Weekly Information about Bright Comets (2024 Oct. 19: South)

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Updated on October 18, 2024
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Best time and the azimuth, altitude (A,h) are at lat. 35 deg in the Southern 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 brightened up to -4.9 mag due to the forward scattering on Oct. 9 in the SOHO coronagraph images (M. Paradowski). It became a great comet of 0 mag on the ground. Now it is 2.6 mag (Oct. 16, Carlos Labordena). It will fade out rapidly after this. It will be unobservable in January in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  16 10.31    2  0.9   0.561   0.675    40    3.5  19:47 ( 97,  6)  
Oct. 26  17 25.12    3 21.0   0.771   0.810    52    4.8  19:55 (103, 13)  

* C/2024 S1 ( ATLAS )

Bright new Kreutz sungrazer comet. It will approach to Sun down to 0.008 a.u. on Oct. 28. It is expected to brighten up to 2 mag, or -4.5 mag at best. Although the brightness evolution almost stopped until mid October, a large outburst occured on Oct. 18 and it brightened up to 10.0 mag (Andrew Pearce). 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 November. In the Southern Hemisphere, it will be unobservable soon. But it will be observable again in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  11 41.11  -18 42.8   0.914   0.485    29    9.3   3:43 (286, 10)  
Oct. 26  13 25.40  -17 16.6   0.893   0.194    10    6.1   3:33 (298, -7)  

* 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 9.2 mag (Oct. 13, Osamu Miyazaki). It will fade out rapidly after this. In the Northern Hemisphere, it will be unobservable in November. But it will be observable again in January. 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. 19  15 19.45   -1 26.1   2.813   1.980    27   10.6  19:47 ( 86, -3)  
Oct. 26  15 33.72   -3 31.1   2.918   2.054    24   11.0  19:55 ( 81, -6)  

* C/2022 E2 ( ATLAS )

Now it is 12.6 mag (Oct. 13, Osamu Miyazaki). 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)  
Oct. 19   7 22.06   56 20.7   3.371   3.680   100   11.9   3:43 (195, -4)  
Oct. 26   7 11.46   58 44.4   3.268   3.685   107   11.9   3:33 (191, -5)  

* 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 11.3 mag (Sept. 23, Jose Guilherme Aguiar). Fading gradually. In the Northern Hemisphere, it is not observable now, but it will appear in February. 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. 19  14 27.71  -47 31.1   3.555   2.852    39   12.3  19:47 ( 42, 15)  
Oct. 26  14 42.40  -47 31.6   3.677   2.933    36   12.5  19:55 ( 39, 12)  

* C/2023 C2 ( ATLAS )

Now it is 13.0 mag (Sept. 20, Taras Prystavski). 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)  
Oct. 19  17 58.18  -32 29.2   2.649   2.390    64   12.9  19:47 ( 77, 45)  
Oct. 26  18 11.01  -30 29.7   2.718   2.381    59   12.9  19:55 ( 77, 39)  

* C/2024 B1 ( Lemmon )

It became much brighter than expected. Now it is 13.8 mag (Sept. 8, Michael Jager). It will fade out rapidly after this. 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 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  13 21.04   45  9.4   1.991   1.641    55   13.4   3:43 (238,-42)  
Oct. 26  13 54.90   42 39.4   2.006   1.652    55   13.5   3:33 (242,-44)  

* 37P/Forbes

Now it is 13.9 mag (Oct. 3, ATLAS South Africa). It will fade out rapidly after this. It will be unobservable in February 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. 19  17 13.76  -26  7.6   1.992   1.620    53   13.9  19:47 ( 80, 33)  
Oct. 26  17 36.43  -25 54.3   2.035   1.624    52   14.0  19:55 ( 78, 31)  

* C/2023 R2 ( PanSTARRS )

It will fade out rapidly after this. It will be fainter than 18 mag in February. In the Northern Hemisphere, it will be unobservable in December. But it will be observable again in January. 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. 19  15  7.00   -1 43.4   2.325   1.474    24   14.0  19:47 ( 84, -5)  
Oct. 26  15 29.49   -2 10.6   2.417   1.561    23   14.4  19:55 ( 82, -8)  

* C/2024 G3 ( ATLAS )

