Weekly Information about Bright Comets (2023 Nov. 18: North)

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Updated on November 22, 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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* C/2023 H2 ( Lemmon )

Now it is 7.4 mag (Nov. 18, Osamu Miyazaki). It will fade out rapidly after this. 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)  
Nov. 18  20 59.69  -21 52.2   0.319   0.963    76    8.4  18:20 ( 17, 30)  
Nov. 25  21 52.86  -33 33.9   0.538   1.016    77    9.7  18:18 (  9, 21)  

* 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 9.6 mag (Nov. 20, Osamu Miyazaki). It will turn to fade out rapidly after brightening. In the Northern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   8 52.20   20 12.9   0.682   1.340   105    9.6   5:06 (  0, 75)  
Nov. 25   9 19.79   19 19.1   0.641   1.315   105    8.8   5:06 (  0, 74)  

* 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). Brightening gradually. It stays extremely low in the Northern Hemisphere. But it will become high in winter. 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)  
Nov. 18  12 17.54  -39  8.4   2.384   1.842    46    9.5   5:09 (323,  2)  
Nov. 25  12 40.32  -39 40.0   2.305   1.776    46    9.3   5:14 (325,  3)  

* 103P/Hartley 2

It approached to Earth down to 0.38 a.u., and brightened up to 8.0 mag in autumn (Sept. 29, Virgilio Gonano). Now it is 10.4 mag (Nov. 19, Osamu Miyazaki). It will fade out rapidly after this. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   8 56.04   -3 42.3   0.528   1.176    96   10.0   5:09 (359, 51)  
Nov. 25   9  1.95   -6 47.1   0.549   1.218   101   10.4   4:48 (  0, 48)  

* 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). Another outburst occured on Nov. 14 (Nick James). Now it is 9.4 mag (Nov. 20, Osamu Miyazaki). It will brighten rapidly after this. In the Northern Hemisphere, it will be getting lower gradually. In the Southern Hemisphere, it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  18  4.34   39 46.3   2.732   2.548    68   11.2  18:20 (115, 42)  
Nov. 25  18 15.52   39  7.4   2.664   2.463    67   11.1  18:18 (115, 39)  

* C/2020 V2 ( ZTF )

Now it is 10.3 mag (Nov. 3, Hiroshi Abe). 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)  
Nov. 18  23 39.37  -43  6.1   2.800   3.101    98   11.2  19:51 (  0, 12)  
Nov. 25  23 31.07  -43  3.3   2.970   3.153    91   11.4  19:15 (  0, 12)  

* 2P/Encke

It brightened up to 8.1 mag in autumn (Oct. 10, Juan Jose Gonzalez). Fading rapidly. 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)  
Nov. 18  16 11.96  -25 54.8   1.664   0.725    11   11.2  18:20 ( 67,-13)  
Nov. 25  16 51.51  -27 25.2   1.777   0.850    13   12.4  18:18 ( 64,-12)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 11.5 mag (Nov. 20, Osamu Miyazaki). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   6 24.48   -7 28.6   3.521   4.221   129   12.3   2:39 (  0, 47)  
Nov. 25   6 17.50   -7  2.4   3.515   4.284   136   12.3   2:05 (  0, 48)  

* 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. Now it is not observable. It will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  15  8.55   -9 46.9   3.067   2.104    10   13.2   5:09 (276, -9)  
Nov. 25  15 10.78   -9 16.2   3.097   2.168    16   13.3   5:14 (280, -2)  

* C/2019 U5 ( PanSTARRS )

Now it is 13.7 mag (Nov. 15, Hiroshi Abe). It stays 14 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)  
Nov. 18  10 43.11  -31 45.1   4.498   4.179    65   13.2   5:09 (336, 18)  
Nov. 25  10 40.32  -33 27.8   4.431   4.210    70   13.2   5:14 (344, 19)  

* C/2023 S2 ( ATLAS )

