Weekly Information about Bright Comets (2024 Sept. 14: North)

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Updated on September 16, 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. The brightness evolution slowed down since May. But it brightened up to 8.2 mag in mid August (Aug. 12, Thomas Lehmann). Now it is 4.6 mag (Sept. 15, Michael Mattiazzo). It brightens up to 2 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 October. In the Southern Hemisphere, it will be unobservable in early October. But it will be observable again in mid October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  10 36.57   -5  9.3   1.433   0.536    15    4.8   4:47 (272, -7)  
Sept.21  10 35.45   -5 55.5   1.191   0.432    20    3.6   4:52 (277,  0)  

* 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. 11, Osamu Miyazaki). 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 in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  13 56.52   12 19.5   2.299   1.625    37    9.2  19:33 ( 93, 17)  
Sept.21  14 15.09    9  6.6   2.395   1.693    36    9.5  19:22 ( 90, 16)  

* 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.14  13  0.77  -47 31.9   2.871   2.435    54   11.1  19:33 ( 48,-26)  
Sept.21  13 20.33  -47 32.7   3.013   2.521    51   11.3  19:22 ( 48,-26)  

* 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.14   7 37.50   46 40.1   3.962   3.666    65   12.2   4:16 (237, 46)  
Sept.21   7 37.60   48 15.4   3.843   3.667    72   12.2   4:22 (234, 52)  

* C/2023 R2 ( PanSTARRS )

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

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  12 51.85    1 41.8   1.955   1.078    20   12.3  19:33 ( 93, -2)  
Sept.21  13 22.08    0 54.5   2.012   1.147    22   12.6  19:22 ( 91,  0)  

* C/2023 C2 ( ATLAS )

Now it is 13.1 mag (Aug. 29, Chris Wyatt). It stays 13 mag for a while. It stays extremely low in the Northern Hemisphere. But it will become high in spring. 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.14  16 54.74  -43 17.8   2.325   2.473    86   12.8  19:33 ( 24,  6)  
Sept.21  17  7.19  -40 59.7   2.384   2.452    81   12.8  19:22 ( 25,  8)  

* C/2024 B1 ( Lemmon )

It became much brighter than expected. Now it is 13.8 mag (Sept. 8, Michael Jager). Fading slowly. 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.14  10  2.48   49 24.3   2.133   1.664    49   13.7   4:16 (225, 24)  
Sept.21  10 41.94   49 51.9   2.076   1.649    51   13.6   4:22 (225, 23)  

* 37P/Forbes

Now it is 13.8 mag (Aug. 31, Chris Wyatt). 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.14  15 25.58  -24 43.6   1.808   1.640    64   13.9  19:33 ( 49, 11)  
Sept.21  15 46.09  -25 17.3   1.841   1.630    61   13.8  19:22 ( 48, 11)  

* 29P/Schwassmann-Wachmann 1

Now it is 16.3 mag (Sept. 8, 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.14   9 37.69   13 19.6   7.091   6.230    29   14.2   4:16 (261, 10)  
Sept.21   9 42.24   12 52.3   7.032   6.232    34   14.2   4:22 (265, 15)  

* 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.14  13 12.40  -18 49.5   5.785   4.983    33   14.3  19:33 ( 74,-10)  
Sept.21  13 19.49  -18 49.4   5.839   4.983    28   14.3  19:22 ( 75,-12)  

* 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.14  22 46.49   -4 45.5   3.731   4.723   169   14.6  23:11 (  0, 50)  
Sept.21  22 43.68   -4 57.4   3.724   4.689   162   14.6  22:41 (  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.14  19 23.65   50 52.2   2.711   3.126   104   14.6  19:48 (180, 74)  
Sept.21  19 27.36   48 56.2   2.794   3.199   104   14.8  19:25 (180, 76)  

* 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). Fading rapidly. 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.14  14 10.71   19 53.1   2.588   1.974    42   14.7  19:33 ( 98, 24)  
Sept.21  14 23.61   16 48.2   2.713   2.054    40   15.1  19:22 ( 96, 21)  

* C/2022 QE78 ( ATLAS )

