Weekly Information about Bright Comets (2026 Oct. 24: North)

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Updated on October 31, 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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* 161P/Hartley-IRAS

Now it is 10.3 mag (Oct. 29, Chris Wyatt). It will fade out rapidly after this. In the Northern Hemisphere, it will be getting lower gradually. But it will be getting higher again after January. 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. 24  20 21.73   10 59.7   0.769   1.351    99   10.6  18:39 ( 17, 65)  
Oct. 31  19 57.65   13 27.4   0.905   1.321    88   10.7  18:32 ( 42, 63)  

* 10P/Tempel 2

It brightened up to 6.9 mag in summer (Aug. 5, Juan Jose Gonzalez). Now it is 11.0 mag (Oct. 29, Chris Wyatt). 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. 24  23 12.99  -28 37.5   0.876   1.655   124   10.9  21:03 (  0, 27)  
Oct. 31  23 21.71  -26 43.8   0.953   1.692   120   11.2  20:44 (  0, 29)  

* 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 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. 24  12  5.45   -4 16.7   1.799   1.024    27   12.3   4:48 (281,  8)  
Oct. 31  12 36.01   -6 41.2   1.797   1.009    26   11.9   4:54 (283,  7)  

* C/2024 T5 ( ATLAS )

Now it is 12.6 mag (Oct. 22, 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. 24   5 45.59  -13 39.9   3.651   4.197   116   12.5   3:38 (  0, 41)  
Oct. 31   5 44.09  -13 36.8   3.557   4.173   122   12.5   3:09 (  0, 41)  

* C/2026 A2 ( Bok )

Now it is 13.1 mag (Oct. 28, Yoshimi Nagai). Fading slowly. 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. 24  19 34.21   59 19.3   1.689   2.070    97   13.2  18:39 (159, 63)  
Oct. 31  20  1.79   55 15.6   1.637   2.042    98   13.1  18:32 (155, 67)  

* 11P/Tempel-Swift-LINEAR

Now it is 14.7 mag (Oct. 17, Alfons Diepvens). It will turn to fade out rapidly after the peak. 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. 24   2 27.55   35 20.2   0.434   1.400   154   13.6   0:20 (180, 89)  
Oct. 31   2 36.08   32 18.8   0.415   1.392   161   13.1   0:01 (  0, 88)  

* P/2026 R2 ( Leonard )

Bright new comet. It approached to Earth down to 0.3 a.u. in early October, and brightened up to 11.7 mag (Sept. 30, Thomas Lehmann). Now it is 14.2 mag (Oct. 29, Chris Wyatt). It will fade out rapidly after this. It will be fainter than 18 mag in January. In the Northern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  16 21.53  -55  7.7   0.556   0.790    52   13.2  18:39 ( 33,-17)  
Oct. 31  16  8.51  -62 58.3   0.707   0.797    52   13.8  18:32 ( 29,-25)  

* 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 12.3 mag (Oct. 28, Alfons Diepvens). It will fade out rapidly after this. 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. 24   3 20.31    3  7.1   1.030   1.983   156   13.5   1:13 (  0, 58)  
Oct. 31   3 13.95    2 27.3   1.051   2.020   162   13.8   0:39 (  0, 58)  

* C/2024 J3 ( ATLAS )

Now it is 13.7 mag (Oct. 27, Yoshimi Nagai). It stays 14 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. 24  18 31.09   41  4.0   3.873   3.876    82   13.7  18:39 (113, 62)  
Oct. 31  18 34.85   40 54.9   3.911   3.872    80   13.7  18:32 (113, 59)  

* 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. 24   7 50.79   14 39.7   1.940   2.231    93   13.9   4:48 (326, 66)  
Oct. 31   7 57.44   13 55.9   1.883   2.255    98   13.9   4:54 (342, 68)  

* 260P/McNaught

It brightened up to 13 mag from summer to autumn. Now it is 14.7 mag (Oct. 28, Alfons Diepvens). 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. 24   6 18.18   47 50.6   0.991   1.668   114   14.0   4:11 (180, 77)  
Oct. 31   6 22.02   49 10.0   0.984   1.708   119   14.2   3:47 (180, 76)

* 88P/Howell

It brightened up to 9.6 mag in the very low sky in spring (Apr. 14, Chris Wyatt). Now it is 14.4 mag (Oct. 22, Toru Yusa). It will fade out rapidly after this. It will be fainter than 18 mag in February. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24   2 46.36   13 39.5   1.522   2.501   166   14.1   0:39 (  0, 69)  
Oct. 31   2 38.33   13 14.7   1.555   2.546   175   14.3   0:04 (  0, 68)  

