Weekly Information about Bright Comets (2023 Oct. 14: North)

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Updated on October 14, 2023
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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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* 2P/Encke

Now it is 8.2 mag (Oct. 12, Virgilio Gonano). It will fade out rapidly after this. It will be fainter than 18 mag in January. It will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  11 58.02    3 23.2   1.086   0.408    22    7.7   4:40 (269,  4)  
Oct. 21  12 50.53   -5 15.0   1.222   0.342    13    7.5   4:46 (273, -5)  

* 103P/Hartley 2

Now it is 8.3 mag (Oct. 12, Virgilio Gonano). It will fade out rapidly after this. 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. 14   7 34.68   19 47.5   0.410   1.064    87    7.5   4:40 (303, 66)  
Oct. 21   7 59.45   13 59.0   0.431   1.071    87    7.5   4:46 (315, 63)  

* C/2023 P1 ( Nishimura )

It approached to Sun down to 0.23 a.u. and brightened up to 2.5 mag in mid September (Sept. 18, Juan Jose Gonzalez). Fading rapidly. It will be fainter than 18 mag in January. Now it is not observable. It will appear soon 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)  
Oct. 14  12 56.12  -23 23.6   1.716   0.807    16    9.2   4:40 (284,-23)  
Oct. 21  12 55.78  -26 52.0   1.841   0.962    19   10.2   4:46 (291,-18)  

* C/2023 H2 ( Lemmon )

It brightened very rapidly. It will approach to Earth down to 0.2 a.u. in November, and it is expected to brighten up to 7.5 mag. Now it is 10.8 mag (Oct. 7, Bob King). It will turn to fade out rapidly after brightening. In the Northern Hemisphere, it will be unobservable in January. But it will be observable again in October. 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. 14  12 20.03   46 53.1   0.994   0.936    56   10.7   4:40 (228, 23)  
Oct. 21  12 40.10   48 17.3   0.770   0.907    60   10.0   4:46 (228, 26)  

* C/2020 V2 ( ZTF )

Now it is 9.8 mag (Oct. 10, Juan Jose Gonzalez). Fading gradually. In the Northern Hemisphere, it will be unobservable in January. 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. 14   0 57.06  -37 46.1   2.067   2.854   134   10.1  23:24 (  0, 17)  
Oct. 21   0 37.26  -39 57.5   2.185   2.902   127   10.3  22:37 (  0, 15)  

* C/2021 S3 ( PanSTARRS )

It is expected to brighten up to 7 mag in early 2024. Now it is 12.3 mag (Sept. 16, Jose G. S. Aguiar). It will brighten rapidly after this. In the Northern Hemisphere, it is not observable now, but it will appear in November. It locates somewhat low in the Southern Hemisphere. But it will become high in winter. The brightness evolution slowed down since May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  10 35.54  -34 28.5   2.781   2.193    45   10.6   4:40 (311, -3)  
Oct. 21  10 54.39  -35 34.1   2.701   2.121    45   10.4   4:46 (313, -2)  

* 12P/Pons-Brooks

It returns for the first time in 70 years. It will brighten up to 4.5 mag in 2024 spring. It suddenly brightened in outburst by 5 mag up to 11.5 mag on July 20 (E. Tamas, Francois Kugel). It brightened again in another outburst up to 11.7 mag on Oct. 5 (Richard Miles). Now it is 11.8 mag (Oct. 11, Osamu Miyazaki). It will brighten rapidly after this. 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. 14  17 26.27   44 36.2   3.019   2.960    77   11.4  18:51 (119, 56)  
Oct. 21  17 31.47   43 27.6   2.968   2.879    75   11.4  18:43 (118, 53)  