It brightened up to 12.6 mag in autumn (Oct. 3, Chris Wyatt). Now it is 13.7 mag (Nov. 2, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in March. 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)  
Nov. 18  19 48.51   -2 58.0   1.220   1.201    64   13.2  18:20 ( 48, 40)  
Nov. 25  20 23.86   -1 59.2   1.257   1.256    66   13.5  18:18 ( 46, 43)  

* C/2022 E2 ( ATLAS )

Now it is 13.9 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). Brightening slowly. It stays observable in good condition. 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)  
Nov. 18   9 41.33    6 32.6   4.422   4.526    89   13.6   5:09 (337, 59)  
Nov. 25   9 39.17    7 11.8   4.256   4.491    97   13.5   5:14 (354, 62)  

* 144P/Kushida

It is expected to brighten up to 8.5 mag from January to February. Now it is 15.4 mag (Nov. 12, Toshihiko Ikemura, Hirohisa Sato). Brightening rapidly. It stays observable in good condition. It is fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   2 52.62   18 36.3   0.618   1.602   170   14.0  23:04 (  0, 74)  
Nov. 25   2 49.78   17 39.4   0.594   1.565   163   13.6  22:33 (  0, 73)  

* 29P/Schwassmann-Wachmann 1

Now it is 12.6 mag (Nov. 13, Taras Prystavski). In the Northern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   8 43.84   20 31.5   5.790   6.154   107   13.7   4:58 (  0, 75)  
Nov. 25   8 43.90   20 29.2   5.685   6.156   114   13.7   4:31 (  0, 75)  

* 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). Now it is 11.1 mag (Nov. 7, Hidetaka Sato). Fading rapidly. It will be fainter than 18 mag in January. In the Northern Hemisphere, it is not observable now, but it will be observable soon. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  12 52.73  -37 55.6   2.145   1.513    39   13.7   5:09 (317, -2)  
Nov. 25  12 50.32  -40 26.0   2.183   1.637    44   14.3   5:14 (324,  1)  

* 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. 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)  
Nov. 18  11 18.30  -43 30.4   7.221   6.745    57   14.0   5:09 (335,  5)  
Nov. 25  11 21.34  -44 30.6   7.207   6.790    61   14.0   5:14 (340,  6)  

* C/2020 K1 ( PanSTARRS )

Now it is 14.8 mag (Oct. 28, ATLAS Chile). Fading slowly. 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)  
Nov. 18  11 50.34  -82 40.0   3.866   3.595    66   14.4   5:09 (354,-30)  
Nov. 25  11 30.05  -84  8.8   3.895   3.630    67   14.4   5:14 (357,-30)  

* C/2022 L2 ( ATLAS )

Now it is 14.9 mag (Sept. 18, Ken-ichi Kadota). Brightening slowly. Now it is not observable. 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)  
Nov. 18  15 19.58   -9 47.7   3.918   2.948     9   14.5   5:09 (275,-11)  
Nov. 25  15 21.94  -11  2.1   3.872   2.919    13   14.4   5:14 (280, -5)  

* C/2021 X1 ( Maury-Attard )

Now it is 14.7 mag (Nov. 1, Ken-ichi Kadota). Fading slowly. It will be getting lower gradually after this, and it will be unobservable in January in the Southern Hemisphere, or in February in the Northern Hemisphere. But it will be observable again in March in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  22 51.11    3 11.2   3.172   3.631   110   14.6  19:03 (  0, 58)  
Nov. 25  22 44.49    3  3.3   3.335   3.661   101   14.8  18:29 (  0, 58)  

* C/2021 G2 ( ATLAS )

Now it is 15.1 mag (Nov. 17, ATLAS Chile). It stays 14 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)  
Nov. 18  11 39.61  -33 21.8   6.009   5.473    53   14.8   5:09 (326, 11)  
Nov. 25  11 45.12  -33 59.8   5.920   5.451    57   14.7   5:14 (331, 14)  

* 32P/Comas Sola

Now it is 14.2 mag (Nov. 15, Ken-ichi Kadota). It stays 15 mag for a while. In the Northern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   3  5.81   16 25.3   1.446   2.431   173   14.9  23:17 (  0, 72)  
Nov. 25   2 59.52   16 37.1   1.431   2.399   165   14.8  22:43 (  0, 72)  

