly. It will be fainter than 18 mag in February. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   8 59.37   14 38.6   1.767   1.591    63   16.3   4:37 (283, 43)  
Oct. 17   9 15.44   12  7.2   1.731   1.604    65   16.3   4:43 (290, 45)  

* C/2021 G2 ( ATLAS )

Now it is 16.1 mag (Oct. 15, Toru Yusa). It stays 17 mag for a while. In the Northern Hemisphere, it will be getting lower gradually. But it will be getting higher again after December. In the Southern Hemisphere, it will be unobservable in November. But it will be observable again in February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  17 11.37   12 32.3   7.873   7.509    65   16.3  18:56 ( 72, 44)  
Oct. 17  17 14.61   12 16.8   7.984   7.546    60   16.4  18:47 ( 75, 41)  

* 2P/Encke

It will brighten up to 6-7 mag from January to February. Now it is 16.4 mag (Oct. 7, D. Buczynski). It will brighten rapidly after this. It will be getting lower gradually after this, and it will be unobservable in January in the Southern Hemisphere, or in February in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   0 30.43   19 11.6   1.077   2.059   165   16.5  23:13 (  0, 74)  
Oct. 17   0 12.88   18  4.7   1.018   1.984   160   16.4  22:28 (  0, 73)  

* 84P/Giclas

Now it is 17.3 mag (Oct. 2, Andrew Pearce). It stays 16 mag for a while. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  20 24.87  -26 12.6   1.556   2.066   105   16.5  19:10 (  0, 29)  
Oct. 17  20 31.43  -25 52.6   1.600   2.033   100   16.4  18:49 (  0, 29)  

* C/2025 J1 ( Borisov )

Now it is 16.8 mag (Sept. 23, Alfons Diepvens). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 14.97   11 22.9   3.647   3.742    87   16.5   4:37 (316, 59)  
Oct. 17   7 13.21    9 40.0   3.546   3.761    94   16.5   4:43 (333, 62)  

* C/2026 AZ17 ( Bok )

Now it is 16.7 mag (Oct. 11, Alfons Diepvens). It stays 17 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January in the Northern Hemisphere, or in December in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  17 36.16    1 12.2   2.691   2.518    69   16.7  18:56 ( 55, 41)  
Oct. 17  17 47.95   -0 29.5   2.744   2.505    65   16.7  18:47 ( 55, 38)  

* C/2022 R6 ( PanSTARRS )

It was observed at 16 mag from 2025 to 2026. Now it is 17.3 mag (Oct. 2, P.-J. Dekelver). It stays 17 mag for a while. It will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  10  7.82    5  4.8   7.790   7.113    44   17.0   4:37 (281, 24)  
Oct. 17  10 11.35    5  4.8   7.723   7.131    50   17.0   4:43 (286, 30)  

* 493P/2024 Q2 ( LONEOS )

Now it is 17.7 mag (Sept. 25, P.-J. Dekelver). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will be observable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   9 54.83   31 43.8   4.577   4.141    58   17.1   4:37 (255, 40)  
Oct. 17  10  1.74   31 19.1   4.507   4.157    63   17.1   4:43 (259, 45)  

* C/2025 R3 ( PanSTARRS )

It brightened up to 4.0 mag in late April (Apr. 30, Chris Wyatt). It brightened up to 1.3 mag due to the forward scattering in the SOHO LASCO images (Apr. 25, Mikolaj Kaszczyk). It faded down to 13.4 mag until summer (Aug. 15, Thomas Lehmann). Fading gradually. It will be fainter than 18 mag in November. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 26.92  -27 41.6   2.986   2.999    81   17.1   4:37 (337, 23)  
Oct. 17   7 21.12  -29  8.9   2.981   3.088    86   17.2   4:43 (346, 24)  

* 346P/Catalina

Now it is 17.5 mag (Oct. 2, ATLAS-HKO, Haleakala). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   8 39.94   18 46.2   2.450   2.288    68   17.2   4:37 (282, 49)  
Oct. 17   8 51.79   18 55.3   2.385   2.303    73   17.1   4:43 (286, 53)  

* C/2025 E1 ( PanSTARRS )

Now it is 17.6 mag (Sept. 12, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  12 43.03  -78  8.1   4.199   4.001    71   17.1   4:37 (346,-37)  
Oct. 17  13 26.27  -79 24.0   4.226   4.003    70   17.2  18:47 ( 13,-37)  

* C/2025 A1 ( Lemmon )

Now it is 16.8 mag (Oct. 8, Kunihiro Shima). It stays 17 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  11  4.15   30 29.2   6.107   5.464    46   17.3   4:37 (250, 26)  
Oct. 17  11 11.32   30 21.4   6.025   5.453    50   17.3   4:43 (253, 30)  

* P/2018 VN2 = P/2026 M2 ( Leonard )

First return of a new periodic comet which was observed at 18 mag in 2018. Now it is 17.2 mag (Sept. 5, ATLAS-MLO, Mauna Loa). Fading gradually. It will be fainter than 18 mag in December. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   2  1.97   24  7.1   1.212   2.167   156   17.3   0:50 (  0, 79)  
Oct. 17   1 58.95   22 30.8   1.203   2.179   164   17.3   0:19 (  0, 78)  

* C/2019 E3 ( ATLAS )