* (3200) Phaethon

It will fade out rapidly after this. It will be fainter than 18 mag in January. Now it is not observable. It will appear in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  12 15.16   -6  5.2   1.122   0.298    14   14.0   4:40 (274, -5)  
Oct. 21  13 50.68  -12 56.1   1.119   0.140     3   11.5  18:43 ( 85,-16)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 12.5 mag (Oct. 13, Osamu Miyazaki). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   6 47.57   -8 17.7   3.684   3.906    95   12.1   4:40 (346, 46)  
Oct. 21   6 44.77   -8 15.9   3.641   3.969   101   12.1   4:46 (359, 47)  

* C/2021 T4 ( Lemmon )

It brightened up to 7.8 mag in late July (July 20, Thomas Lehmann). Now it is 12.9 mag (Oct. 3, Chris Wyatt). Fading slowly. In the Northern Hemisphere, it is not observable now, but it will appear in November. In the Southern Hemisphere, it will be unobservable in December. But it will be observable again in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  14 56.56  -12 14.1   2.655   1.807    25   12.2  18:51 ( 75,  0)  
Oct. 21  14 58.82  -11 42.0   2.773   1.862    19   12.4  18:43 ( 78, -3)  

* C/2023 S2 ( ATLAS )

Now it is 12.6 mag (Oct. 3, Chris Wyatt). It will fade out rapidly after this. In the Northern Hemisphere, it will be getting higher gradually. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  16 55.81   -5 44.4   1.257   1.067    55   12.8  18:51 ( 60, 27)  
Oct. 21  17 27.71   -5 29.2   1.227   1.071    56   12.7  18:43 ( 58, 30)  

* C/2019 U5 ( PanSTARRS )

Now it is 13.7 mag (July 14, Chris Wyatt). It stays 13 mag for a while. It stays extremely 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. 14  10 45.25  -23 44.2   4.762   4.035    39   13.2   4:40 (301,  2)  
Oct. 21  10 46.02  -25 14.6   4.722   4.063    43   13.2   4:46 (307,  6)  

* C/2023 E1 ( ATLAS )

It brightened up to 8.4 mag in late July (July 22, Thomas Lehmann). Now it is 12.0 mag (Oct. 6, Osamu Miyazaki). Fading rapidly. 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. 14  22 34.61  -23 50.4   1.104   1.904   129   13.3  21:05 (  0, 31)  
Oct. 21  22 40.86  -24 48.0   1.249   1.985   123   13.8  20:43 (  0, 30)  

* 62P/Tsuchinshan 1

It is expected to brighten up to 7 mag, and it will be observable in good condition in winter. Now it is 14.4 mag (Oct. 2, Ken-ichi Kadota). Brightening rapidly. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   6 44.49   21 56.9   0.992   1.522    99   14.6   4:40 (326, 75)  
Oct. 21   7  8.01   21 56.8   0.917   1.479   101   13.5   4:46 (334, 76)  

* C/2019 L3 ( ATLAS )

It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 13.2 mag (July 14, 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 getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  10 57.49  -38 40.2   7.207   6.519    43   13.8   4:40 (311,-10)  
Oct. 21  11  2.26  -39 35.8   7.223   6.564    45   13.8   4:46 (315, -6)  

* C/2022 A2 ( PanSTARRS )

It brightened up to 9.5 mag from last winter to early spring (Jan. 30, Katsumi Yoshimoto). Now it is 13.0 mag (Oct. 6, Osamu Miyazaki). It will fade out rapidly after this. 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. 14  22 47.14   -2 41.5   2.511   3.352   141   13.8  21:16 (  0, 52)  
Oct. 21  22 41.69   -4 55.0   2.660   3.417   132   14.1  20:43 (  0, 50)  

* 29P/Schwassmann-Wachmann 1

Now it is 12.2 mag (Sept. 23, Toshiyuki Takahashi). 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. 14   8 35.50   21 11.0   6.340   6.144    74   13.9   4:40 (283, 55)  
Oct. 21   8 38.16   20 59.7   6.231   6.146    80   13.9   4:46 (291, 61)  

* C/2021 X1 ( Maury-Attard )