* 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 14.2 mag (Nov. 3, Toshiyuki Takahashi). 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 be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  23 34.15  -20 59.8   2.897   3.360   109   14.9  19:46 (  0, 34)  
Nov. 25  23 36.83  -19 51.8   3.025   3.401   103   15.1  19:21 (  0, 35)  

* 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.). It will brighten rapidly after this. 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. 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)  
Nov. 18  14 38.30   -5  9.7   5.656   4.732    18   15.0   5:09 (277,  0)  
Nov. 25  14 42.17   -5 34.8   5.540   4.656    24   14.9   5:14 (281,  6)  

* 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 14.3 mag (Nov. 3, Hiroshi Abe). It stays 15 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  16 24.15   15 40.4   6.756   5.997    37   15.0  18:20 (101, 12)  
Nov. 25  16 30.20   15 41.3   6.793   6.034    37   15.0  18:18 (103,  8)  

* C/2022 A2 ( PanSTARRS )

It brightened up to 9.5 mag from last winter to early spring (Jan. 30, Katsumi Yoshimoto). Now it is 14.9 mag (Nov. 13, Ken-ichi Kadota). Fading gradually. It will be fainter than 18 mag in March. 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)  
Nov. 18  22 32.65  -10 53.6   3.361   3.675   100   15.1  18:45 (  0, 44)  
Nov. 25  22 33.02  -11 48.1   3.549   3.740    93   15.3  18:18 (  0, 43)  

* 226P/Pigott-LINEAR-Kowalski

Now it is 15.9 mag (Nov. 17, ATLAS Chile). Fading slowly. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   0 43.39  -39 51.3   1.225   1.812   109   15.4  20:55 (  0, 16)  
Nov. 25   0 38.90  -35  0.3   1.247   1.799   106   15.3  20:23 (  0, 20)  

* 126P/IRAS

It brightened up to 13.6 mag in summer (July 16, Mitsunori Tsumura). Now it is 14.9 mag (Nov. 6, 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)  
Nov. 18  23 23.19   69  2.1   1.594   2.232   117   15.4  19:34 (180, 56)  
Nov. 25  23 16.47   68  2.6   1.662   2.277   116   15.7  19:00 (180, 57)  

* 471P/2023 KF3

David Rankin detected its cometary activity in June. Now it is 15.7 mag (Nov. 13, Toshihiko Ikemura, Hirohisa Sato). Fading slowly. 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)  
Nov. 18  22 31.48   -2 47.2   1.688   2.145   103   15.6  18:44 (  0, 52)  
Nov. 25  22 40.15   -2  8.6   1.753   2.137    98   15.6  18:25 (  0, 53)  

* 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 18 mag (Oct. 14, Martin Masek). Fading slowly. It will be unobservable in January in the Southern Hemisphere, or in February in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  19 43.57  -19 58.2   2.296   1.981    59   15.7  18:20 ( 38, 25)  
Nov. 25  19 59.43  -18 51.0   2.358   1.983    56   15.8  18:18 ( 40, 25)  

* C/2023 E1 ( ATLAS )

It brightened up to 8.4 mag in late July (July 22, Thomas Lehmann). Now it is 18.4 mag (Nov. 15, Toshihiko Ikemura, Hirohisa Sato). Fading rapidly. It will be fainter than 18 mag in January. 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)  
Nov. 18  23  8.97  -25  4.4   1.879   2.306   102   15.8  19:21 (  0, 30)  
Nov. 25  23 16.63  -24 37.6   2.045   2.386    97   16.3  19:01 (  0, 31)  

* 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 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)  
Nov. 18  14 39.73  -49  0.6   3.885   3.088    31   15.9   5:09 (315,-24)  
Nov. 25  14 53.44  -48 54.6   3.946   3.145    31   16.0   5:14 (316,-21)  

* (3200) Phaethon

Fading gradually. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  18 52.35   -0 29.0   0.794   0.811    52   16.0  18:20 ( 63, 33)  
Nov. 25  19 48.96    2 49.8   0.859   0.940    60   16.2  18:18 ( 59, 41)  

