Weekly Information about Bright Comets (2025 Oct. 25: North)

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Updated on October 26, 2025
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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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* C/2025 A6 ( Lemmon )

Now it is 4.3 mag (Oct. 19, Virgilio Gonano). It will fade out rapidly after this. In the Northern Hemisphere, it will be unobservable in November. 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. 25  15 17.77   19 54.6   0.623   0.628    37    4.0  18:38 (102, 17)  
Nov.  1  16 23.58    2 47.6   0.778   0.559    34    3.9  18:31 ( 81, 16)  

* C/2025 R2 ( SWAN )

Now it is 5.6 mag (Oct. 19, Virgilio Gonano). 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. 25  20 23.62   -7 55.8   0.281   1.056    94    6.5  18:38 (  8, 47)  
Nov.  1  21 53.42   -1 36.7   0.365   1.174   111    7.7  19:15 (  0, 54)  

* C/2025 K1 ( ATLAS )

Now it is 9.7 mag (Oct. 25, Piotr Guzik). It will fade out rapidly after this. It will be fainter than 18 mag in February. In the Northern Hemisphere, it will be getting higher gradually. 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. 25  11 49.20   -1 43.1   0.997   0.572    33    9.3   4:49 (282, 14)  
Nov.  1  11 38.34    4 52.4   0.825   0.718    45    9.8   4:55 (284, 26)  

* 210P/Christensen

It is expected to brighten up to 8 mag from late autumn to early winter. Now it is 14.8 mag (Oct. 22, Martin Masek). It brightens up to 8.5 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it is not observable now, but it will appear in November. In the Southern Hemisphere, it will be unobservable in November. But it will be observable again in December. It is much fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  17 13.96  -40  8.7   0.481   0.790    51   10.9  18:38 ( 39, -1)  
Nov.  1  16 37.77  -37 53.4   0.448   0.695    37    9.9  18:31 ( 48, -7)  

* C/2024 E1 ( Wierzchos )

It is expected to brighten up to 5 mag in January. Now it is 12.6 mag (Sept. 30, Thomas Lehmann). It will brighten rapidly after this. In the Northern Hemisphere, it will be unobservable in December. But it will be observable again in February. 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. 25  16 37.84   11 36.5   2.313   1.778    46   11.3  18:38 ( 84, 28)  
Nov.  1  16 47.53    8 12.1   2.271   1.672    42   11.0  18:31 ( 83, 24)  

* 3I/2025 N1 ( ATLAS )

Third interstellar object in history following 1I/'Oumuamua and 2I/Borisov. The eccentricity is extremely big as 6. It approaches to Sun down to 1.38 a.u. in late October. Now it is 10.8 mag (Oct. 2, Thomas Lehmann). It will turn to fade out rapidly after the peak. Now it is not observable. It will appear in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  13 38.94   -7 39.6   2.351   1.366     6   11.2   4:49 (271,-12)  
Nov.  1  13 24.25   -6 31.9   2.280   1.360    16   11.1   4:55 (277, -2)  

* C/2025 T1 ( ATLAS )

Bright new comet. Now it is 12.4 mag (Oct. 21, Martin Masek). It brightens up to 11.5 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it will be unobservable in January. In the Southern Hemisphere, it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  12 56.69   53 59.6   1.264   1.270    67   12.5   4:49 (222, 29)  
Nov.  1  14 15.90   55 14.9   1.135   1.220    69   12.1   4:55 (218, 23)  

* 240P/NEAT

Now it is brighter than originally expected. Now it is 13.1 mag (Sept. 30, Hiroshi Abe). Fading slowly. It stays observable in good condition. It is expected to brighten up to 12 mag and to be observable in good condition from autumn to winter. A 19-mag fragment was found on Oct. 3.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   4 12.25    1 32.3   1.276   2.167   144   12.4   2:00 (  0, 57)  
Nov.  1   4  7.89    2 23.4   1.230   2.157   151   12.3   1:28 (  0, 57)  