Now it is 13.8 mag (Oct. 3, Chris Wyatt). Fading gradually. 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. 14  23 51.38    5 10.2   2.544   3.495   159   14.0  22:19 (  0, 60)  
Oct. 21  23 35.61    4 37.7   2.632   3.520   148   14.1  21:36 (  0, 60)  

* C/2020 K1 ( PanSTARRS )

Now it is 14.3 mag (Oct. 3, Chris Wyatt). 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. It was expected to brighten up to 10 mag from spring to summer. However, it was fainter than originally expected.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  11 58.17  -76 44.7   3.652   3.435    69   14.0   4:40 (344,-33)  
Oct. 21  12  1.48  -77 39.0   3.705   3.465    68   14.1   4:46 (346,-32)  

* C/2022 JK5 ( PanSTARRS )

The ATLAS search program detected its cometary activity in April. It continues to be brightening even after the perihelion passage. Now it is 13.9 mag (Oct. 3, Chris Wyatt). 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. 14  23 33.01  -25 44.8   2.354   3.170   138   14.0  22:02 (  0, 29)  
Oct. 21  23 31.51  -24 58.4   2.446   3.206   132   14.3  21:33 (  0, 30)  

* C/2022 E2 ( ATLAS )

Now it is 14.5 mag (Oct. 2, Ken-ichi Kadota). Brightening slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting higher gradually. It is expected to brighten up to 12 mag from 2024 to 2025.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   9 41.18    4 36.6   5.213   4.705    54   14.2   4:40 (289, 32)  
Oct. 21   9 42.38    4 51.9   5.067   4.668    61   14.1   4:46 (295, 38)  

* 126P/IRAS

It brightened up to 13.6 mag in summer (July 16, Mitsunori Tsumura). Now it is 14.5 mag (Sept. 26, Thomas Lehmann). It will fade out rapidly after this. 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 never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   1 22.34   68 48.6   1.342   2.023   119   14.4  23:49 (180, 56)  
Oct. 21   0 51.85   70 10.2   1.379   2.062   119   14.6  22:51 (180, 55)  

* C/2022 L2 ( ATLAS )

Now it is 14.9 mag (Sept. 18, Ken-ichi Kadota). Brightening slowly. In the Northern Hemisphere, it will be unobservable in November. But it will be observable again in December. In the Southern Hemisphere, it is not observable now, but it will appear in December. It is expected to brighten up to 12.5 mag in 2024 spring. At the high light, it will be observable in excellent condition in the Southern Hemisphere, but it will be low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  15  9.55   -3 20.4   3.944   3.110    29   14.7  18:51 ( 80,  8)  
Oct. 21  15 11.08   -4 41.1   3.965   3.075    23   14.7  18:43 ( 82,  4)  

* 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 14.0 mag (Sept. 22, S. Shurpakov). It stays 15 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 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  15 55.08   16 26.8   6.451   5.811    46   14.7  18:51 ( 91, 28)  
Oct. 21  16  0.63   16 11.4   6.527   5.848    43   14.7  18:43 ( 92, 25)  

* C/2021 G2 ( ATLAS )

Now it is 15.2 mag (July 22, ATLAS Chile). It stays 15 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 getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  11  8.34  -30 20.8   6.351   5.587    37   15.0   4:40 (303, -6)  
Oct. 21  11 14.98  -30 54.8   6.296   5.563    39   14.9   4:46 (307, -2)  

* C/2023 A3 ( Tsuchinshan-ATLAS )

It will approach to Sun down to 0.4 a.u. in late September in 2024, and it is expected to brighten up to 0 mag. Now it is 15.3 mag (Sept. 10, A. Ivanov et al.). Brightening gradually. Now it is not observable. It will appear in November in the Northern Hemisphere, or in December in the Southern Hemisphere. At the high light, in the Northern Hemisphere, it will be observable in good condition after the perihelion passage. In the Southern Hemisphere, it will be observable in the low sky before and after the perihelion passage.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  14 20.11   -2 49.4   6.045   5.100    17   15.5  18:51 ( 88, -2)  
Oct. 21  14 23.48   -3 18.9   5.993   5.028    12   15.4  18:43 ( 90, -5)  

