Weekly Information about Bright Comets (2025 Oct. 18: North)

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Updated on October 17, 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 4.8 mag (Oct. 16, Yoshimi Nagai). It will turn to fade out rapidly after the peak. 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. 18  13 23.10   36 39.7   0.612   0.723    46    4.5   4:44 (233, 12)  
Oct. 25  15 17.77   19 54.6   0.623   0.628    37    4.0  18:38 (102, 17)  

* C/2025 R2 ( SWAN )

Now it is 5.8 mag (Oct. 15, Chris Wyatt). 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. 18  18 14.58  -14 29.9   0.265   0.936    69    6.1  18:45 ( 38, 32)  
Oct. 25  20 23.62   -7 55.8   0.281   1.056    94    6.8  18:38 (  8, 47)  

* C/2025 K1 ( ATLAS )

It brightened up to 10.6 mag until mid September (Sept. 16, Thomas Lehmann). 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 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. 18  12  3.61   -6 57.1   1.155   0.434    21    8.4   4:44 (280,  1)  
Oct. 25  11 49.20   -1 43.1   0.997   0.572    33    9.3   4:49 (282, 14)  

* 210P/Christensen

It is expected to brighten up to 8 mag from late autumn to early winter. Now it is 16.3 mag (Oct. 2, ATLAS Chile). It brightens up to 8.5 mag, but it will turn to fade out rapidly after that. It will be unobservable soon in the Northern Hemisphere, or in November in the Southern Hemisphere. But it will be observable again in November in the Northern Hemisphere, or in December in the Southern Hemisphere. It is much fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 18  17 40.54  -41 11.0   0.514   0.891    63   11.8  18:45 ( 31,  4)  
Oct. 25  17 13.96  -40  8.7   0.481   0.790    51   10.9  18:38 ( 39, -1)  

* 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. 18  13 52.85   -8 41.0   2.409   1.420     5   11.4  18:45 ( 89,-13)  
Oct. 25  13 38.94   -7 39.6   2.351   1.366     6   11.2   4:49 (271,-12)  

* C/2024 E1 ( Wierzchos )

It is expected to brighten up to 5 mag in January. Now it is 13.1 mag (Sept. 21, Seiichi Yoshida). It will brighten rapidly after this. It will be unobservable soon in the Southern Hemisphere, or in December in the Northern Hemisphere. But it will be observable again 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. 18  16 29.02   14 59.0   2.352   1.882    50   11.6  18:45 ( 86, 32)  
Oct. 25  16 37.84   11 36.5   2.313   1.778    46   11.3  18:38 ( 84, 28)  

* 240P/NEAT

Now it is brighter than originally expected. Now it is 13.1 mag (Sept. 30, Hiroshi Abe). It stays 13 mag for a while. 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. 18   4 15.04    0 51.5   1.332   2.179   138   12.5   2:30 (  0, 56)  
Oct. 25   4 12.25    1 32.3   1.276   2.167   144   12.4   2:00 (  0, 57)  

* C/2022 N2 ( PanSTARRS )

Now it is 13.9 mag (Sept. 23, Osamu Miyazaki). 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. 18   3 34.38   26 32.1   3.019   3.887   146   13.3   1:50 (  0, 82)  
Oct. 25   3 32.39   26 32.0   2.984   3.898   153   13.3   1:20 (  0, 82)  

* 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. 18  11  8.07    1  2.3   7.065   6.298    37   14.2   4:44 (281, 17)  
Oct. 25  11 12.06    0 30.6   6.992   6.299    42   14.2   4:49 (286, 23)  

* 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. 18  19 20.18    7 43.0   3.808   3.914    88   14.3  18:45 ( 36, 58)  
Oct. 25  19 16.96    6 17.9   3.909   3.889    81   14.4  18:38 ( 43, 54)  

* 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. 18   7 19.94   19 48.2   1.135   1.583    95   15.3   4:44 (321, 71)  
Oct. 25   7 43.18   20  1.1   1.041   1.529    97   14.4   4:49 (327, 73)  

* C/2021 G2 ( ATLAS )

Now it is 14.8 mag (Sept. 27, Ken-ichi Kadota). It stays 15 mag for a while. It will be unobservable soon in the Southern Hemisphere, or in November in the Northern Hemisphere. But it will be observable again 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. 18  15 50.17   -1 13.3   6.632   5.851    35   14.5  18:45 ( 78, 15)  
Oct. 25  15 55.57   -1 15.6   6.706   5.878    31   14.6  18:38 ( 80, 12)  