* P/2026 T1 ( ATLAS )

Bright new comet. It must be just in outburst. Now it is 14.4 mag (Oct. 18, Michael Jager). It stays 15 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. 24  19 24.44   -5  9.2   3.533   3.537    82   14.2  18:39 ( 31, 45)  
Oct. 31  19 30.79   -5 18.8   3.631   3.541    76   14.3  18:32 ( 35, 43)  

* 29P/Schwassmann-Wachmann 1

Now it is 13.6 mag (Aug. 2, Andrew Pearce). In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it will be unobservable temporarily in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  12 19.55   -9 11.5   7.222   6.318    22   14.3   4:48 (283,  2)  
Oct. 31  12 24.03   -9 45.6   7.172   6.318    28   14.3   4:54 (288,  7)  

* 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. 24   7 43.81  -73 14.0  13.650  13.505    79   14.5   4:48 (357,-19)  
Oct. 31   7 45.00  -73 41.3  13.639  13.485    79   14.5   4:54 (359,-19)  

* C/2024 R4 ( PanSTARRS )

Now it is 14.3 mag (Oct. 17, 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. 24  19 43.96   44 45.8   5.106   5.313    96   14.5  18:39 (133, 74)  
Oct. 31  19 41.67   44  0.5   5.136   5.283    93   14.5  18:32 (125, 71)  

* 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 14.5 mag (Oct. 22, Toru Yusa). Fading rapidly. It will be fainter than 18 mag in November. It will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  10 49.20   -1  7.4   1.137   0.854    46   14.7   4:48 (291, 25)  
Oct. 31  11  4.95   -2 29.2   1.210   0.940    49   15.7   4:54 (295, 27)  

* 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. 24  12  6.51   10 23.1   2.922   2.173    34   14.9   4:48 (269, 16)  
Oct. 31  12 20.28    8 48.4   2.885   2.180    37   14.9   4:54 (273, 19)  

* C/2023 R1 ( PanSTARRS )

Now it is 14.7 mag (Sept. 19, Mike Olason). It stays 15 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in December. In the Southern Hemisphere, it will be unobservable in November. But it will be observable again in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  15 30.95  -19 40.0   4.854   3.975    25   15.0  18:39 ( 68, -3)  
Oct. 31  15 32.72  -20 15.4   4.931   4.003    18   15.1  18:32 ( 70, -7)  

* (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. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  20 26.44   45 39.6   0.476   1.203   104   15.0  18:39 (161, 79)  
Oct. 31  21 14.70   38 29.3   0.572   1.300   109   15.4  18:39 (180, 87)  

* C/2025 V2 ( Rankin )

It is expected to brighten up to 12.5 mag in 2027 spring. Now it is 16.5 mag (Oct. 25, Martin Masek). Brightening gradually. In the Northern Hemisphere, it will be getting higher gradually. 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. 24  12 41.27   14 58.4   3.442   2.649    31   15.4   4:48 (260, 12)  
Oct. 31  12 55.26   14 25.7   3.344   2.596    35   15.3   4:54 (263, 15)  

* 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. 24  14  4.03   -3 45.6   5.398   4.416     8   15.6  18:39 ( 93,-11)  
Oct. 31  14 11.54   -4 19.2   5.339   4.364     9   15.5   4:54 (268,-11)  

* C/2022 QE78 ( ATLAS )

Now it is 16.7 mag (Oct. 19, D. Buczynski). It stays 16 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 December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  11 30.24   26 15.8   6.799   6.225    51   15.6   4:48 (258, 32)  
Oct. 31  11 35.68   26 17.3   6.740   6.249    56   15.6   4:54 (262, 37)  

* C/2022 N2 ( PanSTARRS )

Now it is 16.1 mag (Oct. 9, Ken-ichi Kadota). 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. 24   7 34.06   25 22.0   5.160   5.406    99   15.9   4:48 (317, 77)  
Oct. 31   7 35.31   25 20.7   5.093   5.446   105   15.9   4:54 (352, 80)  

* C/2025 M2 ( PanSTARRS )

It is expected to brighten up to 12 mag from 2027 to 2028. Now it is 15.5 mag (Oct. 14, Jean-Gabriel Bosch). 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. 24  18 38.57  -21 26.5   5.005   4.736    68   15.9  18:39 ( 34, 26)  
Oct. 31  18 37.81  -21 25.1   5.075   4.685    61   15.9  18:32 ( 39, 23)  