Now it is 15.7 mag (Sept. 1, Hiroshi Abe). 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.14   6 34.45    3 17.2   6.293   6.080    73   15.0   4:16 (300, 40)  
Sept.21   6 37.60    3 12.9   6.172   6.059    78   14.9   4:22 (308, 45)  

* 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.14  22 14.27  -70 51.2   5.061   5.510   111   14.9  22:38 (  0,-16)  
Sept.21  21 55.97  -70 44.0   5.182   5.566   107   15.0  21:53 (  0,-16)  

* 154P/Brewington

Now it is 14.2 mag (Sept. 1, Thomas Lehmann). 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.14   7 55.58   35 46.1   2.175   1.861    58   15.2   4:16 (250, 41)  
Sept.21   8 12.37   35 16.7   2.160   1.903    61   15.6   4:22 (252, 44)  

* 130P/McNaught-Hughes

Now it is 14.2 mag (Sept. 1, Hiroshi Abe). Fading gradually. 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.14   2 42.68    8 15.0   1.431   2.217   130   15.2   3:11 (  0, 63)  
Sept.21   2 40.83    8  7.2   1.405   2.248   137   15.3   2:41 (  0, 63)  

* 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 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.14  13 38.99  -50 50.7   2.942   2.608    61   15.5  19:33 ( 42,-22)  
Sept.21  13 48.23  -49 39.9   2.921   2.503    56   15.3  19:22 ( 44,-22)  

* 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.14   6 26.19   17 39.4   6.967   6.780    75   15.4   4:16 (286, 51)  
Sept.21   6 26.75   17 49.9   6.906   6.836    81   15.4   4:22 (294, 57)  

* 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.14   5 30.41   15 52.7   1.127   1.491    88   15.5   4:16 (304, 60)  
Sept.21   5 43.20   18 10.7   1.101   1.517    92   15.7   4:22 (308, 65)  

* 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.14   4 22.18  -67 26.2  15.763  15.959    99   15.5   4:16 (357,-13)  
Sept.21   4 21.95  -67 55.3  15.745  15.935    99   15.5   4:21 (  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.14  10 16.17   13  0.4   2.741   1.830    20   15.6   4:16 (256,  2)  
Sept.21  10 33.80   11 39.6   2.727   1.840    22   15.6   4:22 (259,  4)  

* 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.14   9 55.05  -26 44.1   4.041   3.302    37   15.6   4:16 (292,-16)  
Sept.21   9 55.66  -27 42.4   4.048   3.343    40   15.7   4:22 (297,-11)  

* 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). Brightening 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.14   4 33.96    6 16.2   1.346   1.854   103   16.0   4:16 (337, 59)  
Sept.21   4 39.72    8 47.2   1.262   1.840   108   15.7   4:22 (350, 63)  

* 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.14   5 34.27   55 46.9   2.580   2.708    86   15.9   4:16 (213, 62)  
Sept.21   5 51.05   57 36.6   2.497   2.686    89   15.8   4:22 (207, 63)  

* 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.14   6 42.18  -27 25.4   1.891   1.903    75   16.2   4:16 (321, 15)  
Sept.21   6 47.28  -26 32.4   1.790   1.866    78   16.0   4:22 (326, 20)  

* 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.14   6 13.37   15 10.0   3.477   3.416    78   16.2   4:16 (292, 52)  
Sept.21   6 19.75   14 43.8   3.389   3.423    83   16.1   4:22 (300, 57)  

* C/2019 U5 ( PanSTARRS )

Now it is 15.5 mag (Sept. 5, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it will be unobservable soon. 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.14   7 55.98  -38 25.7   6.209   5.844    64   16.3   4:16 (316, -3)  
Sept.21   7 56.11  -39 28.3   6.202   5.887    67   16.3   4:22 (322,  1)  

* 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 stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  21 27.65   -6 19.9   1.432   2.357   149   16.3  21:50 (  0, 49)  
Sept.21  20 57.78   -8 37.2   1.533   2.357   135   16.5  20:53 (  0, 46)  

* 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.14   7 47.63   26 29.6   3.199   2.791    57   16.4   4:16 (262, 39)  
Sept.21   7 58.63   25 58.1   3.108   2.777    61   16.3   4:22 (266, 43)  