Very far object. It stays 18 mag for a while. In the Northern Hemisphere, it will be unobservable in February. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   0  3.47  -45  7.0  11.110  11.737   126   17.4  22:47 (  0, 10)  
Oct. 17  23 59.96  -44 54.0  11.186  11.754   122   17.4  22:16 (  0, 10)  

* 188P/LINEAR-Mueller

Now it is 17.9 mag (Aug. 24, W. Hasubick). Fading slowly. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   6 21.11   35  7.0   2.447   2.824   101   17.5   4:37 (267, 84)  
Oct. 17   6 25.40   35 35.7   2.380   2.844   107   17.5   4:43 (222, 89)  

* C/2022 E2 ( ATLAS )

It was observed at 12-13 mag for a long time in 2024. Now it is 17.2 mag (Oct. 12, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag in November. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  21 51.89   24  8.8   6.545   7.247   131   17.5  20:36 (  0, 79)  
Oct. 17  21 48.74   23  7.9   6.657   7.291   126   17.6  20:05 (  0, 78)  

* C/2024 G4 ( PanSTARRS )

Now it is 17.6 mag (Sept. 16, ATLAS Chile). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  20  4.91   -6 35.4   4.792   5.145   105   17.5  18:56 (  2, 48)  
Oct. 17  20  7.50   -7 11.7   4.911   5.161    98   17.6  18:47 (  8, 48)  

* C/2025 B2 ( Borisov )

Now it is 17.2 mag (Oct. 1, Taras Prystavski). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  17  1.67   73 24.4   8.213   8.240    88   17.6  18:56 (162, 45)  
Oct. 17  17  8.77   72 18.1   8.201   8.241    88   17.6  18:47 (161, 45)  

* C/2026 P2 ( PanSTARRS )

It is expected to brighten up to 13.5 mag from late 2027 to early 2028. At the high light, it will be observable in good condition in the Northern Hemisphere. But it will not be observable in the Southern Hemisphere. Now it is 17.3 mag (Oct. 7, Ken-ichi Kadota). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   1 29.42   -1 47.4   3.818   4.802   169   17.7   0:18 (  0, 53)  
Oct. 17   1 22.99   -1 39.0   3.765   4.748   169   17.6  23:39 (  0, 54)  

* 93P/Lovas 1

Now it is 17.7 mag (Sept. 22, P.-J. Dekelver). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  10  5.42   17 20.7   2.833   2.309    49   17.7   4:37 (270, 31)  
Oct. 17  10 16.14   16 11.3   2.807   2.352    53   17.8   4:43 (274, 35)  

* C/2023 X2 ( Lemmon )

Now it is 17.8 mag (July 6, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  15  7.30   53 35.1   5.864   5.529    65   17.8  18:56 (135, 35)  
Oct. 17  15 15.13   52 19.6   5.885   5.549    65   17.8  18:47 (134, 33)  

* 65P/Gunn

Now it is 17.7 mag (Oct. 7, Hidenori Nohara). Fading slowly. It will be fainter than 18 mag soon. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   0 23.33   -8 49.5   2.686   3.649   162   17.8  23:07 (  0, 46)  
Oct. 17   0 18.99   -9  0.4   2.735   3.665   155   17.9  22:35 (  0, 46)  

* P/2009 Y2 ( Kowalski )

Now it is 18.2 mag (Oct. 6, Toshiyuki Takahashi). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   5 20.26   39 44.5   1.842   2.417   113   18.0   4:08 (180, 85)  
Oct. 17   5 24.50   39  1.4   1.757   2.405   119   17.8   3:45 (180, 86)  

* 373P/Rinner

It has not been observed yet in this apparition. It has brightened up to 4 mag in 2016, and 10 mag in 2021. It was not detected, fainter than 20 mag on Sept. 14 (Jean-Francois Soulier). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   8 31.16    8 24.9   2.482   2.314    68   17.9   4:37 (296, 45)  
Oct. 17   8 41.58    7  4.3   2.413   2.320    72   17.9   4:43 (303, 48)  

* P/2021 N1 = P/2026 M1 ( ZTF )

First return of a new periodic comet which brightened up to 17 mag in 2021. It approached to Earth down to 0.17 a.u. from June to July. It brightened up to 15.2 mag (July 14, Andrew Pearce). Now it is 18.2 mag (Sept. 19, Mike Olason). It will fade out rapidly after this. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   4 59.36   48 24.9   0.637   1.390   114   18.4   3:48 (180, 77)  
Oct. 17   4 49.95   48 25.1   0.652   1.452   122   18.6   3:11 (180, 77)  

* 266P/Christensen

Now it is 18.8 mag (Oct. 12, D. Buczynski). Brightening slowly. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10   7 24.88   25 40.7   2.184   2.358    87   18.9   4:37 (288, 68)  
Oct. 17   7 34.81   25 30.2   2.096   2.351    91   18.7   4:43 (297, 72)  

* SWAN26Q

New comet discovered on Aug. 24 from SWAN images by Hanjie Tan. Although it was bright as 11 mag at the discovery, it faded down to 14 mag on Sept. 9. It was not detected, fainter than 16 mag, on Oct. 8. (Mike Olason). Fading rapidly. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 10  11 29.36    1 48.2   1.805   0.982    24   19.2   4:37 (272,  5)  
Oct. 17  11 27.23   -1 15.3   1.857   1.120    30   19.9   4:43 (279, 11)  

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