Weekly Information about Bright Comets (2024 Sept. 21: North)

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Updated on September 25, 2024
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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/2023 A3 ( Tsuchinshan-ATLAS )

It will approach to Sun down to 0.4 a.u. in late September, and it is expected to brighten up to 2 mag. Now it is 3.1 mag (Sept. 23, Virgilio Gonano). It will turn to fade out rapidly after the peak. It will be unobservable temporarily around Oct. 10.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  10 35.45   -5 55.5   1.191   0.432    20    3.6   4:52 (277,  0)  
Sept.28  10 47.87   -6  2.8   0.897   0.391    22    2.7   4:58 (281,  4)  

* 13P/Olbers

It returned for the first time in 68 years. It brightened up to 6.2 mag in early summer (July 1, Virgilio Gonano). Now it is 8.8 mag (Sept. 19, Virgilio Gonano). It will fade out rapidly after this. It will be unobservable in October in the Southern Hemisphere, or in November in the Northern Hemisphere. But it will be observable again in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  14 15.09    9  6.6   2.395   1.693    36    9.5  19:22 ( 90, 16)  
Sept.28  14 32.51    6  7.5   2.496   1.763    34    9.9  19:12 ( 87, 14)  

* 12P/Pons-Brooks

It returns for the first time in 70 years. It brightened up to 3.7 mag in early April (Apr. 6, Jose Guilherme Aguiar). Now it is 10.4 mag (Sept. 5, Thomas Lehmann). Fading gradually. In the Northern Hemisphere, it is not observable now. 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)  
Sept.21  13 20.33  -47 32.7   3.013   2.521    51   11.3  19:22 ( 48,-26)  
Sept.28  13 38.68  -47 32.4   3.154   2.605    48   11.6  19:12 ( 48,-25)  

* C/2022 E2 ( ATLAS )

Now it is 12.9 mag (Sept. 4, Ken-ichi Kadota). It stays 12 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)  
Sept.21   7 37.60   48 15.4   3.843   3.667    72   12.2   4:22 (234, 52)  
Sept.28   7 36.52   50  1.0   3.722   3.668    79   12.1   4:28 (230, 57)  

* C/2023 R2 ( PanSTARRS )

It will fade out rapidly after this. In the Northern Hemisphere, it will be unobservable in December. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  13 22.08    0 54.5   2.012   1.147    22   12.6  19:22 ( 91,  0)  
Sept.28  13 50.69    0  9.2   2.079   1.223    23   13.0  19:12 ( 88,  2)  

* C/2023 C2 ( ATLAS )

Now it is 13.1 mag (Aug. 29, Chris Wyatt). It stays 13 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)  
Sept.21  17  7.19  -40 59.7   2.384   2.452    81   12.8  19:22 ( 25,  8)  
Sept.28  17 19.80  -38 46.2   2.447   2.433    77   12.8  19:12 ( 27,  9)  

* C/2024 B1 ( Lemmon )

It became much brighter than expected. Now it is 13.8 mag (Sept. 8, Michael Jager). Fading 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.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  10 41.94   49 51.9   2.076   1.649    51   13.6   4:22 (225, 23)  
Sept.28  11 22.99   49 40.6   2.033   1.639    53   13.5   4:28 (224, 22)  

* 37P/Forbes

Now it is 13.9 mag (Sept. 20, Mike Olason). Fading gradually. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  15 46.09  -25 17.3   1.841   1.630    61   13.8  19:22 ( 48, 11)  
Sept.28  16  7.27  -25 43.7   1.876   1.623    59   13.8  19:12 ( 47, 11)  

* 29P/Schwassmann-Wachmann 1

Now it is 16.5 mag (Sept. 20, Jean-Francois Soulier). In the Northern Hemisphere, it will be getting higher gradually. 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)  
Sept.21   9 42.24   12 52.3   7.032   6.232    34   14.2   4:22 (265, 15)  
Sept.28   9 46.60   12 25.5   6.963   6.234    40   14.2   4:28 (269, 21)  

* C/2021 G2 ( ATLAS )