* C/2021 Y1 ( ATLAS )

Now it is 14.3 mag (July 7, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in January. 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. 14  13 18.55  -49 23.4   3.479   2.812    41   15.5  18:51 ( 50,-35)  
Oct. 21  13 36.59  -49 20.7   3.571   2.866    38   15.5   4:46 (310,-34)  

* 213P/Van Ness

It has not been observed yet in this apparition. It was expected to brighten rapidly up to 15 mag in summer. But actually, it is not detected, fainter than 19 mag (Aug. 12, Martin Masek). Fading slowly. It locates somewhat 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)  
Oct. 14  18 27.00  -24 24.4   1.981   1.993    76   15.5  18:51 ( 28, 25)  
Oct. 21  18 41.69  -23 39.6   2.045   1.987    72   15.5  18:43 ( 30, 25)  

* 32P/Comas Sola

It is expected to brighten up to 14.5 mag in winter. Now it is 16.5 mag (Oct. 6, ATLAS-HKO, Haleakala). 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)  
Oct. 14   3 30.37   15 30.4   1.713   2.599   145   15.6   2:03 (  0, 71)  
Oct. 21   3 27.41   15 42.6   1.635   2.564   153   15.5   1:33 (  0, 71)  

* 471P/2023 KF3

David Rankin detected its cometary activity in June. Now it is 15.7 mag (Sept. 24, Ken-ichi Kadota). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  22  5.97   -4 16.8   1.422   2.214   131   15.6  20:36 (  0, 51)  
Oct. 21  22  8.37   -4 12.4   1.465   2.196   125   15.6  20:11 (  0, 51)  

* 199P/Shoemaker 4

Now it is 14.6 mag (Aug. 5, J. L. Virlichie, P. Traverse, H. Roy, G. Houdin). Fading slowly. It will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  18 39.93  -34 27.6   2.981   2.950    78   15.6  18:51 ( 21, 17)  
Oct. 21  18 49.78  -34 34.2   3.078   2.958    73   15.7  18:43 ( 23, 16)  

* C/2022 E3 ( ZTF )

It approached to Earth down to 0.29 a.u. in early February, and it brightened up to 4.5 mag (Feb. 1, Juan Jose Gonzalez). Now it is 16.1 mag (Oct. 4, ATLAS Chile). Fading slowly. 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)  
Oct. 14   6 23.25  -53  1.4   3.684   3.838    91   15.7   4:40 (358,  2)  
Oct. 21   6 14.45  -55 15.0   3.726   3.911    93   15.8   4:19 (  0,  0)  

* C/2022 S4 ( Lemmon )

It is expected to brighten up to 14 mag in 2024 summer. At the high light, it is not observable in the Northern Hemisphere. Now it is 16.5 mag (Oct. 6, Jean-Claude Merlin). It stays 16 mag for a while. 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. 14   3 10.52  -12 23.1   3.062   3.919   144   15.9   1:43 (  0, 43)  
Oct. 21   3  3.45  -14 47.9   2.996   3.873   147   15.8   1:09 (  0, 40)  

* 237P/LINEAR

It brightened up to 11.8 mag in summer (June 17, Osamu Miyazaki). Now it is 14.9 mag (Sept. 28, Ken-ichi Kadota). 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. 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. 14  20  3.44   -2 57.1   1.893   2.313   101   15.8  18:51 (  7, 52)  
Oct. 21  20 12.15   -3  7.3   1.995   2.340    97   16.1  18:43 ( 11, 51)  

* C/2023 K1 ( ATLAS )

It brightened very rapidly. Now it is 15.2 mag (Aug. 23, ATLAS South Africa). It will fade out rapidly after this. It will be fainter than 18 mag in December. Now it is not observable. It will appear in November in the Northern Hemisphere. 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. 14  14 22.57  -16 51.2   3.004   2.085    18   15.8  18:51 ( 76, -9)  
Oct. 21  14 27.10  -15 39.3   3.065   2.104    12   16.1  18:43 ( 79,-11)  