It approaches to Sun down to 0.09 a.u. on Jan. 13. 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 15.6 mag (Sept. 15, ATLAS Chile). 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. But it will be observable again in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  14 30.18  -45 54.5   2.756   2.062    37   14.3  19:47 ( 43, 14)  
Oct. 26  14 41.96  -45  7.8   2.690   1.944    33   14.0  19:55 ( 41, 10)  

* 29P/Schwassmann-Wachmann 1

Now it is 14.6 mag (Sept. 29, Toshiyuki Takahashi). 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. 19   9 58.19   11  9.6   6.709   6.238    57   14.1   3:43 (247, 12)  
Oct. 26  10  1.47   10 46.5   6.610   6.240    64   14.1   3:33 (245, 15)  

* 333P/LINEAR

It is expected to brighten very rapidly up to 10 mag from November to Decemebr. Now it is 18.9 mag (July 7, J. L. Virlichie, P. Traverse, H. Roy). It brightens up to 9.5 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it will be getting higher gradually. 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. 19  10 38.36   -0 38.5   1.737   1.250    45   15.5   3:43 (263, 12)  
Oct. 26  10 45.42    1 47.6   1.561   1.210    50   14.1   3:33 (259, 12)  

* C/2021 G2 ( ATLAS )

Now it is 14.1 mag (Aug. 29, Chris Wyatt). It stays 14 mag for a while. 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. 19  13 48.61  -19  1.2   5.971   4.992     9   14.4  19:47 ( 58,-10)  
Oct. 26  13 55.95  -19  5.5   5.981   4.995     6   14.4   3:33 (304,-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 14.4 mag (Oct. 17, 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 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. 19  22 36.12   -5 29.1   3.823   4.558   132   14.5  20:43 (180, 60)  
Oct. 26  22 35.61   -5 30.3   3.874   4.526   125   14.5  20:15 (180, 60)  

* C/2022 QE78 ( ATLAS )

Now it is 15.3 mag (Oct. 7, Andrew Pearce). 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)  
Oct. 19   6 45.81    2 57.0   5.676   5.976   102   14.6   3:43 (208, 48)  
Oct. 26   6 46.62    2 55.2   5.557   5.956   109   14.6   3:33 (202, 50)  

* 487P/2024 N5 ( Siding Spring )

First return of a new periodic comet which brightened up to 16 mag in 2012. Now it is 15.6 mag (Oct. 9, ATLAS-MLO, Mauna Loa). 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 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. 19   4 46.11   22 21.8   0.985   1.815   132   14.8   2:56 (180, 33)  
Oct. 26   4 41.87   26 43.4   0.938   1.816   139   14.6   2:25 (180, 28)  

* 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 16.0 mag (Oct. 9, ATLAS South Africa). It brightens up to 13.5 mag, but it will turn to fade out rapidly after that. 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 January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19   6 52.85  -21 40.5   1.340   1.752    96   15.1   3:43 (238, 68)  
Oct. 26   6 48.94  -19 40.5   1.221   1.733   102   14.8   3:33 (224, 70)  

* C/2023 Q1 ( PanSTARRS )

Now it is 16.3 mag (Oct. 2, D. Buczynski). 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)  
Oct. 19   7  1.85   64 31.3   2.213   2.617   102   15.4   3:43 (190,-11)  
Oct. 26   7 19.73   66  6.1   2.155   2.605   105   15.3   3:33 (189,-12)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. Now it is 15.2 mag (Oct. 2, ATLAS South Africa). 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)  
Oct. 19  21  6.67  -68 32.4   5.724   5.789    88   15.4  19:47 (  5, 56)  
Oct. 26  21  0.45  -67 47.1   5.866   5.845    83   15.5  19:55 ( 12, 56)  

* C/2021 S3 ( PanSTARRS )

It brightened up to 9.6 mag from February to March (Feb. 25, Thomas Lehmann). Now it is 14.2 mag (Oct. 1, Ken-ichi Kadota). 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)  
Oct. 19  19 50.83   41 39.6   3.184   3.488    99   15.4  19:47 (160,  9)  
Oct. 26  19 58.21   40  3.9   3.296   3.560    97   15.6  19:55 (154,  9)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 15.7 mag (Oct. 9, 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. 19   6 23.90   18 37.3   6.655   7.058   110   15.5   3:43 (195, 35)  
Oct. 26   6 21.87   18 50.7   6.600   7.114   117   15.5   3:33 (189, 36)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.2 mag (Sept. 26, Martin Masek). 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. 19   4 15.67  -69 37.2  15.708  15.839    95   15.5   2:24 (  0, 55)  
Oct. 26   4 12.84  -69 57.2  15.705  15.815    94   15.5   1:54 (  0, 55)  