Now it is 14.1 mag (Aug. 29, Chris Wyatt). It stays 14 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in November. In the Southern Hemisphere, it will be unobservable in October. But it will be observable again in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  13 19.49  -18 49.4   5.839   4.983    28   14.3  19:22 ( 75,-12)  
Sept.28  13 26.68  -18 50.8   5.885   4.984    23   14.3  19:12 ( 76,-14)  

* C/2022 N2 ( PanSTARRS )

It is expected to brighten up to 13 mag in 2025 autumn, and it will be observable in good condition. Now it is 14.5 mag (Sept. 5, Ken-ichi Kadota). It stays 15 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  22 43.68   -4 57.4   3.724   4.689   162   14.6  22:41 (  0, 50)  
Sept.28  22 41.13   -5  8.4   3.730   4.656   154   14.5  22:11 (  0, 50)  

* C/2021 S3 ( PanSTARRS )

It brightened up to 9.6 mag from February to March (Feb. 25, Thomas Lehmann). Now it is 13.3 mag (Sept. 5, Osamu Miyazaki). Fading gradually. 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)  
Sept.21  19 27.36   48 56.2   2.794   3.199   104   14.8  19:25 (180, 76)  
Sept.28  19 32.06   47  1.4   2.883   3.272   103   14.9  19:12 (172, 78)  

* C/2022 QE78 ( ATLAS )

Now it is 15.7 mag (Sept. 1, Hiroshi Abe). It stays 14 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   6 37.60    3 12.9   6.172   6.059    78   14.9   4:22 (308, 45)  
Sept.28   6 40.34    3  8.4   6.048   6.038    84   14.8   4:28 (317, 50)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. Now it is 14.0 mag (Aug. 31, Chris Wyatt). Fading slowly. 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)  
Sept.21  21 55.97  -70 44.0   5.182   5.566   107   15.0  21:53 (  0,-16)  
Sept.28  21 39.81  -70 23.6   5.311   5.622   103   15.1  21:09 (  0,-15)  

* C/2024 G3 ( ATLAS )

It approaches to Sun down to 0.09 a.u. on Jan. 13, 2025. According to the calculation, it will brighten up to -1 mag. But probably, it will be disintegrated. At the high light, it may be observable after the perihelion passage only in the Southern Hemisphere. Now it is 15.7 mag (Aug. 31, ATLAS South Africa). It will brighten rapidly after this. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  13 48.23  -49 39.9   2.921   2.503    56   15.3  19:22 ( 44,-22)  
Sept.28  13 57.97  -48 35.7   2.893   2.397    51   15.1  19:12 ( 46,-23)  

* C/2023 V4 ( Camarasa-Duszanowicz )

It brightened very rapidly up to 10.0 mag in June (June 11, Virgilio Gonano). Now it is 14.1 mag (Sept. 4, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in November. It will be unobservable in October in the Southern Hemisphere, or in November in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  14 23.61   16 48.2   2.713   2.054    40   15.1  19:22 ( 96, 21)  
Sept.28  14 35.66   14  0.2   2.839   2.134    37   15.5  19:12 ( 94, 19)  

* 130P/McNaught-Hughes

Now it is 14.9 mag (Sept. 4, Ken-ichi Kadota). 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)  
Sept.21   2 40.83    8  7.2   1.405   2.248   137   15.3   2:41 (  0, 63)  
Sept.28   2 37.46    7 55.1   1.386   2.279   144   15.4   2:11 (  0, 63)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 15.1 mag (Sept. 4, Ken-ichi Kadota). 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)  
Sept.21   6 26.75   17 49.9   6.906   6.836    81   15.4   4:22 (294, 57)  
Sept.28   6 26.82   18  0.9   6.842   6.891    88   15.4   4:28 (304, 64)  

* P/2024 N5 ( Siding Spring )

First return of a new periodic comet which brightened up to 16 mag in 2012. It is expected to brighten rapidly up to 14.5 mag in autumn. Now it is 16.6 mag (Sept. 6, E. Cortes). 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 December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   4 39.72    8 47.2   1.262   1.840   108   15.7   4:22 (350, 63)  
Sept.28   4 44.12   11 36.6   1.183   1.830   113   15.5   4:17 (  0, 67)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.0 mag (Sept. 10, Thomas Lehmann). 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)  
Sept.21   4 21.95  -67 55.3  15.745  15.935    99   15.5   4:21 (  0,-13)  
Sept.28   4 21.18  -68 23.4  15.732  15.911    98   15.5   3:53 (  0,-13)  