* C/2022 QE78 ( ATLAS )

Now it is 15.6 mag (Sept. 28, Alfons Diepvens). It stays 15 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. 18   9  6.79   19 15.9   5.724   5.483    71   14.7   4:44 (284, 52)  
Oct. 25   9 11.03   19 28.4   5.620   5.485    77   14.6   4:49 (290, 58)  

* 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. 18  13 36.39   -8 24.7   3.053   2.058     1   15.0  18:45 ( 91,-16)  
Oct. 25  13 51.06   -9 55.4   3.004   2.011     2   14.7   4:49 (271,-16)  

* 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.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 18  18 33.57  -10 16.2   5.347   5.168    74   15.0  18:45 ( 38, 37)  
Oct. 25  18 35.56   -9 50.6   5.417   5.131    68   15.0  18:38 ( 42, 35)  

* 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. 18   5 41.99  -72 47.8  14.626  14.636    88   15.0   3:55 (  0,-18)  
Oct. 25   5 40.50  -73 13.8  14.620  14.614    87   15.0   3:26 (  0,-18)  

* 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. 18   9 55.96    4 50.0   2.929   2.501    55   15.0   4:44 (290, 34)  
Oct. 25  10  6.32    3 33.0   2.868   2.513    59   15.0   4:49 (296, 37)  

* 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. 18  22 57.95   48 56.3   4.358   5.049   129   15.2  21:09 (180, 76)  
Oct. 25  22 49.35   47  2.9   4.423   5.089   127   15.3  20:33 (180, 78)  

* 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. 18   3 13.34  -45 47.1   5.528   6.090   120   15.5   1:28 (  0,  9)  
Oct. 25   3  9.49  -46  1.1   5.492   6.048   119   15.5   0:57 (  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. 18  13 52.07  -57  2.7   2.557   2.026    47   15.6  18:45 ( 40,-34)  
Oct. 25  14  8.30  -54 56.3   2.585   1.977    43   15.5  18:38 ( 43,-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. 18  20  0.95  -13 53.0   2.502   2.772    94   15.9  18:45 ( 10, 41)  
Oct. 25  20  6.28  -13 55.0   2.566   2.740    89   15.9  18:38 ( 15, 40)  

* 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. 18  22 38.67  -10  4.4   2.033   2.808   132   16.0  20:51 (  0, 45)  
Oct. 25  22 38.02   -9 32.4   2.105   2.808   126   16.1  20:22 (  0, 46)  

* 414P/STEREO

It brightened very rapidly. Now it is 15.0 mag (Sept. 23, Ken-ichi Kadota). Fading rapidly. It will be fainter than 18 mag soon. It will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 18  12 26.99  -13 43.6   1.589   0.690    16   16.1   4:44 (282, -7)  
Oct. 25  12 58.75  -17 17.6   1.699   0.784    15   17.7   4:49 (285, -9)  

* C/2023 C2 ( ATLAS )

It brightened up to 12.7 mag in 2024 summer (Aug. 7, 2024, Thomas Lehmann). Now it is 15.7 mag (Sept. 23, ATLAS-MLO, Mauna Loa). Fading slowly. 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. 18  22 19.90   56 18.4   3.636   4.228   120   16.1  20:31 (180, 69)  
Oct. 25  22 17.60   55 27.3   3.707   4.283   119   16.2  20:02 (180, 69)  

* 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. 18  18 59.43  -30 39.5   3.025   2.990    78   16.2  18:45 ( 21, 21)  
Oct. 25  19  8.48  -30 19.2   3.123   2.997    73   16.2  18:38 ( 24, 20)  

* 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. 18   8 49.44   33 52.5   4.091   4.029    79   16.3   4:44 (262, 61)  
Oct. 25   8 52.33   35 25.8   3.991   4.046    86   16.3   4:49 (261, 68)  

* 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. 18   8 49.92  -11 23.5   6.868   6.575    68   16.4   4:44 (318, 33)  
Oct. 25   8 52.48  -11 34.7   6.777   6.578    74   16.3   4:49 (326, 37)  