* C/2022 N2 ( PanSTARRS )

Now it is 13.9 mag (Sept. 23, Osamu Miyazaki). Fading 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. 25   3 32.39   26 32.0   2.984   3.898   153   13.3   1:20 (  0, 82)  
Nov.  1   3 29.86   26 28.1   2.961   3.910   160   13.3   0:50 (  0, 82)  

* 24P/Schaumasse

It will brighten up to 8 mag in winter, and will be observable in good condition. Now it is 15.9 mag (Oct. 1, Thomas Lehmann). Brightening rapidly. 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. 25   7 43.18   20  1.1   1.041   1.529    97   14.4   4:49 (327, 73)  
Nov.  1   8  8.19   20  9.8   0.955   1.477    98   13.5   4:55 (333, 73)  

* 29P/Schwassmann-Wachmann 1

It will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  11 12.06    0 30.6   6.992   6.299    42   14.2   4:49 (286, 23)  
Nov.  1  11 15.83   -0  0.3   6.910   6.300    48   14.2   4:55 (292, 28)  

* C/2023 R1 ( PanSTARRS )

It is expected to brighten up to 13 mag in early summer in 2026. Now it is 14.4 mag (Sept. 12, Andrew Pearce). It stays 14 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. But it will be observable again in January in the Northern Hemisphere, or in February in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  19 16.96    6 17.9   3.909   3.889    81   14.4  18:38 ( 43, 54)  
Nov.  1  19 14.72    4 59.7   4.009   3.864    74   14.4  18:31 ( 49, 49)  

* 88P/Howell

Now it is 17.7 mag (July 24, Thomas Lehmann). It will brighten rapidly after this. Now it is not observable. It will appear in January in the Southern Hemisphere, or in December in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  13 51.06   -9 55.4   3.004   2.011     2   14.7   4:49 (271,-16)  
Nov.  1  14  6.34  -11 26.3   2.951   1.965     5   14.5   4:55 (275,-13)  

* C/2021 G2 ( ATLAS )

Now it is 14.8 mag (Sept. 27, Ken-ichi Kadota). It stays 15 mag for a while. In the Northern Hemisphere, it will be unobservable in November. But it will be observable again in December. 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. 25  15 55.57   -1 15.6   6.706   5.878    31   14.6  18:38 ( 80, 12)  
Nov.  1  16  1.10   -1 16.3   6.771   5.906    27   14.6  18:31 ( 82,  9)  

* C/2022 QE78 ( ATLAS )

Now it is 14.9 mag (Oct. 17, Ken-ichi Kadota). It stays 14 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. 25   9 11.03   19 28.4   5.620   5.485    77   14.6   4:49 (290, 58)  
Nov.  1   9 14.85   19 43.6   5.514   5.489    83   14.6   4:55 (299, 63)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.3 mag (Sept. 29, Andrew Pearce). It stays 15 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. 25   5 40.50  -73 13.8  14.620  14.614    87   15.0   3:26 (  0,-18)  
Nov.  1   5 38.29  -73 37.7  14.614  14.592    86   15.0   2:56 (  0,-19)  

* C/2024 J3 ( ATLAS )

It will brighten up to 13 mag in 2026. Now it is 15.4 mag (Oct. 2, ATLAS-MLO, Mauna Loa). It stays 15 mag for a while. It will be getting lower gradually after this, and it will be unobservable in December. But it will be observable again in January in the Northern Hemisphere, or in February in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  18 35.56   -9 50.6   5.417   5.131    68   15.0  18:38 ( 42, 35)  
Nov.  1  18 38.06   -9 24.2   5.482   5.094    62   15.0  18:31 ( 47, 32)  