* 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 (Nov. 13, ATLAS South Africa). 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)  
Nov. 18   3 11.45  -66  1.6  16.892  17.004    94   16.1  23:22 (  0,-11)  
Nov. 25   3  8.30  -66  3.7  16.903  16.980    92   16.0  22:51 (  0,-11)  

* 199P/Shoemaker 4

Now it is 17.3 mag (Nov. 11, ATLAS Chile). Fading slowly. It will be unobservable in January. But it will be observable again in March in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  19 34.44  -34 21.7   3.444   3.001    55   16.1  18:20 ( 32, 12)  
Nov. 25  19 46.55  -34  8.6   3.528   3.013    51   16.2  18:18 ( 34, 11)  

* C/2022 S4 ( Lemmon )

Now it is 16.2 mag (Nov. 15, Toshihiko Ikemura, Hirohisa Sato). It stays 16 mag for a while. In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in March. In the Southern Hemisphere, it stays observable in good condition. The brightness evolution is slower than originally expected.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   2 28.95  -23 27.9   2.926   3.691   134   16.2  22:39 (  0, 31)  
Nov. 25   2 20.06  -25  7.5   2.953   3.647   128   16.1  22:03 (  0, 30)  

* C/2022 A3 ( Lemmon-ATLAS )

Now it is 16.8 mag (Nov. 11, ATLAS South Africa). It stays 16 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)  
Nov. 18   9 40.28  -52 29.9   3.887   3.730    73   16.2   5:09 (353,  2)  
Nov. 25   9 37.17  -55 24.4   3.846   3.738    76   16.2   5:14 (359,  0)  

* 237P/LINEAR

It brightened up to 11.8 mag in summer (June 17, Osamu Miyazaki). Now it is 16.5 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). It will fade out rapidly after this. It will be fainter than 18 mag in January. In the Northern Hemisphere, it will be getting lower gradually. 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)  
Nov. 18  20 51.88   -2 52.9   2.423   2.451    79   16.2  18:20 ( 29, 48)  
Nov. 25  21  2.64   -2 35.7   2.533   2.480    75   16.4  18:18 ( 34, 47)  

* 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 (Nov. 15, ATLAS Chile). Fading slowly. It will be fainter than 18 mag in March. 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)  
Nov. 18   5 17.50  -61 42.4   3.970   4.199    96   16.2   1:32 (  0, -7)  
Nov. 25   4 59.13  -62 28.9   4.050   4.270    96   16.3   0:46 (  0, -7)  

* C/2023 S3 ( Lemmon )

Now it is 16.3 mag (Nov. 17, ATLAS Chile). Fading slowly. It will be unobservable in January. But it will be observable again in February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   0 48.23  -31 22.9   0.617   1.377   116   16.3  20:54 (  0, 23)  
Nov. 25  23 38.86  -36 45.4   0.733   1.289    95   16.4  19:20 (  0, 18)  

* 207P/NEAT

It will approach to Earth down to 0.2 a.u. from February to March, and it is expected to brighten up to 13 mag. Now it is 18.1 mag (Nov. 13, Toshihiko Ikemura, Hirohisa Sato). 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)  
Nov. 18  23 54.06   -6 38.8   0.653   1.437   120   16.6  20:06 (  0, 48)  
Nov. 25  23 52.12   -8 27.9   0.641   1.367   112   16.4  19:36 (  0, 47)  

* 117P/Helin-Roman-Alu 1

Now it is 15.4 mag (Nov. 13, ATLAS Chile). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   0  3.82   -8  6.9   3.167   3.787   122   16.5  20:16 (  0, 47)  
Nov. 25   0  3.66   -7 45.9   3.274   3.803   115   16.6  19:48 (  0, 47)  

* C/2022 V2 ( Lemmon )

It is expected to brighten up to 16 mag in winter. Now it is 17.7 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). 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. It is fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  11 54.92    3 53.6   2.422   2.072    57   16.6   5:09 (296, 38)  
Nov. 25  11 53.86    1  4.5   2.316   2.081    63   16.5   5:14 (307, 42)  