* 144P/Kushida

It is expected to brighten up to 8.5 mag from January to February. Now it is 19.1 mag (Sept. 26, P. Carson). Brightening rapidly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   3  2.31   21 21.4   0.876   1.813   150   16.4   1:35 (  0, 76)  
Oct. 21   3  2.47   21  9.8   0.806   1.767   157   15.9   1:08 (  0, 76)  

* 226P/Pigott-LINEAR-Kowalski

It is expected to brighten up to 15 mag from autumn to winter. Now it is 16.6 mag (Oct. 4, ATLAS Chile). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will be observable 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)  
Oct. 14   1 48.97  -56 56.2   1.255   1.903   114   16.2   0:23 (  0, -2)  
Oct. 21   1 31.03  -54 51.3   1.233   1.881   114   16.0  23:31 (  0,  0)  

* 117P/Helin-Roman-Alu 1

Now it is 15.8 mag (Oct. 5, ATLAS Chile). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   0 16.43   -8 28.3   2.764   3.709   158   16.0  22:45 (  0, 47)  
Oct. 21   0 12.53   -8 35.7   2.822   3.725   151   16.1  22:14 (  0, 47)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 16.4 mag (Sept. 28, ATLAS Chile). It stays 16 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. 14   3 26.12  -65  3.5  16.874  17.128   103   16.1   1:58 (  0,-10)  
Oct. 21   3 23.57  -65 21.1  16.871  17.103   101   16.1   1:28 (  0,-10)  

* C/2022 A3 ( Lemmon-ATLAS )

Now it is 16.5 mag (Apr. 10, Michael Jager). It stays 16 mag for a while. In the Northern Hemisphere, it will be unobservable in November. 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. 14   9 36.52  -38 49.1   4.142   3.706    57   16.3   4:40 (322,  2)  
Oct. 21   9 39.03  -41 22.5   4.088   3.709    60   16.2   4:46 (328,  3)  

* C/2020 Y2 ( ATLAS )

It brightened up to 14.1 mag in 2022 spring (Mar. 22, 2022, Chris Wyatt). Now it is 16.3 mag (Oct. 6, Jean-Claude Merlin). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   2 17.47   -2 38.5   4.454   5.407   161   16.4   0:51 (  0, 52)  
Oct. 21   2 10.14   -2 35.1   4.487   5.455   165   16.4   0:16 (  0, 53)  

* 71P/Clark

It brightened up to 12.8 mag in spring (Mar. 8, Taras Prystavski). Now it is 16.1 mag (Sept. 13, Ken-ichi Kadota). 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. 14   0 52.34   -5 58.9   1.736   2.712   165   16.5  23:21 (  0, 49)  
Oct. 21   0 46.09   -6  7.3   1.798   2.749   158   16.7  22:47 (  0, 49)  

* 81P/Wild 2

Now it is 16.2 mag (Sept. 13, ATLAS South Africa). Fading slowly. It will be fainter than 18 mag in December. It locates somewhat low in the Northern Hemisphere. 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. 14  17 59.28  -22  0.2   3.212   3.016    69   16.7  18:51 ( 36, 24)  
Oct. 21  18  8.29  -22  4.8   3.340   3.054    64   16.9  18:43 ( 38, 23)  

* C/2022 W3 ( Leonard )

Now it is 16.7 mag (Sept. 5, Thomas Lehmann). It will fade out rapidly after this. It will be fainter than 18 mag in November. It locates somewhat low in the Northern Hemisphere. 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. 14  18 56.52  -30 30.3   1.992   2.105    82   16.7  18:51 ( 19, 22)  
Oct. 21  19  1.31  -32 24.4   2.182   2.173    76   17.1  18:43 ( 22, 19)  