* 43P/Wolf-Harrington

Now it is 16.3 mag (Sept. 28, Alfons Diepvens). It stays 15 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. 25  10  6.32    3 33.0   2.868   2.513    59   15.0   4:49 (296, 37)  
Nov.  1  10 16.18    2 16.2   2.804   2.525    63   15.0   4:55 (302, 40)  

* C/2022 E2 ( ATLAS )

It was observed at 12-13 mag for a long time in 2024. Now it is 14.8 mag (Oct. 2, Thomas Lehmann). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  22 49.35   47  2.9   4.423   5.089   127   15.3  20:33 (180, 78)  
Nov.  1  22 42.35   45  7.4   4.504   5.129   124   15.4  19:59 (180, 80)  

* C/2024 T5 ( ATLAS )

Now it is 15.1 mag (Oct. 2, ATLAS Chile). It stays 15 mag for a while. It stays extremely low in the Northern Hemisphere. But it will become high in autumn. In the Southern Hemisphere, it stays observable in good condition. It is expected to brighten up to 12 mag in winter between 2026 and 2027.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   3  9.49  -46  1.1   5.492   6.048   119   15.5   0:57 (  0,  9)  
Nov.  1   3  5.31  -46  7.2   5.464   6.006   118   15.4   0:25 (  0,  9)  

* C/2025 L1 ( ATLAS )

It is expected to brighten up to 13.5 mag and to be observable in good condition in 2026 spring. Now it is 16.8 mag (Aug. 12, ATLAS South Africa). Brightening slowly. In the Northern Hemisphere, it is not observable now, but it will appear in December. It stays extremely 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. 25  14  8.30  -54 56.3   2.585   1.977    43   15.5  18:38 ( 43,-34)  
Nov.  1  14 22.75  -52 56.5   2.605   1.932    38   15.4   4:55 (315,-34)  

* 78P/Gehrels 2

It will brighten up to 12 mag in 2026 summer. Now it is 16.2 mag (Sept. 18, Francois Kugel). Brightening slowly. 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. 25  20  6.28  -13 55.0   2.566   2.740    89   15.9  18:38 ( 15, 40)  
Nov.  1  20 12.58  -13 52.6   2.628   2.708    83   15.8  18:31 ( 19, 39)  

* 235P/LINEAR

It stays 16 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in spring. In the Southern Hemisphere, it will be unobservable in November. But it will be observable again in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  12  2.32   -4 18.8   2.838   2.032    29   16.0   4:49 (282, 10)  
Nov.  1  12 17.84   -5 42.7   2.789   2.020    32   15.9   4:55 (286, 12)  

* 47P/Ashbrook-Jackson

Now it is 15.5 mag (Sept. 29, ATLAS Chile). Fading slowly. 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 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  22 38.02   -9 32.4   2.105   2.808   126   16.1  20:22 (  0, 46)  
Nov.  1  22 38.54   -8 55.8   2.184   2.808   119   16.2  19:56 (  0, 46)  

* C/2024 A1 ( ATLAS )

Now it is 16.6 mag (Oct. 3, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   8 52.33   35 25.8   3.991   4.046    86   16.3   4:49 (261, 68)  
Nov.  1   8 54.47   37  7.6   3.893   4.063    92   16.2   4:55 (257, 74)  

* C/2023 C2 ( ATLAS )

It brightened up to 12.7 mag in 2024 summer (Aug. 7, 2024, Thomas Lehmann). Now it is 15.6 mag (Sept. 30, Hiroshi Abe). Fading slowly. 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. 25  22 17.60   55 27.3   3.707   4.283   119   16.2  20:02 (180, 69)  
Nov.  1  22 16.70   54 33.6   3.786   4.338   117   16.3  19:33 (180, 70)  