* 112P/Urata-Niijima

Now it is 16.0 mag (Oct. 17, Toru Yusa). 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. 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. 24   8 24.35   43 34.4   1.062   1.484    92   16.1   4:48 (237, 71)  
Oct. 31   8 48.48   45 12.1   1.048   1.503    94   16.1   4:54 (230, 72)  

* 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. 24  23 54.74   16 38.0   0.975   1.907   151   16.4  21:43 (  0, 72)  
Oct. 31  23 37.07   14 56.5   0.947   1.827   140   16.2  20:57 (  0, 70)  

* 114P/Wiseman-Skiff

Now it is 16.8 mag (Oct. 22, Toru Yusa). Fading gradually. 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. 24   9 30.53    9 31.7   1.696   1.620    68   16.3   4:48 (297, 47)  
Oct. 31   9 44.63    6 53.6   1.661   1.639    71   16.4   4:54 (304, 48)  

* 84P/Giclas

Now it is 17.2 mag (Oct. 11, Ken-ichi Kadota). It stays 16 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. 24  20 39.47  -25 25.3   1.646   2.001    95   16.4  18:39 (  2, 30)  
Oct. 31  20 48.86  -24 50.7   1.691   1.971    90   16.4  18:32 (  5, 30)  

* 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. 24  17 18.10   12  3.3   8.090   7.582    56   16.4  18:39 ( 78, 37)  
Oct. 31  17 21.82   11 51.9   8.189   7.618    52   16.5  18:32 ( 81, 34)  

* C/2025 J1 ( Borisov )

Now it is 16.7 mag (Oct. 17, 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. 24   7 10.42    7 53.2   3.449   3.780   101   16.5   4:48 (352, 63)  
Oct. 31   7  6.56    6  2.9   3.358   3.801   109   16.4   4:31 (  0, 61)  

* C/2026 AZ17 ( Bok )

Now it is 16.7 mag (Oct. 18, ATLAS-HKO, Haleakala). It stays 17 mag for a while. 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. 24  18  0.29   -2  4.6   2.799   2.494    62   16.7  18:39 ( 56, 36)  
Oct. 31  18 13.13   -3 32.6   2.855   2.485    58   16.7  18:32 ( 56, 33)  

* C/2022 R6 ( PanSTARRS )

It was observed at 16 mag from 2025 to 2026. Now it is 17.2 mag (Oct. 24, ATLAS-HKO, Haleakala). 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. 24  10 14.63    5  6.2   7.647   7.149    56   17.0   4:48 (292, 35)  
Oct. 31  10 17.62    5  9.2   7.564   7.167    62   16.9   4:54 (298, 41)  

* 346P/Catalina

Now it is 17.3 mag (Oct. 21, 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. 24   9  3.04   19  7.4   2.319   2.319    77   17.1   4:48 (291, 58)  
Oct. 31   9 13.64   19 23.7   2.252   2.336    82   17.0   4:54 (298, 62)  

* 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. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  10  8.14   30 57.3   4.433   4.173    68   17.0   4:48 (262, 50)  
Oct. 31  10 14.00   30 38.8   4.355   4.189    73   17.0   4:54 (266, 55)  

* 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 16.5 mag (Oct. 21, 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. 24   1 55.62   20 45.2   1.205   2.193   170   17.0  23:44 (  0, 76)  
Oct. 31   1 52.39   18 55.0   1.221   2.208   171   17.1  23:14 (  0, 74)  

* C/2026 O1 ( PanSTARRS )

Now it is 17.1 mag (Oct. 17, Ken-ichi Kadota). Brightening slowly. It will be unobservable in January in the Northern Hemisphere, or in February in the Southern Hemisphere. At the high light, it will be observable in good condition in the Southern Hemisphere, but it will not be observable in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  22 17.06  -30 51.3   3.146   3.653   113   17.1  20:06 (  0, 24)  
Oct. 31  22  8.96  -31 31.4   3.201   3.585   104   17.1  19:31 (  0, 24)  

* 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 stays observable in good condition. 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. 24  11 18.32   30 16.6   5.938   5.443    55   17.2   4:48 (255, 36)  
Oct. 31  11 25.12   30 15.0   5.846   5.433    60   17.2   4:54 (258, 41)  

* C/2025 E1 ( PanSTARRS )

Now it is 17.6 mag (Sept. 12, 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. 24  14 18.91  -80 22.8   4.256   4.007    68   17.2  18:39 ( 12,-35)  
Oct. 31  15 20.25  -80 56.3   4.287   4.011    67   17.2  18:32 ( 11,-34)  