* C/2022 L2 ( ATLAS )

Now it is 15.6 mag (July 24, Thomas Lehmann). It stays 16 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. 19   9 52.74  -32 21.5   3.974   3.513    55   15.7   3:43 (287, 37)  
Oct. 26   9 50.09  -33 40.4   3.935   3.557    60   15.7   3:33 (287, 41)  

* 130P/McNaught-Hughes

Now it is 15.5 mag (Oct. 7, A. Pearce). 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. 19   2 20.62    7  7.0   1.392   2.376   168   15.7   0:31 (180, 48)  
Oct. 26   2 13.98    6 52.4   1.419   2.409   173   15.9  23:52 (180, 48)  

* 30P/Reinmuth 1

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

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  11 40.92    6  3.5   2.660   1.900    32   15.7   3:43 (266, -5)  
Oct. 26  11 56.80    4 40.6   2.640   1.920    35   15.8   3:33 (267, -4)  

* P/2023 S1

Now it is 15.9 mag (Sept. 30, Ken-ichi Kadota). 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)  
Oct. 19   8 37.99   23 39.3   2.718   2.728    80   15.9   3:43 (224, 17)  
Oct. 26   8 46.37   23  3.9   2.618   2.717    84   15.8   3:33 (222, 19)  

* 472P/2023 RL75 ( NEAT-LINEAR )

Now it is 15.8 mag (Oct. 9, 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. 19   6 37.81   12 45.4   3.044   3.455   106   15.8   3:43 (201, 40)  
Oct. 26   6 40.19   12 14.7   2.964   3.465   112   15.8   3:33 (196, 41)  

* C/2024 A1 ( ATLAS )

Now it is 16.9 mag (Oct. 9, ATLAS South Africa). 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)  
Oct. 19   8 16.33  -26 31.9   4.511   4.387    76   16.2   3:43 (268, 54)  
Oct. 26   8 16.82  -26 41.3   4.399   4.360    81   16.1   3:33 (265, 58)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.5 mag (Oct. 9, Ken-ichi Kadota). 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)  
Oct. 19   7  8.90  -28 25.6   6.799   6.889    91   16.2   3:43 (259, 69)  
Oct. 26   7  9.90  -28 53.9   6.715   6.875    95   16.2   3:33 (256, 72)  

* 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 17 mag for a while. In the Northern Hemisphere, it will never be observable after this. 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. 19  12  3.70  -49 22.5   9.595   8.903    43   16.3   3:43 (316, 21)  
Oct. 26  12  8.36  -49 55.3   9.634   8.947    44   16.3   3:33 (316, 24)  

* C/2023 H5 ( Lemmon )

It will be observable at 15 mag for a long time in 2025 in the Northern Hemisphere. Brightening slowly. 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. 19  11 37.04   24 29.7   5.444   4.791    44   16.4   3:43 (250,-14)  
Oct. 26  11 42.58   25  6.6   5.335   4.767    50   16.3   3:33 (248,-12)  

* C/2019 U5 ( PanSTARRS )

Now it is 15.9 mag (Oct. 10, 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)  
Oct. 19   7 49.93  -43 59.9   6.146   6.062    80   16.5   3:43 (299, 62)  
Oct. 26   7 46.36  -45  8.7   6.130   6.106    83   16.5   3:33 (304, 66)  

* C/2023 T3 ( Fuls )

Brightening slowly. It locates somewhat low in the Northern Hemisphere. 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. 19  11 18.33  -19  4.6   4.438   3.659    34   16.6   3:43 (284, 14)  
Oct. 26  11 27.78  -20 12.0   4.379   3.644    37   16.5   3:33 (284, 16)  

* 43P/Wolf-Harrington

Now it is 16.5 mag (Oct. 9, 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)  
Oct. 19   2  8.85   20 23.1   2.168   3.146   166   16.6   0:20 (180, 34)  
Oct. 26   2  4.03   19 45.1   2.131   3.119   172   16.6  23:43 (180, 35)  