* 65P/Gunn

Now it is 16.3 mag (Sept. 25, ATLAS South Africa). It stays 17 mag for a while. It will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  19  8.48  -30 19.2   3.123   2.997    73   16.2  18:38 ( 24, 20)  
Nov.  1  19 18.03  -29 56.6   3.219   3.005    68   16.3  18:31 ( 26, 20)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.6 mag (Oct. 2, ATLAS-MLO, Mauna Loa). It stays 16 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. 25   8 52.48  -11 34.7   6.777   6.578    74   16.3   4:49 (326, 37)  
Nov.  1   8 54.62  -11 45.0   6.682   6.581    79   16.3   4:55 (335, 40)  

* 261P/Larson

Now it is 16.7 mag (Sept. 18, Francois Kugel). It stays 17 mag for a while. 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 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  20 20.68  -14 39.8   1.778   2.075    92   16.5  18:38 ( 10, 40)  
Nov.  1  20 30.94  -14  0.4   1.841   2.062    88   16.5  18:31 ( 13, 40)  

* C/2023 H5 ( Lemmon )

Now it is 16.7 mag (Sept. 30, Thomas Lehmann). It stays 17 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. 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. 25  14 49.81   63 24.1   4.552   4.419    76   16.5  18:38 (149, 31)  
Nov.  1  15 11.02   63 26.4   4.526   4.432    78   16.5  18:31 (149, 31)  

* 217P/LINEAR

It brightened up to 12.1 mag in early summer (June 10, Taras Prystavski). Now it is 15.8 mag (Oct. 1, Katsumi Yoshimoto). Fading gradually. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   8 57.85   12 43.3   2.136   2.165    78   16.7   4:49 (303, 56)  
Nov.  1   9  4.56   12 31.6   2.102   2.222    83   16.9   4:55 (313, 60)  

* 302P/Lemmon-PanSTARRS

It brightened very rapidly, and it became brighter than expected. Now it is 15.8 mag (Sept. 27, Katsumi Yoshimoto). Fading slowly. It will be fainter than 18 mag in January. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   0 23.46   -5 48.5   2.543   3.445   150   16.8  22:07 (  0, 49)  
Nov.  1   0 20.76   -5 58.7   2.607   3.454   143   16.8  21:37 (  0, 49)  

* 493P/2024 Q2 ( LONEOS )

Now it is 16.9 mag (Sept. 28, Alfons Diepvens). It stays 17 mag for a while. 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. 25   5 16.16   50 40.8   3.207   3.854   124   16.8   3:04 (180, 74)  
Nov.  1   5 14.52   51 28.4   3.139   3.849   129   16.8   2:35 (180, 74)  

* 145P/Shoemaker-Levy 5

Now it is 17.3 mag (Oct. 1, ATLAS-MLO, Mauna Loa). 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. 25  22 18.31  -20  6.4   1.440   2.092   117   16.9  20:03 (  0, 35)  
Nov.  1  22 21.15  -18 45.6   1.483   2.066   111   16.8  19:38 (  0, 36)  

* C/2023 X2 ( Lemmon )

Now it is 16.9 mag (Oct. 3, ATLAS-MLO, Mauna Loa). It stays 17 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. 25   9 10.84   80 11.5   4.866   5.112    98   16.9   4:49 (187, 43)  
Nov.  1   9 40.61   81 37.1   4.817   5.108   101   16.9   4:55 (186, 42)  

* C/2023 F3 ( ATLAS )

Now it is 16.9 mag (July 13, Taras Prystavski). It stays 17 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in spring. 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. 25  11  2.58  -23  4.6   6.245   5.558    42   16.9   4:49 (306,  9)  
Nov.  1  11  3.10  -23 20.4   6.189   5.577    48   16.9   4:55 (312, 14)  

* C/2024 R4 ( PanSTARRS )

Brightening rapidly. It is expected to brighten up to 13 mag from 2027 to 2028. Now it is 17.0 mag (Sept. 30, Thomas Lehmann). It stays 17 mag for a while. 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 December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  21 34.54   22 27.7   6.693   7.197   116   17.0  19:19 (  0, 78)  
Nov.  1  21 32.24   22  8.7   6.744   7.157   110   17.0  18:49 (  0, 77)  