* 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.14   6 56.82  -26  3.1   7.211   6.963    71   16.4   4:16 (317, 14)  
Sept.21   7  0.10  -26 29.9   7.132   6.948    75   16.4   4:22 (323, 18)  

* 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.14  16 10.12  -22 43.6   3.371   3.232    73   16.4  19:33 ( 43, 19)  
Sept.21  16 18.44  -22 48.2   3.469   3.240    68   16.5  19:22 ( 44, 17)  

* 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.14   6 59.42  -37 18.3   5.664   5.477    74   16.5   4:16 (324,  5)  
Sept.21   7  0.63  -37 47.9   5.660   5.525    77   16.5   4:22 (329,  8)  

* 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.14   8  4.00  -25 54.7   4.995   4.533    57   16.6   4:16 (306,  4)  
Sept.21   8  7.57  -25 58.5   4.911   4.503    60   16.5   4:22 (311,  9)  

* 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 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.14  13 25.34  -39 26.5   5.881   5.300    50   16.6  19:33 ( 54,-18)  
Sept.21  13 26.71  -39 18.0   5.946   5.290    45   16.6  19:22 ( 56,-21)  

* 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.14  23 31.00  -20 39.9   1.559   2.537   162   16.7  23:55 (  0, 34)  
Sept.21  23 25.21  -20 34.2   1.598   2.560   159   16.8  23:22 (  0, 35)  

* 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.14   2 33.31  -69  1.3  10.091  10.440   107   16.7   3:01 (  0,-14)  
Sept.21   2 25.43  -69 19.6  10.110  10.446   106   16.7   2:25 (  0,-14)  

* 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.14   0 57.18    0  9.6   1.081   2.047   157   16.8   1:25 (  0, 55)  
Sept.21   0 55.00   -0 36.2   1.055   2.040   164   16.8   0:56 (  0, 55)  

* 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.14  19 26.47   36 49.6   3.980   4.441   111   16.8  19:51 (180, 88)  
Sept.21  19 19.72   34 36.8   4.058   4.460   107   16.8  19:22 ( 68, 89)  

* 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.14   7 44.67   13 29.5   5.330   4.841    56   16.9   4:16 (277, 33)  
Sept.21   7 49.73   12 40.0   5.244   4.845    61   16.9   4:22 (282, 38)  

* 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.14  23 18.79   31  2.3   5.245   6.101   145   17.0  23:43 (  0, 86)  
Sept.21  23 10.52   30 26.3   5.188   6.056   147   16.9  23:07 (  0, 86)  

* 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.14   6 41.55   31  3.4   2.047   1.992    72   16.9   4:16 (264, 54)  
Sept.21   6 53.22   32 15.2   2.023   2.045    76   17.1   4:22 (264, 59)  

* 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 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.14  17 15.96   28 17.0   7.716   7.706    85   16.9  19:33 ( 82, 65)  
Sept.21  17 17.92   27 43.0   7.826   7.747    81   17.0  19:22 ( 84, 62)  

* 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.14   0 13.81  -26 12.1   1.564   2.510   154   17.1   0:42 (  0, 29)  
Sept.21   0  7.89  -27 37.5   1.527   2.463   152   17.1   0:09 (  0, 28)  

* 2020 TS2

It approached to Sun down to 0.12 a.u. on Aug. 4. Fading rapidly. 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.14   3 17.59  -62 34.6   0.266   1.115   107   17.1   3:52 (  0, -7)  
Sept.21   0 35.24  -57 13.9   0.368   1.243   122   18.3   0:40 (  0, -3)  

* 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.14   3 51.67   40 19.1   1.391   1.926   105   17.1   4:16 (187, 85)  
Sept.21   3 59.20   42 17.7   1.352   1.942   110   17.2   4:00 (180, 83)  

* 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.14   2 23.43   21 55.6   2.543   3.283   130   17.3   2:51 (  0, 77)  
Sept.21   2 22.27   21 50.8   2.447   3.256   137   17.1   2:23 (  0, 77)  

* 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.14  22 48.02   -6 52.6   1.203   2.200   169   17.2  23:12 (  0, 48)  
Sept.21  22 43.81   -7  7.5   1.201   2.177   161   17.2  22:41 (  0, 48)  