* 30P/Reinmuth 1

Now it is 16.5 mag (Apr. 3, Taras Prystavski). It stays 16 mag for a while. 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 November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  10 33.80   11 39.6   2.727   1.840    22   15.6   4:22 (259,  4)  
Sept.28  10 51.11   10 16.6   2.712   1.852    24   15.6   4:28 (262,  7)  

* 154P/Brewington

Now it is 15.4 mag (Sept. 4, Ken-ichi Kadota). 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)  
Sept.21   8 12.37   35 16.7   2.160   1.903    61   15.6   4:22 (252, 44)  
Sept.28   8 27.91   34 45.1   2.141   1.946    65   16.3   4:28 (254, 47)  

* C/2022 L2 ( ATLAS )

Now it is 15.6 mag (July 24, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in October. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   9 55.66  -27 42.4   4.048   3.343    40   15.7   4:22 (297,-11)  
Sept.28   9 55.84  -28 45.7   4.044   3.384    43   15.7   4:28 (302, -5)  

* C/2023 Q1 ( PanSTARRS )

Now it is 16.7 mag (Sept. 6, Ken-ichi Kadota). It stays 15 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)  
Sept.21   5 51.05   57 36.6   2.497   2.686    89   15.8   4:22 (207, 63)  
Sept.28   6  8.31   59 24.5   2.418   2.666    93   15.7   4:28 (201, 63)  

* 146P/Shoemaker-LINEAR

Now it is 15.3 mag (Sept. 8, Thomas Lehmann). 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)  
Sept.21   5 43.20   18 10.7   1.101   1.517    92   15.7   4:22 (308, 65)  
Sept.28   5 54.67   20 31.6   1.074   1.547    96   15.9   4:28 (314, 71)  

* C/2024 M1 ( ATLAS )

It is expected to brighten up to 13.5 mag, and it will be observable in good condition in winter. Now it is 16.8 mag (Sept. 9, ATLAS Chile). Brightening gradually. 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)  
Sept.21   6 47.28  -26 32.4   1.790   1.866    78   16.0   4:22 (326, 20)  
Sept.28   6 51.15  -25 35.2   1.684   1.832    81   15.8   4:28 (332, 24)  

* 472P/2023 RL75 ( NEAT-LINEAR )

Now it is 16.1 mag (Sept. 4, ATLAS-HKO, Haleakala). 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)  
Sept.21   6 19.75   14 43.8   3.389   3.423    83   16.1   4:22 (300, 57)  
Sept.28   6 25.44   14 15.8   3.301   3.430    88   16.1   4:28 (310, 61)  

* C/2019 L3 ( ATLAS )

It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 15.1 mag (Aug. 2, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it will never be observable after this. It locates somewhat low in the Southern Hemisphere. But it will become high in autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  11 43.87  -47 33.3   9.361   8.725    48   16.1   4:22 (307,-38)  
Sept.28  11 48.94  -47 57.0   9.431   8.770    46   16.2   4:28 (309,-34)  

* P/2023 S1

Now it is 16.8 mag (Sept. 3, ATLAS-MLO, Mauna Loa). Brightening slowly. 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)  
Sept.21   7 58.63   25 58.1   3.108   2.777    61   16.3   4:22 (266, 43)  
Sept.28   8  9.23   25 24.8   3.013   2.764    66   16.2   4:28 (269, 47)  

* C/2019 U5 ( PanSTARRS )

Now it is 15.5 mag (Sept. 5, ATLAS Chile). It stays 17 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)  
Sept.21   7 56.11  -39 28.3   6.202   5.887    67   16.3   4:22 (322,  1)  
Sept.28   7 55.64  -40 33.8   6.191   5.931    70   16.4   4:28 (327,  4)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.9 mag (Sept. 9, ATLAS Chile). 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)  
Sept.21   7  0.10  -26 29.9   7.132   6.948    75   16.4   4:22 (323, 18)  
Sept.28   7  2.97  -26 58.1   7.051   6.933    79   16.4   4:28 (330, 21)  