* C/2025 Q3 ( ATLAS )

Now it is 17.2 mag (Oct. 23, Ken-ichi Kadota). It stays 17 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. 25   4  3.54   37 21.2   1.696   2.554   142   17.2   1:52 (180, 87)  
Nov.  1   3 49.32   33 55.6   1.588   2.511   152   17.0   1:10 (  0, 89)  

* 164P/Christensen

Now it is 16.9 mag (Oct. 13, Ken-ichi Kadota). 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. 25  10 12.70   20 14.5   2.430   2.184    63   17.1   4:49 (277, 46)  
Nov.  1  10 24.41   20  0.1   2.390   2.222    68   17.0   4:55 (281, 50)  

* C/2023 RS61 ( PanSTARRS )

Although it is around 20 mag usually, now it is bright in outburst. Now it is 17.1 mag (Oct. 13, Ken-ichi Kadota). It stays 17 mag for a while. 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. 25   3  5.14   38 32.2   7.998   8.869   149   17.1   0:53 (180, 86)  
Nov.  1   3  2.45   38 31.3   7.954   8.860   154   17.0   0:23 (180, 86)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 17.4 mag (July 26, ATLAS South Africa). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in December. 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. 25   0 28.50  -56 56.4  10.624  10.983   108   17.0  22:12 (  0, -2)  
Nov.  1   0 23.84  -56 32.3  10.700  10.995   104   17.1  21:40 (  0, -1)  

* 195P/Hill

Now it is 17.7 mag (Sept. 18, Hidetaka Sato). It stays 17 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. 25   9 36.60  -20 35.0   4.822   4.456    62   17.1   4:49 (321, 23)  
Nov.  1   9 41.29  -21 47.0   4.749   4.458    67   17.1   4:55 (328, 26)  

* C/2025 J1 ( Borisov )

Now it is 17.3 mag (Oct. 13, Ken-ichi Kadota). 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.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  11 18.22   70 31.5   4.064   4.131    86   17.2   4:49 (204, 41)  
Nov.  1  11 19.12   71 10.0   3.960   4.100    91   17.1   4:55 (202, 44)  

* C/2025 R1 ( ATLAS )

Now it is 17.1 mag (Oct. 17, Ken-ichi Kadota). Fading slowly. It will be fainter than 18 mag in December. In the Northern Hemisphere, it will be getting lower gradually. 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. 25  18 43.69   65  8.4   1.686   2.007    93   17.2  18:38 (157, 54)  
Nov.  1  18 40.63   58 24.8   1.740   1.994    89   17.2  18:31 (144, 56)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. It is fading very slowly. Now it is 16.9 mag (Sept. 29, ATLAS South Africa). It stays 18 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be getting lower gradually. But it will be getting higher again after January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  18 54.00  -68 40.2   8.822   8.586    73   17.2  18:38 ( 11,-16)  
Nov.  1  18 55.69  -68  6.6   8.949   8.636    68   17.2  18:31 ( 13,-16)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 17.2 mag (Sept. 28, Alfons Diepvens). 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. 25   6 16.55   29 10.1   9.318   9.820   117   17.4   4:04 (  0, 84)  
Nov.  1   6 14.65   29 23.1   9.266   9.869   125   17.4   3:35 (  0, 84)  

* C/2019 U5 ( PanSTARRS )

Now it is 17.1 mag (Sept. 2, Andrew Pearce). It stays 18 mag for a while. It stays extremely 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. 25   5 44.50  -45 57.1   8.144   8.422   102   17.4   3:31 (  0,  9)  
Nov.  1   5 39.63  -46 31.5   8.154   8.466   105   17.4   2:59 (  0,  9)  

* C/2023 U1 ( Fuls )