* C/2022 QE78 ( ATLAS )

Now it is 16.0 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). 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)  
Nov. 18   4 50.61  -12 47.0   6.438   7.249   142   16.6   1:05 (  0, 42)  
Nov. 25   4 48.11  -12 48.8   6.390   7.217   144   16.6   0:35 (  0, 42)  

* C/2021 S4 ( Tsuchinshan )

Now it is 16.8 mag (Nov. 4, 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)  
Nov. 18   4 54.63   41 35.6   5.812   6.696   151   16.7   1:10 (180, 83)  
Nov. 25   4 51.82   41 42.6   5.779   6.694   156   16.7   0:40 (180, 83)  

* C/2020 Y2 ( ATLAS )

It brightened up to 14.1 mag in 2022 spring (Mar. 22, 2022, Chris Wyatt). Now it is 16.0 mag (Nov. 16, ATLAS Chile). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   1 42.79   -1 53.4   4.796   5.645   146   16.7  21:54 (  0, 53)  
Nov. 25   1 37.12   -1 35.3   4.915   5.693   138   16.7  21:21 (  0, 54)  

* 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 17.1 mag (Nov. 14, ATLAS Chile). It stays 16 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January. But it will be observable again in March in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  20 40.85  -18 39.8   6.656   6.431    72   16.7  18:20 ( 25, 33)  
Nov. 25  20 43.91  -18 25.2   6.720   6.389    66   16.7  18:18 ( 31, 31)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 17.1 mag (Nov. 11, 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)  
Nov. 18   4  3.64  -77 26.0  10.379  10.313    83   16.8   0:17 (  0,-22)  
Nov. 25   3 46.48  -77 20.9  10.403  10.313    82   16.8  23:27 (  0,-22)  

* C/2020 S4 ( PanSTARRS )

It brightened up to 13.9 mag in early 2023 (Jan. 21, Hidenori Nohara). Now it is 16.3 mag (June 17, Ken-ichi Kadota). It stays 17 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  13 39.05    7 48.3   4.976   4.247    38   16.8   5:09 (275, 20)  
Nov. 25  13 46.56    7 23.9   4.951   4.284    43   16.8   5:14 (279, 25)  

* C/2022 U3 ( Bok )

Now it is 17.3 mag (Nov. 15, A. Diepvens). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere. But it will become high in autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18   5  1.49   37 42.6   4.315   5.214   152   16.9   1:17 (180, 87)  
Nov. 25   4 58.10   37 15.7   4.260   5.194   159   16.9   0:46 (180, 88)  

* C/2023 C2 ( ATLAS )

It is expected to brighten up to 12.5 mag in 2024 summer. Now it is 17.3 mag (July 28, ATLAS South Africa). Brightening slowly. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it will be getting higher gradually. Around the high light, it is observable in good condition in the Southern Hemisphere, but it locates very low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  13  3.99  -51 29.3   5.128   4.461    43   17.0   5:09 (326,-12)  
Nov. 25  13 14.73  -52 37.1   5.047   4.406    45   17.0   5:14 (329,-11)  

* 170P/Christensen

Now it is 16.1 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). 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)  
Nov. 18   3 37.82    4 19.4   2.177   3.143   165   17.1  23:49 (  0, 59)  
Nov. 25   3 33.04    4  8.6   2.202   3.157   162   17.2  23:16 (  0, 59)  

* 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 17.5 mag (Nov. 14, ATLAS Chile). 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)  
Nov. 18   3 53.92  -21 22.5   2.359   3.174   139   17.4   0:09 (  0, 34)  
Nov. 25   3 45.30  -21  9.6   2.297   3.102   138   17.1  23:28 (  0, 34)  