* C/2024 A1 ( ATLAS )

Now it is 17.3 mag (Sept. 5, ATLAS Chile). Brightening slowly. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   8  7.57  -25 58.5   4.911   4.503    60   16.5   4:22 (311,  9)  
Sept.28   8 10.65  -26  4.8   4.820   4.473    64   16.4   4:28 (316, 13)  

* C/2023 TD22 ( Lemmon )

Brightened rapidly. Now it is 16.1 mag (Sept. 5, Ken-ichi Kadota). Fading gradually. It will be fainter than 18 mag in November. It will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  20 57.78   -8 37.2   1.533   2.357   135   16.5  20:53 (  0, 46)  
Sept.28  20 33.10  -10 26.0   1.664   2.360   122   16.6  20:02 (  0, 45)  

* 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 16.2 mag (Sept. 10, Thomas Lehmann). It stays 17 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)  
Sept.21   7  0.63  -37 47.9   5.660   5.525    77   16.5   4:22 (329,  8)  
Sept.28   7  1.15  -38 19.1   5.653   5.574    80   16.5   4:28 (335, 11)  

* 299P/Catalina-PanSTARRS

It brightened very rapidly in outburst in late May. Now it is 17.0 mag (Sept. 4, ATLAS Chile). Fading slowly. It will be unobservable in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  16 18.44  -22 48.2   3.469   3.240    68   16.5  19:22 ( 44, 17)  
Sept.28  16 27.20  -22 53.0   3.565   3.248    63   16.6  19:12 ( 46, 16)  

* C/2023 F3 ( ATLAS )

Now it is 16.9 mag (Aug. 23, ATLAS South Africa). It stays 16 mag for a while. 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)  
Sept.21  13 26.71  -39 18.0   5.946   5.290    45   16.6  19:22 ( 56,-21)  
Sept.28  13 28.34  -39 14.5   6.001   5.280    40   16.6  19:12 ( 57,-24)  

* 253P/PanSTARRS

Now it is 16.9 mag (Sept. 4, Masayoshi Yoshimi). 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)  
Sept.21   0 55.00   -0 36.2   1.055   2.040   164   16.8   0:56 (  0, 55)  
Sept.28   0 51.97   -1 24.0   1.039   2.035   170   16.7   0:25 (  0, 54)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 17.0 mag (Sept. 1, ATLAS South Africa). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   2 25.43  -69 19.6  10.110  10.446   106   16.7   2:25 (  0,-14)  
Sept.28   2 16.82  -69 32.8  10.136  10.452   105   16.7   1:49 (  0,-14)  

* 89P/Russell 2

Now it is 16.2 mag (Sept. 8, ATLAS Chile). It will fade out rapidly after this. 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)  
Sept.21  23 25.21  -20 34.2   1.598   2.560   159   16.8  23:22 (  0, 35)  
Sept.28  23 19.98  -20 18.7   1.648   2.584   153   17.0  22:49 (  0, 35)  

* C/2022 U1 ( Leonard )

Now it is 16.8 mag (Sept. 3, S. Shurpakov). It stays 17 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)  
Sept.21  19 19.72   34 36.8   4.058   4.460   107   16.8  19:22 ( 68, 89)  
Sept.28  19 14.43   32 25.7   4.149   4.480   102   16.9  19:12 ( 67, 84)  

* C/2022 U3 ( Bok )

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)  
Sept.21   7 49.73   12 40.0   5.244   4.845    61   16.9   4:22 (282, 38)  
Sept.28   7 54.35   11 49.3   5.153   4.851    67   16.8   4:28 (289, 43)  

* C/2023 R1 ( PanSTARRS )

Now it is 17.0 mag (Sept. 1, 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 unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  23 10.52   30 26.3   5.188   6.056   147   16.9  23:07 (  0, 86)  
Sept.28  23  2.35   29 42.8   5.147   6.012   146   16.8  22:31 (  0, 85)  