It continues brightening even after the perihelion passage. Now it is 17.5 mag (Oct. 1, ATLAS Chile). It stays 18 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. 25   0 25.79  -68 14.7   5.515   5.741    98   17.5  22:08 (  0,-13)  
Nov.  1   0  8.79  -67 30.9   5.603   5.767    94   17.5  21:24 (  0,-12)  

* C/2023 H1 ( PanSTARRS )

Now it is 17.0 mag (Sept. 25, ATLAS-MLO, Mauna Loa). Fading slowly. It will be fainter than 18 mag in December. It will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  19 55.85  -14  2.5   5.137   5.177    86   17.5  18:38 ( 18, 39)  
Nov.  1  19 59.45  -13 43.9   5.272   5.205    80   17.6  18:31 ( 23, 38)  

* 48P/Johnson

Now it is 16.4 mag (Oct. 2, ATLAS-MLO, Mauna Loa). Fading slowly. 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. 25   3 51.37    3  2.8   1.750   2.660   150   17.6   1:39 (  0, 58)  
Nov.  1   3 45.82    2 46.9   1.749   2.690   156   17.8   1:06 (  0, 58)  

* C/2024 X2 ( ATLAS )

Now it is 17.7 mag (June 26, ATLAS Chile). 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. 25   9 24.16   -6 26.6   4.063   3.795    67   17.6   4:49 (314, 37)  
Nov.  1   9 24.88   -5 58.0   3.964   3.810    73   17.6   4:55 (322, 42)  

* (3200) Phaethon

Fading slowly. It will be fainter than 18 mag in December. 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. 25   3  1.18   42 33.0   1.450   2.344   146   17.7   0:50 (180, 82)  
Nov.  1   2 42.10   41 30.1   1.434   2.360   152   17.6   0:04 (180, 83)  

* C/2020 K1 ( PanSTARRS )

It brightened up to 12.1 mag in 2023 spring (May 20, 2023, Jose Guilherme de S. Aguiar). Now it is 17.4 mag (Mar. 25, ATLAS South Africa). It stays 18 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. 25   6 39.64  -20  0.6   7.975   8.265   103   17.7   4:26 (  0, 35)  
Nov.  1   6 37.80  -20 15.0   7.939   8.312   108   17.7   3:57 (  0, 35)  

* 414P/STEREO

It brightened up to 14.4 mag in September (Sept. 17, Ken-ichi Kadota). Fading rapidly. Now it is not observable.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  12 58.75  -17 17.6   1.699   0.784    15   17.7   4:49 (285, -9)  
Nov.  1  13 28.18  -20  7.1   1.806   0.882    14   19.3   4:55 (288,-10)  

* C/2024 G4 ( PanSTARRS )

Now it is 17.8 mag (Sept. 21, Alfons Diepvens). It stays 18 mag for a while. It will be unobservable in November in the Southern Hemisphere, or in December in the Northern Hemisphere. But it will be observable again in January in the Northern Hemisphere, or in February in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  17 23.53    3 57.0   5.557   5.032    53   17.7  18:38 ( 70, 33)  
Nov.  1  17 29.85    3 18.5   5.612   5.020    49   17.8  18:31 ( 72, 29)  

* 242P/Spahr

Now it is 17.8 mag (Mar. 17, ATLAS Chile). It stays 18 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. 25   8  1.52  -11 40.2   4.144   4.204    86   17.8   4:49 (341, 41)  
Nov.  1   8  4.11  -12 26.6   4.066   4.214    91   17.8   4:55 (351, 42)  

* 276P/Vorobjov

Now it is 18.1 mag (Sept. 17, ATLAS-HKO, Haleakala). It stays 18 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. 25   7  9.17    7 58.4   3.804   4.147   103   17.8   4:49 (356, 63)  
Nov.  1   7 10.32    7 26.2   3.717   4.158   109   17.8   4:30 (  0, 62)  

* C/2024 L5 ( ATLAS )