* 302P/Lemmon-PanSTARRS

Now it is 17.4 mag (Sept. 6, ATLAS South Africa). It stays 17 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in summer. 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.14  18 54.39  -22 28.1   2.886   3.383   111   17.2  19:33 (  4, 32)  
Sept.21  18 57.07  -22 34.0   2.974   3.376   104   17.2  19:22 (  7, 32)  

* C/2022 S4 ( Lemmon )

It has started fading before the perihelion passage. Now it is 17.0 mag (Aug. 11, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag in November. 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.14  10 52.04  -64 46.7   3.033   2.824    68   17.3   4:16 (329,-38)  
Sept.21  11 24.71  -64 28.3   3.107   2.840    65   17.4   4:22 (329,-38)  

* 338P/McNaught

Now it is 17.5 mag (Sept. 9, ATLAS-HKO, Haleakala). Fading slowly. It will be fainter than 18 mag in November. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14   2 49.63   28  9.3   1.609   2.308   122   17.4   3:18 (  0, 83)  
Sept.21   2 48.19   30  0.6   1.555   2.315   128   17.4   2:49 (  0, 85)  

* 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.14  15 57.08   -6 59.1   3.105   2.882    67   17.4  19:33 ( 56, 29)  
Sept.21  16  6.14   -7 37.8   3.189   2.886    63   17.4  19:22 ( 58, 27)  

* 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.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  20 38.55   19 17.6   4.650   5.382   132   17.4  21:03 (  0, 74)  
Sept.21  20 32.10   18 27.4   4.764   5.428   127   17.5  20:29 (  0, 73)  

* C/2024 L5 ( ATLAS )

Now it is 17.1 mag (Sept. 4, ATLAS Chile). It stays 17 mag for a while. It will be unobservable soon in the Northern Hemisphere, or in November in the Southern Hemisphere. But it will be observable again in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14  15  4.45  -29 32.6   4.193   3.814    61   17.4  19:33 ( 50,  4)  
Sept.21  15  3.53  -29 12.8   4.282   3.786    54   17.4  19:22 ( 52,  1)  

* 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.14   4 18.93   -6 43.3   3.578   3.998   107   17.5   4:16 (349, 48)  
Sept.21   4 20.80   -7 46.4   3.494   3.994   112   17.5   4:21 (  0, 47)  

* C/2021 S4 ( Tsuchinshan )

Now it is 17.6 mag (Apr. 11, Mt. Lemmon Survey). 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.14   7 21.56   38 52.5   7.239   6.891    66   17.6   4:16 (248, 48)  
Sept.21   7 25.96   38 58.7   7.152   6.903    71   17.6   4:22 (250, 53)  

* 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 is not observable now, but it will appear in October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.14   8 20.19   35 32.0   2.650   2.212    53   17.6   4:16 (248, 36)  
Sept.21   8 35.21   35  1.5   2.617   2.242    57   17.6   4:22 (251, 39)  

* 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.14  18 22.64  -37 55.4   7.256   7.543   102   17.6  19:33 (  9, 16)  
Sept.21  18 22.07  -37 21.9   7.326   7.500    96   17.6  19:22 ( 13, 16)  

* 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.14  16  2.37  -15 40.8   2.529   2.388    70   17.7  19:33 ( 49, 23)  
Sept.21  16 12.39  -16 40.3   2.581   2.361    66   17.6  19:22 ( 50, 21)  

* 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.14  21 26.66   14 28.2   0.678   1.609   144   17.9  21:51 (  0, 70)  
Sept.21  21 26.04   13 51.9   0.661   1.572   140   17.7  21:23 (  0, 69)  

* 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.14   7 30.82   31 21.8   2.122   1.877    62   17.8   4:16 (258, 44)  
Sept.21   7 48.48   31 11.2   2.089   1.902    65   17.7   4:22 (260, 47)  

* 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.14   3 39.41   17  1.2   3.911   4.427   114   17.8   4:07 (  0, 72)  
Sept.21   3 38.77   17  2.6   3.830   4.441   121   17.7   3:39 (  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.14   3 14.43   15 56.4   3.307   3.919   120   18.0   3:42 (  0, 71)  
Sept.21   3 14.58   15 34.5   3.220   3.916   127   17.9   3:15 (  0, 71)  

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