* 43P/Wolf-Harrington

Now it is 17.5 mag (Sept. 5, ATLAS-HKO, Haleakala). 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)  
Sept.21   2 22.27   21 50.8   2.447   3.256   137   17.1   2:23 (  0, 77)  
Sept.28   2 20.14   21 39.3   2.360   3.228   144   17.0   1:53 (  0, 77)  

* C/2019 T4 ( ATLAS )

It brightened up to 11.1 mag in early 2022 (Mar. 31, 2022, F. Kugel, J.-G. Bosch, J. Nicolas). Now it is 16.1 mag (Sept. 2, ATLAS-MLO, Mauna Loa). It stays 18 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)  
Sept.21  17 17.92   27 43.0   7.826   7.747    81   17.0  19:22 ( 84, 62)  
Sept.28  17 20.27   27 10.1   7.934   7.788    78   17.1  19:12 ( 85, 59)  

* 49P/Arend-Rigaux

It will brighten up to 14 mag in 2025 spring. Now it is 17.5 mag (Sept. 4, ATLAS Chile). 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)  
Sept.21   0  7.89  -27 37.5   1.527   2.463   152   17.1   0:09 (  0, 28)  
Sept.28   0  1.43  -28 51.5   1.502   2.416   148   17.0  23:30 (  0, 26)  

* 190P/Mueller

Now it is 17.3 mag (Sept. 6, 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)  
Sept.21  22 43.81   -7  7.5   1.201   2.177   161   17.2  22:41 (  0, 48)  
Sept.28  22 40.36   -7 18.3   1.211   2.156   153   17.1  22:10 (  0, 48)  

* 192P/Shoemaker-Levy 1

Now it is 17.1 mag (Sept. 3, ATLAS-MLO, Mauna Loa). It will fade out rapidly after this. It will be fainter than 18 mag in October. 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)  
Sept.21   6 53.22   32 15.2   2.023   2.045    76   17.1   4:22 (264, 59)  
Sept.28   7  3.83   33 27.8   1.996   2.100    81   17.3   4:28 (264, 64)  

* 328P/LONEOS-Tucker

Now it is 17.0 mag (Sept. 4, ATLAS-MLO, Mauna Loa). It will fade out rapidly after this. 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)  
Sept.21   3 59.20   42 17.7   1.352   1.942   110   17.2   4:00 (180, 83)  
Sept.28   4  5.02   44 10.8   1.316   1.960   114   17.3   3:38 (180, 81)  

* 302P/Lemmon-PanSTARRS

Now it is 17.4 mag (Sept. 6, ATLAS South Africa). It stays 18 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  18 57.07  -22 34.0   2.974   3.376   104   17.2  19:22 (  7, 32)  
Sept.28  19  0.68  -22 37.8   3.064   3.369    98   17.3  19:12 ( 11, 32)  

* 338P/McNaught

Now it is 17.5 mag (Sept. 9, ATLAS-HKO, Haleakala). Fading gradually. 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)  
Sept.21   2 48.19   30  0.6   1.555   2.315   128   17.4   2:49 (  0, 85)  
Sept.28   2 44.96   31 47.9   1.509   2.324   134   17.4   2:18 (  0, 87)  

* 242P/Spahr

Now it is 18.5 mag (Sept. 6, 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)  
Sept.21   4 20.80   -7 46.4   3.494   3.994   112   17.5   4:21 (  0, 47)  
Sept.28   4 21.89   -8 51.9   3.416   3.991   118   17.4   3:54 (  0, 46)  

* C/2022 S4 ( Lemmon )

It has started fading before the perihelion passage. Now it is 17.0 mag (Aug. 11, Thomas Lehmann). It stays 18 mag for a while. In the Northern Hemisphere, it will never be observable after this. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  11 24.71  -64 28.3   3.107   2.840    65   17.4   4:22 (329,-38)  
Sept.28  11 54.66  -63 59.8   3.185   2.858    62   17.5   4:28 (328,-37)  

* 362P/(457175) 2008 GO98

Now it is 16.1 mag (June 5, Toshiyuki Takahashi). It stays 18 mag for a while. It will be unobservable in November 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)  
Sept.21  16  6.14   -7 37.8   3.189   2.886    63   17.4  19:22 ( 58, 27)  
Sept.28  16 15.63   -8 14.8   3.270   2.890    59   17.5  19:12 ( 59, 25)  