It brightened up to 14.7 mag in spring (Apr. 7, Taras Prystavski). It stays 18 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. 25  11 23.02   -1  4.7   4.754   4.040    39   17.8   4:49 (286, 19)  
Nov.  1  11 23.44   -1  0.6   4.691   4.074    46   17.9   4:55 (291, 26)  

* C/2024 N3 ( Sarneczky )

Now it is 17.9 mag (Oct. 3, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. In the Northern Hemisphere, it will be getting lower gradually. 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. 25  16 54.93   39 57.7   5.556   5.236    66   17.8  18:38 (114, 43)  
Nov.  1  17  0.26   38 29.5   5.607   5.251    64   17.9  18:31 (114, 40)  

* C/2024 J2 ( Wierzchos )

It brightened rapidly up to 14.6 mag in last winter (Jan. 31, Thomas Lehmann). Now it is 17.3 mag (Oct. 2, ATLAS South Africa). Fading gradually. It will be fainter than 18 mag in November. It stays extremely 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. 25   2 42.98  -48 45.9   2.580   3.176   118   17.8   0:31 (  0,  6)  
Nov.  1   2 33.86  -50  4.2   2.684   3.238   115   18.0  23:49 (  0,  5)  

* C/2021 S3 ( PanSTARRS )

It brightened up to 9.6 mag from February to March in 2024 (Feb. 25, 2024, Thomas Lehmann). Now it is 17.9 mag (Sept. 17, Ken-ichi Kadota). Fading slowly. It will be fainter than 18 mag in November. 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. 25  22 51.17   39  7.8   6.216   6.907   130   17.8  20:35 (180, 86)  
Nov.  1  22 49.70   38 13.6   6.320   6.965   127   17.9  20:06 (180, 87)  

* C/2025 L2 ( MAPS )

Now it is 17.6 mag (Sept. 29, ATLAS Chile). It stays 18 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. 25  20 20.18  -57 43.8   2.841   2.892    82   17.9  18:38 (  4, -3)  
Nov.  1  20 21.96  -58 11.2   2.924   2.878    77   17.9  18:31 (  7, -4)  

* C/2025 R3 ( PanSTARRS )

It is expected to brighten up to 7 mag in 2026 April. Now it is 18.9 mag (Sept. 19, Roland Fichtl). It will brighten rapidly after this. It will be unobservable in February in the Northern Hemisphere, or in December in the Southern Hemisphere. At the high light, it is observable in the low sky before the perihelion passage in the Northern Hemisphere, or after the perihelion in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  23 49.47   37  6.1   2.202   3.048   141   18.1  21:32 (180, 88)  
Nov.  1  23 31.42   35 35.3   2.163   2.958   135   17.9  20:47 (180, 89)  

* C/2013 C2 ( Tenagra )

It brightened in major outburst of 5 mag. Now it is 18.1 mag (Oct. 11, John Maikner). It stays 18 mag for a while. It will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25  19 45.80   -3 21.9  15.031  15.003    86   18.0  18:38 ( 26, 49)  
Nov.  1  19 46.57   -3 26.5  15.157  15.016    80   18.1  18:31 ( 33, 46)  

* 486P/2024 H1 ( Leonard )

Now it is 16.5 mag (Oct. 3, ATLAS Chile). Fading gradually. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 25   0 10.06    2 40.5   1.752   2.670   151   18.2  21:54 (  0, 58)  
Nov.  1   0  7.97    2 18.2   1.823   2.692   144   18.4  21:25 (  0, 57)  

* 489P/Denning

It had been lost for 113 years. It will pass the perihelion on Dec. 4. It brightened up to 18 mag in outburst in 2007. 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. 25   9 36.03   18 28.6   1.641   1.623    71   22.6   4:49 (286, 52)  
Nov.  1   9 56.42   16 53.7   1.580   1.603    73   22.5   4:55 (291, 54)  

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