* P/2023 M4 ( ATLAS )

Now it is 16.6 mag (Sept. 18, Ken-ichi Kadota). Fading slowly. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually. It was very faint as 21.5 mag in 2021. It seems to be bright temporarily in outburst.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  21  6.62  -12  0.4   4.074   4.591   115   16.7  19:37 (  0, 43)  
Oct. 21  21  7.53  -11 57.3   4.188   4.605   108   16.8  19:10 (  0, 43)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 16.7 mag (Sept. 15, J. L. Virlichie, P. Traverse, H. Roy). 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. 14   5 16.75  -75 50.3  10.280  10.314    89   16.8   3:47 (  0,-21)  
Oct. 21   5  5.32  -76 22.7  10.296  10.314    88   16.8   3:09 (  0,-21)  

* C/2021 S4 ( Tsuchinshan )

Now it is 17.2 mag (Sept. 26, ATLAS-HKO, Haleakala). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   5  2.38   40 20.1   6.156   6.710   119   16.8   3:35 (180, 85)  
Oct. 21   5  1.89   40 39.4   6.068   6.706   126   16.8   3:07 (180, 84)  

* C/2022 N2 ( PanSTARRS )

It is expected to brighten up to 11.5 mag in 2025 autumn, and it will be observable in good condition. Now it is 17.0 mag (Sept. 22, ATLAS South Africa). It stays 17 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)  
Oct. 14  20 32.51  -19 26.3   6.309   6.646   105   16.8  19:03 (  0, 36)  
Oct. 21  20 33.19  -19 20.6   6.378   6.603    98   16.8  18:43 (  2, 36)  

* C/2022 QE78 ( ATLAS )

Now it is 16.6 mag (Sept. 27, 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)  
Oct. 14   4 58.76  -11 46.9   6.846   7.407   120   16.9   3:31 (  0, 43)  
Oct. 21   4 57.88  -12  3.9   6.745   7.375   126   16.8   3:03 (  0, 43)  

* 219P/LINEAR

Now it is 17.2 mag (Oct. 3, ATLAS South Africa). It stays 17 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January in the Northern Hemisphere, or in December in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  18 29.07  -12 30.1   2.509   2.490    77   16.8  18:51 ( 34, 36)  
Oct. 21  18 38.97  -12 34.5   2.577   2.475    72   16.9  18:43 ( 36, 35)  

* C/2022 V2 ( Lemmon )

Now it is 17.7 mag (July 12, A. Diepvens). 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. 14  11 48.42   16 40.1   2.848   2.075    32   16.9   4:40 (259, 13)  
Oct. 21  11 50.82   14 12.5   2.780   2.068    36   16.9   4:46 (265, 18)  

* 170P/Christensen

Now it is 17.0 mag (Sept. 28, A. Diepvens). Fading slowly. It will be fainter than 18 mag in January. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   3 57.25    6 19.7   2.253   3.080   139   17.0   2:30 (  0, 61)  
Oct. 21   3 54.73    5 50.7   2.213   3.092   146   17.0   2:00 (  0, 61)  

* 2019 AV4

The cometary activity was detected by Masayoshi Yoshimi on Sept. 15. Now it is 16.0 mag (Sept. 15, Masayoshi Yoshimi). 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. In the Southern Hemisphere, it will be unobservable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  21 18.58   45 21.1   0.243   1.129   117   17.0  19:48 (180, 79)  
Oct. 21  21 25.09   51 45.5   0.261   1.128   114   17.2  19:28 (180, 73)  

* 77P/Longmore

It brightened up to 13.8 mag in spring (Apr. 26, Thomas Lehmann). Now it is 16.3 mag (Sept. 22, ATLAS South Africa). 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)  
Oct. 14  16 12.43  -40 50.5   3.165   2.660    51   17.1  18:51 ( 42, -5)  
Oct. 21  16 27.96  -41 12.0   3.243   2.680    47   17.3  18:43 ( 42, -6)  