* C/2024 L5 ( ATLAS )

Now it is 17.1 mag (Sept. 4, ATLAS Chile). 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 will be getting lower gradually after this, and 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)  
Sept.21  15  3.53  -29 12.8   4.282   3.786    54   17.4  19:22 ( 52,  1)  
Sept.28  15  3.27  -28 57.4   4.362   3.759    47   17.4  19:12 ( 55, -2)  

* 305P/Skiff

It will brighten up to 16 mag and will be observable in good condition in winter. Now it is 18.4 mag (Sept. 10, Michael Jager). Brightening slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  21 26.04   13 51.9   0.661   1.572   140   17.7  21:23 (  0, 69)  
Sept.28  21 27.68   13  2.4   0.650   1.539   136   17.5  20:58 (  0, 68)  

* 48P/Johnson

Now it is 17.1 mag (Sept. 5, ATLAS Chile). Brightening gradually. It will be unobservable in December. It will brighten up to 14.5 mag in 2025 spring. But the condition is bad.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  16 12.39  -16 40.3   2.581   2.361    66   17.6  19:22 ( 50, 21)  
Sept.28  16 23.22  -17 37.8   2.631   2.335    62   17.5  19:12 ( 50, 19)  

* C/2021 X1 ( Maury-Attard )

It brightened up to 14 mag in early 2023 and 2023 autumn. Now it is 17.2 mag (Aug. 27, A. Diepvens). Fading slowly. It will be fainter than 18 mag in October. 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)  
Sept.21  20 32.10   18 27.4   4.764   5.428   127   17.5  20:29 (  0, 73)  
Sept.28  20 26.55   17 36.8   4.890   5.475   121   17.6  19:56 (  0, 73)  

* C/2021 S4 ( Tsuchinshan )

Now it is 17.6 mag (Apr. 11, Mt. Lemmon Survey). 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)  
Sept.21   7 25.96   38 58.7   7.152   6.903    71   17.6   4:22 (250, 53)  
Sept.28   7 29.94   39  6.0   7.061   6.914    77   17.5   4:28 (251, 59)  

* C/2024 J3 ( ATLAS )

Now it is 17.1 mag (Sept. 3, ATLAS Chile). It stays 17 mag for a while. It will be unobservable in December. It is expected to brighten up to 13 mag in 2026, and it will be observable in excellent condition in the Northern Hemisphere. In the Southern Hemisphere, it locates very low at the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21  18 22.07  -37 21.9   7.326   7.500    96   17.6  19:22 ( 13, 16)  
Sept.28  18 22.07  -36 48.6   7.397   7.457    89   17.6  19:12 ( 16, 16)  

* 50P/Arend

Now it is 17.3 mag (Aug. 29, B. Kumar). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.21   8 35.21   35  1.5   2.617   2.242    57   17.6   4:22 (251, 39)  
Sept.28   8 49.37   34 29.9   2.582   2.272    61   17.6   4:28 (253, 43)  

* P/2024 O3 ( LINEAR )

First return of a new periodic comet which brightened up to 15 mag in 2010. Now it is 17.8 mag (Sept. 4, M. Zhang, X. Gao). It stays 18 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)  
Sept.21   7 48.48   31 11.2   2.089   1.902    65   17.7   4:22 (260, 47)  
Sept.28   8  5.24   30 56.4   2.056   1.928    68   17.7   4:28 (262, 50)  

* 117P/Helin-Roman-Alu 1

Now it is 18.6 mag (Aug. 29, D. Buczynski). 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)  
Sept.21   3 38.77   17  2.6   3.830   4.441   121   17.7   3:39 (  0, 72)  
Sept.28   3 37.36   17  1.8   3.756   4.454   128   17.7   3:10 (  0, 72)  

* 276P/Vorobjov

Now it is 17.4 mag (Sept. 7, 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)  
Sept.21   3 14.58   15 34.5   3.220   3.916   127   17.9   3:15 (  0, 71)  
Sept.28   3 13.91   15  8.6   3.142   3.913   134   17.9   2:47 (  0, 70)  

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