* 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. 18  20 11.36  -15 14.5   1.716   2.088    97   16.5  18:45 (  7, 40)  
Oct. 25  20 20.68  -14 39.8   1.778   2.075    92   16.5  18:38 ( 10, 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. 18  14 29.29   63 20.8   4.582   4.407    73   16.5  18:45 (149, 30)  
Oct. 25  14 49.81   63 24.1   4.552   4.419    76   16.5  18:38 (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. 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. 18   8 49.96   12 59.4   2.166   2.107    73   16.6   4:44 (296, 51)  
Oct. 25   8 57.85   12 43.3   2.136   2.165    78   16.7   4:49 (303, 56)  

* 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. 18   0 26.81   -5 31.9   2.491   3.436   158   16.7  22:38 (  0, 50)  
Oct. 25   0 23.46   -5 48.5   2.543   3.445   150   16.8  22:07 (  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. 18   5 16.50   49 49.8   3.283   3.860   118   16.9   3:32 (180, 75)  
Oct. 25   5 16.16   50 40.8   3.207   3.854   124   16.8   3:04 (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. 18  22 17.10  -21 19.3   1.401   2.119   123   16.9  20:29 (  0, 34)  
Oct. 25  22 18.31  -20  6.4   1.440   2.092   117   16.9  20:03 (  0, 35)  

* 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. 18  11  1.67  -22 49.7   6.290   5.540    38   16.9   4:44 (301,  3)  
Oct. 25  11  2.58  -23  4.6   6.245   5.558    42   16.9   4:49 (306,  9)  

* 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. 18   8 45.91   78 43.2   4.921   5.118    95   17.0   4:44 (189, 44)  
Oct. 25   9 10.84   80 11.5   4.866   5.112    98   16.9   4:49 (187, 43)  

* 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. 18  21 37.36   22 47.0   6.649   7.236   122   17.0  19:49 (  0, 78)  
Oct. 25  21 34.54   22 27.7   6.693   7.197   116   17.0  19:19 (  0, 78)  

* 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. 18   0 33.53  -57 15.9  10.554  10.970   112   17.0  22:45 (  0, -2)  
Oct. 25   0 28.50  -56 56.4  10.624  10.983   108   17.0  22:12 (  0, -2)  

* 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. 18   3  7.64   38 30.2   8.056   8.879   143   17.1   1:23 (180, 86)  
Oct. 25   3  5.14   38 32.2   7.998   8.869   149   17.1   0:53 (180, 86)  

* 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. 18  10  0.24   20 32.5   2.466   2.146    59   17.2   4:44 (273, 42)  
Oct. 25  10 12.70   20 14.5   2.430   2.184    63   17.1   4:49 (277, 46)  

* 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 17 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. 18  18 53.20  -69 15.8   8.690   8.535    77   17.1  18:45 (  9,-16)  
Oct. 25  18 54.00  -68 40.2   8.822   8.586    73   17.2  18:38 ( 11,-16)  

* 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. 18   9 31.48  -19 24.1   4.892   4.453    58   17.2   4:44 (314, 20)  
Oct. 25   9 36.60  -20 35.0   4.822   4.456    62   17.1   4:49 (321, 23)  

* C/2025 R1 ( ATLAS )

Now it is 17.5 mag (Sept. 23, 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. 18  18 54.71   72 21.6   1.655   2.024    96   17.2  18:45 (168, 51)  
Oct. 25  18 43.69   65  8.4   1.686   2.007    93   17.2  18:38 (157, 54)  

* 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. 18  11 15.95   70  4.2   4.166   4.161    82   17.3   4:44 (205, 39)  
Oct. 25  11 18.22   70 31.5   4.064   4.131    86   17.2   4:49 (204, 41)  

* C/2025 Q3 ( ATLAS )

Now it is 17.3 mag (Oct. 13, ATLAS-TDO). 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. 18   4 15.82   40  6.2   1.822   2.599   132   17.5   2:32 (180, 85)  
Oct. 25   4  3.54   37 21.2   1.696   2.554   142   17.2   1:52 (180, 87)  

* 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. 18   6 18.06   28 57.0   9.378   9.771   110   17.4   4:33 (  0, 84)  
Oct. 25   6 16.55   29 10.1   9.318   9.820   117   17.4   4:04 (  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. 18   5 48.80  -45 18.7   8.140   8.378   100   17.4   4:03 (  0, 10)  
Oct. 25   5 44.50  -45 57.1   8.144   8.422   102   17.4   3:31 (  0,  9)  

* 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. 18  19 52.72  -14 20.0   5.002   5.149    92   17.4  18:45 ( 13, 40)  
Oct. 25  19 55.85  -14  2.5   5.137   5.177    86   17.5  18:38 ( 18, 39)  