* 154P/Brewington

It brightened up to 12.0 mag in June (June 13, Ken-ichi Kadota). Now it is 16.1 mag (Oct. 1, Toshiyuki Takahashi). Fading slowly. It will be fainter than 18 mag in February. 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. 19   9  6.71   33 11.4   2.066   2.082    77   16.6   3:43 (222,  6)  
Oct. 26   9 16.95   32 45.0   2.035   2.129    81   16.7   3:33 (222,  7)  

* 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 16.8 mag (Oct. 4, ATLAS South Africa). 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)  
Oct. 19   6 58.24  -39 54.4   5.620   5.719    90   16.6   3:43 (293, 73)  
Oct. 26   6 55.71  -40 23.4   5.609   5.767    94   16.6   3:33 (298, 76)  

* 305P/Skiff

It will brighten up to 16 mag and will be observable in good condition in winter. Now it is 17.3 mag (Oct. 9, ATLAS South Africa). 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. 19  21 48.66    9 57.6   0.647   1.461   124   16.9  19:56 (180, 45)  
Oct. 26  22  1.17    8 58.6   0.654   1.443   120   16.7  19:55 (175, 46)  

* C/2022 U3 ( Bok )

Now it is 18.9 mag (Sept. 30, Yasukazu Ikari). 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. 19   8  5.30    9 12.3   4.866   4.870    84   16.7   3:43 (227, 33)  
Oct. 26   8  7.85    8 19.1   4.768   4.877    90   16.7   3:33 (224, 36)  

* C/2023 R1 ( PanSTARRS )

Now it is 16.8 mag (Oct. 9, 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 December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  22 40.02   26 57.8   5.129   5.879   135   16.7  20:46 (180, 28)  
Oct. 26  22 33.75   25 56.0   5.154   5.835   129   16.7  20:13 (180, 29)  

* 253P/PanSTARRS

Now it is 16.0 mag (Oct. 9, ATLAS South Africa). 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. 19   0 41.74   -3 24.2   1.059   2.027   161   16.7  22:48 (180, 58)  
Oct. 26   0 39.32   -3 46.2   1.087   2.027   153   16.8  22:18 (180, 59)  

* 146P/Shoemaker-LINEAR

It brightened up to 14.4 mag in summer (Aug. 17, Hiroshi Abe). Now it is 16.9 mag (Sept. 30, Hiroshi Abe). 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. 19   6 18.87   28  3.6   1.004   1.653   111   16.7   3:43 (191, 26)  
Oct. 26   6 22.71   30 45.4   0.986   1.694   117   16.9   3:33 (188, 24)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 17.0 mag (Oct. 5, ATLAS Chile). 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)  
Oct. 19   1 48.56  -69 35.8  10.245  10.471   100   16.8  23:54 (  0, 56)  
Oct. 26   1 39.13  -69 23.7  10.291  10.477    98   16.8  23:17 (  0, 56)  

* 299P/Catalina-PanSTARRS

It brightened very rapidly in outburst in late May, and brightened up to 14.9 mag (May 19, Taras Prystavski). Now it is 17.2 mag (Oct. 3, ATLAS Chile). It stays 17 mag for a while. 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. 19  16 55.74  -23  5.2   3.833   3.274    49   16.9  19:47 ( 80, 28)  
Oct. 26  17  5.84  -23  7.1   3.913   3.284    44   17.0  19:55 ( 77, 23)  

* 48P/Johnson

Now it is 16.9 mag (Oct. 11, 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)  
Oct. 19  17  0.17  -20 13.0   2.764   2.261    50   17.1  19:47 ( 84, 28)  
Oct. 26  17 13.85  -20 57.0   2.801   2.237    46   16.9  19:55 ( 80, 24)  

* 190P/Mueller

Now it is 17.5 mag (Sept. 23, A. Diepvens). Fading slowly. 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. 19  22 37.40   -7 11.6   1.295   2.100   132   17.0  20:45 (180, 62)  
Oct. 26  22 39.37   -6 53.7   1.338   2.084   126   17.0  20:19 (180, 62)  

* C/2022 U1 ( Leonard )

Now it is 16.5 mag (Oct. 1, A. Diepvens). It stays 18 mag for a while. 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 unobservable in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  19  6.02   26 23.4   4.468   4.542    87   17.1  19:47 (144, 19)  
Oct. 26  19  5.22   24 37.3   4.585   4.565    82   17.2  19:55 (136, 15)  