* 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. 24   7 13.89  -30 32.8   2.977   3.176    92   17.4   4:48 (356, 24)  
Oct. 31   7  5.21  -31 50.7   2.977   3.264    97   17.5   4:29 (  0, 23)  

* 188P/LINEAR-Mueller

Now it is 18.0 mag (Oct. 17, Ken-ichi Kadota). 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. 24   6 28.37   36  5.0   2.316   2.864   113   17.5   4:21 (180, 89)  
Oct. 31   6 29.92   36 34.8   2.256   2.885   120   17.5   3:55 (180, 88)  

* 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. 24  23 56.69  -44 37.4  11.272  11.772   118   17.5  21:46 (  0, 11)  
Oct. 31  23 53.69  -44 17.5  11.366  11.789   113   17.5  21:15 (  0, 11)  

* 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 17.0 mag (Oct. 22, ATLAS South Africa). 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. 24   1 16.43   -1 27.9   3.729   4.694   164   17.6  23:05 (  0, 54)  
Oct. 31   1  9.91   -1 13.4   3.710   4.640   157   17.5  22:31 (  0, 54)  

* 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. 24   5 27.05   38  8.2   1.677   2.396   125   17.7   3:20 (180, 87)  
Oct. 31   5 27.86   37  4.0   1.604   2.387   132   17.6   2:53 (180, 88)  

* 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). 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. 24  21 46.17   22  8.3   6.781   7.336   120   17.6  19:35 (  0, 77)  
Oct. 31  21 44.18   21 10.9   6.913   7.380   114   17.7  19:06 (  0, 76)  

* C/2025 B2 ( Borisov )

Now it is 17.5 mag (Oct. 20, ATLAS-HKO, Haleakala). 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. 24  17 16.12   71 14.3   8.191   8.243    89   17.6  18:39 (159, 44)  
Oct. 31  17 23.65   70 13.1   8.186   8.244    89   17.6  18:32 (157, 44)  

* C/2024 G4 ( PanSTARRS )

Now it is 17.9 mag (Oct. 11, Ken-ichi Kadota). 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. 24  20 10.62   -7 44.5   5.033   5.179    92   17.7  18:39 ( 14, 46)  
Oct. 31  20 14.24   -8 13.5   5.156   5.196    86   17.7  18:32 ( 20, 45)  

* C/2026 S2 ( ATLAS )

Now it is 18.1 mag (Oct. 8, M. Jaeger, G. Rhemann, E. Prosperi). 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. 24   6  3.66   -0 56.7   4.203   4.730   116   17.9   3:56 (  0, 54)  
Oct. 31   5 55.96   -1 35.9   4.080   4.710   124   17.8   3:21 (  0, 53)  

* C/2023 X2 ( Lemmon )

Now it is 17.8 mag (July 6, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. 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. 24  15 22.89   51  9.4   5.905   5.570    65   17.8  18:39 (133, 31)  
Oct. 31  15 30.55   50  4.7   5.923   5.592    65   17.8  18:32 (133, 29)  

* 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. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24   8 51.33    5 42.0   2.342   2.327    76   17.9   4:48 (311, 50)  
Oct. 31   9  0.34    4 18.6   2.272   2.335    81   17.8   4:54 (321, 53)  

* 93P/Lovas 1

Now it is 18.0 mag (Oct. 8, Kunihiro Shima). 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. 24  10 26.11   15  4.1   2.776   2.395    57   17.9   4:48 (279, 39)  
Oct. 31  10 35.32   13 59.8   2.741   2.439    62   18.0   4:54 (285, 43)  

* 65P/Gunn

Now it is 17.6 mag (Oct. 9, Ken-ichi Kadota). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24   0 15.16   -9  5.3   2.798   3.681   148   17.9  22:04 (  0, 46)  
Oct. 31   0 11.98   -9  4.1   2.872   3.696   140   18.0  21:33 (  0, 46)  

* 69P/Taylor

It has not been observed yet in this apparition. 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. 24   7 15.94   11 49.1   1.863   2.275   101   18.1   4:48 (348, 66)  
Oct. 31   7 22.43   12 13.0   1.781   2.272   106   17.9   4:47 (  0, 67)  

* 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. It will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 24  11 24.93   -4  9.5   1.890   1.253    37   20.4   4:48 (287, 16)  
Oct. 31  11 22.15   -6 56.9   1.910   1.381    44   20.9   4:54 (295, 21)  

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