* C/2023 F3 ( ATLAS )

Now it is 17.7 mag (Sept. 14, Jean-Claude Merlin). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in January. 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. It stays 16 mag in the Southern sky for a long time from 2024 to 2025.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  16 23.92  -39 32.0   6.841   6.289    52   17.2  18:51 ( 41, -2)  
Oct. 21  16 24.98  -39 34.1   6.902   6.261    46   17.2  18:43 ( 44, -5)  

* C/2022 U3 ( Bok )

Now it is 17.6 mag (Sept. 26, ATLAS-HKO, Haleakala). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   5 10.16   38 58.3   4.768   5.321   118   17.3   3:43 (180, 86)  
Oct. 21   5  9.80   38 49.9   4.658   5.299   125   17.2   3:15 (180, 86)  

* C/2022 U1 ( Leonard )

Now it is 17.5 mag (Sept. 28, Ken-ichi Kadota). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will appear in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   0 36.59   58  6.4   3.720   4.419   129   17.3  23:04 (180, 67)  
Oct. 21   0 15.06   57 20.6   3.692   4.402   130   17.3  22:15 (180, 68)  

* C/2022 R6 ( PanSTARRS )

Now it is 17.6 mag (Sept. 27, 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. 14   5 16.25  -38 36.1   7.614   7.966   107   17.4   3:48 (  0, 16)  
Oct. 21   5 15.71  -39  9.7   7.551   7.941   109   17.4   3:20 (  0, 16)  

* C/2020 R7 ( ATLAS )

It brightened up to 13.4 mag in last summer (July 7, 2022, Giuseppe Pappa). Now it is 17.4 mag (Sept. 7, Thomas Lehmann). It stays 18 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14  15 32.56   29 11.6   5.342   4.760    49   17.4  18:51 (106, 30)  
Oct. 21  15 36.13   29  7.9   5.411   4.808    48   17.5  18:43 (108, 27)  

* 465P/2023 L1 ( Hill )

First return of a new periodic comet which brightened up to 15 mag in 2008. Now it is 18.8 mag (Sept. 23, A. Diepvens). 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. 14   4  8.32   13 49.9   1.880   2.696   136   17.7   2:41 (  0, 69)  
Oct. 21   4  6.18   12 22.8   1.855   2.725   144   17.8   2:11 (  0, 68)  

* 207P/NEAT

Now it is 18.7 mag (Oct. 3, Catalina Sky Survey). It will brighten rapidly after this. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   0 32.01    4 44.2   0.801   1.791   169   18.0  23:01 (  0, 60)  
Oct. 21   0 22.68    2 29.8   0.752   1.720   159   17.7  22:24 (  0, 57)  

* 246P/NEAT

It brightened up to 14 mag from 2020 to 2021. Now it is 17.9 mag (Aug. 24, W. Hasubick). 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. 14   2 57.96    3 14.5   3.849   4.764   153   17.9   1:31 (  0, 58)  
Oct. 21   2 53.99    2 59.0   3.826   4.775   160   17.9   0:59 (  0, 58)  

* C/2021 A9 ( PanSTARRS )

Now it is 18.9 mag (Sept. 25, W. Hasubick). 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. 14   7 43.28   10 58.6   7.800   7.766    84   18.0   4:40 (312, 58)  
Oct. 21   7 41.44   10 43.8   7.672   7.764    91   17.9   4:46 (327, 62)  

* 13P/Olbers

It returned for the first time in 68 years. It will brighten up to 7.5 mag in 2024 summer. Now it is 19.8 mag (Sept. 27, J. Nicolas, F. Kugel). It will brighten rapidly after this. It stays observable in good condition. At the high light, it locates low in the Northern Hemisphere, or it is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Oct. 14   4 23.81  -19 26.3   2.843   3.522   125   18.8   2:56 (  0, 36)  
Oct. 21   4 20.08  -20  5.0   2.725   3.453   130   18.5   2:25 (  0, 35)  

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