* P/2010 A3 ( Hill )

First return of a new periodic comet which brightened up to 15 mag in 2010. It is expected to brighten up to 15 mag from winter to spring, and it will be observable in excellent condition in the Northern Hemisphere. But actually, it is fainter than this ephemeris. Now it is 19.3 mag (Oct. 8, John Maikner). Brightening gradually. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19   3  2.23    4 38.3   1.301   2.255   157   17.4   1:13 (180, 50)  
Oct. 26   2 57.29    4 51.6   1.232   2.206   164   17.1   0:40 (180, 50)  

* 49P/Arend-Rigaux

It will brighten up to 14 mag in 2025 spring. Now it is 17.3 mag (Oct. 13, Ken-ichi Kadota). Brightening slowly. 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. 19  23 43.04  -30 53.6   1.491   2.273   131   17.1  21:50 (180, 86)  
Oct. 26  23 38.68  -30 56.6   1.504   2.225   124   17.2  21:18 (180, 86)  

* 242P/Spahr

Now it is 17.6 mag (Oct. 9, ATLAS South Africa). 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. 19   4 20.31  -12 10.8   3.231   3.983   133   17.2   2:30 (180, 67)  
Oct. 26   4 18.25  -13 12.9   3.189   3.981   137   17.2   2:01 (180, 68)  

* C/2023 TD22 ( Lemmon )

Brightened rapidly. Now it is 16.2 mag (Sept. 28, A. Diepvens). Fading slowly. 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)  
Oct. 19  19 47.08  -13 38.3   2.158   2.384    90   17.2  19:47 (123, 57)  
Oct. 26  19 38.70  -14 13.1   2.334   2.396    81   17.4  19:55 (111, 49)  

* 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 16.7 mag (Oct. 9, ATLAS-MLO, Mauna Loa). It stays 18 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 soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  17 29.37   25 42.7   8.246   7.912    67   17.3  19:47 (127,  5)  
Oct. 26  17 32.98   25 18.3   8.343   7.953    63   17.3  19:55 (121,  0)  

* 302P/Lemmon-PanSTARRS

Now it is 17.0 mag (Oct. 4, ATLAS South Africa). It stays 18 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. 19  19 16.53  -22 35.7   3.343   3.350    81   17.4  19:47 (102, 57)  
Oct. 26  19 23.26  -22 30.1   3.435   3.344    76   17.4  19:55 ( 97, 51)  

* C/2024 J2 ( Wierzchos )

Now it is 17.5 mag (Oct. 9, D. Buczynski). Brightening slowly. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it is not observable now. It will brighten up to 15.5 mag from winter to spring. But it is not observable around the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19  15 31.69   38 19.0   3.028   2.594    55   17.5  19:47 (122,-22)  
Oct. 26  15 47.70   37 48.6   2.956   2.537    55   17.4  19:55 (120,-25)  

* 492P/2024 O3 ( LINEAR )

First return of a new periodic comet which brightened up to 15 mag in 2010. Now it is 17.4 mag (Oct. 13, Ken-ichi Kadota). 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. 19   8 49.17   30  1.3   1.950   2.021    79   17.5   3:43 (222, 10)  
Oct. 26   9  1.48   29 44.0   1.913   2.056    83   17.4   3:33 (221, 11)  

* 338P/McNaught

Now it is 17.2 mag (Oct. 9, ATLAS-MLO, Mauna Loa). Fading gradually. 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. 19   2 25.20   36 17.3   1.432   2.355   151   17.4   0:36 (180, 19)  
Oct. 26   2 16.23   37 20.1   1.429   2.367   154   17.5  23:55 (180, 17)  

* C/2021 S4 ( Tsuchinshan )

Now it is 17.6 mag (Oct. 13, Ken-ichi Kadota). 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)  
Oct. 19   7 38.96   39 36.0   6.780   6.949    95   17.5   3:43 (204, 10)  
Oct. 26   7 40.90   39 48.5   6.688   6.962   101   17.5   3:33 (201, 11)  

* 89P/Russell 2

Now it is 17.0 mag (Oct. 10, 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)  
Oct. 19  23 10.14  -18 38.5   1.865   2.657   134   17.5  21:17 (180, 73)  
Oct. 26  23  9.19  -17 50.6   1.956   2.682   127   17.7  20:49 (180, 73)  