* 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. 18   0 44.91  -68 43.8   5.435   5.715   101   17.4  22:55 (  0,-14)  
Oct. 25   0 25.79  -68 14.7   5.515   5.741    98   17.5  22:08 (  0,-13)  

* 48P/Johnson

Now it is 16.2 mag (Sept. 30, Thomas Lehmann). 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. 18   3 56.03    3 22.9   1.762   2.630   143   17.4   2:11 (  0, 58)  
Oct. 25   3 51.37    3  2.8   1.750   2.660   150   17.6   1:39 (  0, 58)  

* C/2024 X2 ( ATLAS )

Now it is 17.7 mag (June 26, 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. 18   9 22.74   -6 51.9   4.155   3.780    61   17.7   4:44 (307, 31)  
Oct. 25   9 24.16   -6 26.6   4.063   3.795    67   17.6   4:49 (314, 37)  

* C/2024 J2 ( Wierzchos )

It brightened rapidly up to 14.6 mag in winter (Jan. 31, Thomas Lehmann). Now it is 17.1 mag (Sept. 25, ATLAS-MLO, Mauna Loa). 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. 18   2 51.88  -47  1.7   2.486   3.114   120   17.6   1:07 (  0,  8)  
Oct. 25   2 42.98  -48 45.9   2.580   3.176   118   17.8   0:31 (  0,  6)  

* 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. 18   6 41.04  -19 44.3   8.015   8.218    98   17.7   4:44 (357, 35)  
Oct. 25   6 39.64  -20  0.6   7.975   8.265   103   17.7   4:26 (  0, 35)  

* 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. 18  17 17.53    4 38.3   5.498   5.045    58   17.7  18:45 ( 67, 36)  
Oct. 25  17 23.53    3 57.0   5.557   5.032    53   17.7  18:38 ( 70, 33)  

* (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. 18   3 19.35   43  7.6   1.482   2.327   138   17.9   1:36 (180, 82)  
Oct. 25   3  1.18   42 33.0   1.450   2.344   146   17.7   0:50 (180, 82)  

* 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. 18   7 58.26  -10 53.1   4.223   4.194    81   17.8   4:44 (331, 39)  
Oct. 25   8  1.52  -11 40.2   4.144   4.204    86   17.8   4:49 (341, 41)  

* 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. 18  22 53.24   40  1.4   6.123   6.848   133   17.8  21:05 (180, 85)  
Oct. 25  22 51.17   39  7.8   6.216   6.907   130   17.8  20:35 (180, 86)  

* C/2024 N3 ( Sarneczky )

Now it is 17.5 mag (Sept. 23, 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. 18  16 49.81   41 32.2   5.504   5.221    68   17.8  18:45 (116, 46)  
Oct. 25  16 54.93   39 57.7   5.556   5.236    66   17.8  18:38 (114, 43)  

* 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. 18   7  7.24    8 31.4   3.893   4.137    97   17.8   4:44 (340, 62)  
Oct. 25   7  9.17    7 58.4   3.804   4.147   103   17.8   4:49 (356, 63)  

* 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. 18  20 20.45  -57 11.2   2.754   2.907    88   17.8  18:45 (  2, -2)  
Oct. 25  20 20.18  -57 43.8   2.841   2.892    82   17.9  18:38 (  4, -3)  

* C/2023 A3 ( Tsuchinshan-ATLAS )

It brightened up to -3 mag due to the forward scattering in the SOHO coronagraph images (Oct. 9, 2024, Q.-c. Zhang, Charles S. Morris). It became a great comet of 0 mag on the ground. Now it is 17.2 mag (Oct. 2, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag soon. In the Northern Hemisphere, it will be getting lower gradually. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 18  17 57.57   14 54.7   5.714   5.462    70   17.8  18:45 ( 70, 50)  
Oct. 25  17 59.68   14 15.5   5.869   5.532    65   18.0  18:38 ( 73, 46)  

* 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. 18  19 45.24   -3 16.5  14.904  14.989    93   17.9  18:45 ( 19, 50)  
Oct. 25  19 45.80   -3 21.9  15.031  15.003    86   18.0  18:38 ( 26, 49)  

* 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. 18   0 13.14    3  9.2   1.692   2.649   159   18.1  22:25 (  0, 58)  
Oct. 25   0 10.06    2 40.5   1.752   2.670   151   18.2  21:54 (  0, 58)  

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