* 65P/Gunn

It will be observable at 15-16 mag from 2024 to 2025. Now it is 17.9 mag (Apr. 25, A. Diepvens). Brightening slowly. 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)  
Nov. 18  12 29.36    4 58.9   4.412   3.862    50   17.3   5:09 (289, 32)  
Nov. 25  12 35.98    4 22.4   4.312   3.847    55   17.2   5:14 (294, 37)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.7 mag (Nov. 13, Jean-Claude Merlin). 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)  
Nov. 18   5  9.13  -40 47.6   7.358   7.841   115   17.2   1:24 (  0, 14)  
Nov. 25   5  6.63  -40 59.6   7.326   7.817   116   17.2   0:54 (  0, 14)  

* C/2022 U1 ( Leonard )

Now it is 16.9 mag (Nov. 12, ATLAS-HKO, Haleakala). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  23  8.73   51 17.3   3.759   4.338   119   17.2  19:20 (180, 74)  
Nov. 25  22 58.31   49 26.4   3.816   4.324   114   17.3  18:42 (180, 76)  

* P/2023 M4 ( ATLAS )

Now it is 16.8 mag (Nov. 7, ATLAS Chile). Fading slowly. It will be fainter than 18 mag in January. 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)  
Nov. 18  21 17.45  -11 17.3   4.674   4.662    83   17.3  18:20 ( 17, 42)  
Nov. 25  21 21.30  -11  0.4   4.795   4.676    77   17.4  18:18 ( 24, 41)  

* P/2001 Q6 ( NEAT )

First return of a new periodic comet which brightened up to 10 mag in 2001. It is expected to brighten up to 12-13 mag from February to March in 2024. It will brighten rapidly after this. In the Northern Hemisphere, it will be getting higher gradually. 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)  
Nov. 18  23 17.52  -32  9.0   1.470   1.918   100   17.7  19:29 (  0, 23)  
Nov. 25  23 11.63  -27 50.9   1.492   1.862    95   17.6  18:56 (  0, 28)  

* C/2020 F2 ( ATLAS )

Now it is 17.0 mag (Apr. 11, Michael Jager). 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 be observable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  12 32.59   12 39.6   9.807   9.263    54   17.6   5:09 (280, 36)  
Nov. 25  12 33.15   12 48.3   9.716   9.275    60   17.6   5:14 (286, 43)  

* 71P/Clark

It brightened up to 12.8 mag in spring (Mar. 8, Taras Prystavski). Now it is 17.0 mag (Oct. 19, 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)  
Nov. 18   0 31.10   -5 22.6   2.164   2.895   129   17.6  20:43 (  0, 50)  
Nov. 25   0 30.23   -4 54.3   2.279   2.931   122   17.9  20:14 (  0, 50)  

* C/2021 A9 ( PanSTARRS )

Now it is 18.3 mag (Nov. 13, Toshihiko Ikemura, Hirohisa Sato). 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)  
Nov. 18   7 28.94    9 52.3   7.193   7.761   121   17.8   3:44 (  0, 65)  
Nov. 25   7 24.52    9 42.1   7.092   7.760   129   17.8   3:12 (  0, 65)  

* 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 soon. 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)  
Nov. 18  23 12.03   66 26.8   0.350   1.191   117   17.8  19:26 (180, 58)  
Nov. 25   0  0.02   67 12.8   0.377   1.222   120   17.9  19:47 (180, 58)  

* 404P/2020 M6 ( Bressi )

Now it is 18.8 mag (Nov. 14, Toshihiko Ikemura, Hirohisa Sato). 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)  
Nov. 18   4 59.24   24 40.1   3.196   4.133   158   17.8   1:15 (  0, 80)  
Nov. 25   4 54.99   24 23.4   3.166   4.133   166   17.8   0:43 (  0, 79)  

* C/2023 V5 ( Leonard )

Tiny member of Comet C/1988 A1 ( Liller )'s group. Now it is 17.4 mag (Nov. 6, Catalina Sky Survey). It will fade out rapidly after this. In the Northern Hemisphere, it will be getting lower gradually. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov. 18  20  3.72   16 33.9   0.405   0.973    75   18.4  18:20 ( 66, 56)  
Nov. 25  19 29.23   21 57.2   0.542   0.917    66   18.8  18:18 ( 85, 48)  

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Copyright(C) Seiichi Yoshida (comet@aerith.net). All rights reserved.