* C/2024 J3 ( ATLAS )

Now it is 17.5 mag (Oct. 2, ATLAS Chile). It stays 17 mag for a while. It will be unobservable in December. But it will be observable again in January in the Southern Hemisphere, or in February in the Northern Hemisphere. 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)  
Oct. 19  18 25.23  -35 11.4   7.608   7.327    69   17.6  19:47 ( 75, 51)  
Oct. 26  18 27.23  -34 40.3   7.672   7.284    63   17.5  19:55 ( 73, 44)  

* (3200) Phaethon

Parent asteroid of Geminids meteor shower. Now it is 18.5 mag (Sept. 12, ATLAS-HKO, Haleakala). Brightening slowly. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 19   5 19.40   38 32.7   1.449   2.156   122   17.9   3:30 (180, 16)  
Oct. 26   5 11.02   39  3.7   1.334   2.120   130   17.6   2:54 (180, 16)  

* 117P/Helin-Roman-Alu 1

Now it is 17.0 mag (Sept. 14, Ken-ichi Kadota). 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. 19   3 28.78   16 46.9   3.591   4.492   151   17.7   1:39 (180, 38)  
Oct. 26   3 24.74   16 38.5   3.560   4.505   159   17.7   1:08 (180, 38)  

* 50P/Arend

Now it is 18.5 mag (Oct. 10, D. Buczynski). 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)  
Oct. 19   9 26.26   32 58.8   2.457   2.369    73   17.7   3:43 (226,  3)  
Oct. 26   9 36.58   32 33.0   2.410   2.402    77   17.7   3:33 (225,  4)  

* (308607) 2005 WY3

Peculiar asteroid moving along a cometary orbit. 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. 19   4  3.77   -5 53.7   2.212   3.042   139   17.9   2:14 (180, 61)  
Oct. 26   4  1.41   -7 28.4   2.128   2.992   144   17.7   1:44 (180, 62)  

* 328P/LONEOS-Tucker

Now it is 17.8 mag (Oct. 10, Yasukazu Ikari). It will fade out rapidly after this. It will be fainter than 18 mag soon. 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. 19   4  9.70   48 59.8   1.239   2.024   129   17.7   2:20 (180,  6)  
Oct. 26   4  6.59   50 10.8   1.226   2.049   134   17.9   1:50 (180,  5)  

* 276P/Vorobjov

Now it is 17.3 mag (Oct. 4, Mt. Lemmon Survey). 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. 19   3  7.45   13 30.6   2.969   3.906   157   17.8   1:18 (180, 41)  
Oct. 26   3  4.13   12 53.2   2.936   3.904   164   17.8   0:47 (180, 42)  

* 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)  
Oct. 19  13  8.82  -62  7.3   3.419   2.920    52   17.8   3:43 (333, 21)  
Oct. 26  13 29.04  -61 28.5   3.492   2.944    49   17.9   3:33 (333, 20)  

* (343158) Marsyas

Peculiar asteroid moving along a cometary orbit. It will approach to Sun down to 0.49 a.u. on Nov. 29. It brightens up to 17 mag, but it will turn to fade out rapidly after that. It locates somewhat low in the Northern Hemisphere. 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. 19  10  4.46    2 50.8   1.113   0.964    54   18.2   3:43 (254, 16)  
Oct. 26  10 24.56   -3 37.3   0.873   0.861    54   17.8   3:33 (260, 20)  

* C/2021 X1 ( Maury-Attard )

It brightened up to 14 mag in early 2023 and 2023 autumn. Now it is 17.9 mag (Sept. 6, Ken-ichi Kadota). Fading slowly. It will be fainter than 18 mag soon. 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. 19  20 15.31   15 14.6   5.321   5.615   102   17.9  19:47 (155, 36)  
Oct. 26  20 13.21   14 33.3   5.475   5.661    95   18.0  19:55 (144, 33)  

* 192P/Shoemaker-Levy 1

It brightened up to 15.9 mag in summer (July 8, Hidetaka Sato). Now it is 17.8 mag (Sept. 12, ATLAS-HKO, Haleakala). It will fade out rapidly after this. 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. 19   7 28.04   37 21.6   1.912   2.268    97   17.9   3:43 (203, 13)  
Oct. 26   7 33.12   38 47.1   1.885   2.325   103   18.1   3:33 (200, 13)  

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