Weekly Information about Bright Comets (2024 Feb. 3: North)

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Updated on February 4, 2024
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Best time and the azimuth, altitude (A,h) are at lat. 35 deg in the Northern Hemisphere.
Azimuth indicates 0 for south, 90 for west, 180 for north, 270 for east.

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* 62P/Tsuchinshan 1

Now it is 8.2 mag (Jan. 21, Michael Jager). 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)  
Feb.  3  12 36.82    9 52.6   0.501   1.351   127    8.4   3:47 (  0, 65)  
Feb. 10  12 41.25    9 46.7   0.504   1.383   133    8.7   3:24 (  0, 65)  

* 12P/Pons-Brooks

It returns for the first time in 70 years. It will brighten up to 4.5 mag in spring. It suddenly brightened in major outburst by 5 mag up to 11.5 mag on July 20 (E. Tamas, Francois Kugel). It brightened again in another major outburst up to 9.4 mag on Nov. 15 (Nick James). Now it is 8.2 mag (Feb. 1, Osamu Miyazaki). It will brighten rapidly after this. In the Northern Hemisphere, it will be unobservable in April. In the Southern Hemisphere, it is not observable now, but it will appear in April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  21 30.76   38 15.8   1.898   1.566    55    8.9  18:56 (125, 18)  
Feb. 10  22  1.28   38  6.9   1.833   1.473    53    8.6  19:02 (125, 18)  

* C/2021 S3 ( PanSTARRS )

Now it is 9.8 mag (Jan. 23, Taras Prystavski). 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 May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  16 46.71  -25 16.5   1.518   1.332    59    9.4   5:31 (325, 20)  
Feb. 10  17  9.68  -20 58.3   1.454   1.322    62    9.2   5:26 (322, 24)  

* 144P/Kushida

Now it is 10.0 mag (Feb. 1, 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)  
Feb.  3   4 13.79   15 49.1   0.705   1.402   111   10.1  19:23 (  0, 71)  
Feb. 10   4 33.36   16 19.6   0.740   1.410   108   10.1  19:15 (  0, 71)  

* C/2023 S3 ( Lemmon )

Now it is 13.3 mag (Dec. 16, Michael Mattiazzo). It will fade out rapidly after this. It will be fainter than 18 mag in April. 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)  
Feb.  3  20 18.22  -34 57.9   1.721   0.872    20   11.9   5:31 (300,-19)  
Feb. 10  20  7.90  -33 55.7   1.683   0.919    26   12.5   5:26 (303,-13)  

* C/2022 E2 ( ATLAS )

Now it is 12.7 mag (Jan. 31, Osamu Miyazaki). It stays 13 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)  
Feb.  3   8 17.88   20 33.2   3.201   4.172   168   12.5  23:25 (  0, 76)  
Feb. 10   8  5.50   22  9.3   3.210   4.143   158   12.4  22:45 (  0, 77)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. Now it is 13.8 mag (Jan. 18, ATLAS South Africa). Fading slowly. In the Northern Hemisphere, it will never be observable after this. It locates somewhat low in the Southern Hemisphere. But it will become high in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  23 28.52  -39 48.4   4.409   3.695    38   12.9  18:56 ( 44, -5)  
Feb. 10  23 32.39  -39 36.9   4.499   3.751    36   13.0  19:02 ( 48,-10)  

* C/2023 A3 ( Tsuchinshan-ATLAS )

It will approach to Sun down to 0.4 a.u. in late September, and it is expected to brighten up to 0 mag. Now it is 13.5 mag (Jan. 21, Michael Jager). It will brighten rapidly after this. It stays observable in good condition. 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)  
Feb.  3  15 10.79   -7 53.9   3.814   3.870    85   13.3   5:31 (342, 45)  
Feb. 10  15 10.99   -7 51.6   3.608   3.787    92   13.1   5:26 (350, 47)  

* 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 13.5 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). It will fade out rapidly after this. It will be fainter than 18 mag in May. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   8  9.35   -9 41.3   0.868   1.792   150   13.2  23:16 (  0, 45)  
Feb. 10   8  4.30   -7 55.3   0.939   1.854   148   13.6  22:44 (  0, 47)  

* P/2023 W1 ( 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. Now it is 16.4 mag (Jan. 11, Toshihiko Ikemura, Hirohisa Sato). Fading gradually. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will never be observable after this. Thomas Lehmann reported it was bright as 13.1 mag on Jan. 28.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  23 43.56   15 34.4   1.835   1.439    51   13.7  18:56 ( 87, 33)  
Feb. 10  23 52.46   19 36.5   1.862   1.422    48   13.2  19:02 ( 95, 30)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 13.0 mag (Jan. 31, Osamu Miyazaki). Fading slowly. In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in May. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   5 12.66    2  0.1   4.316   4.904   121   13.2  20:21 (  0, 57)  
Feb. 10   5  9.81    3  2.7   4.473   4.965   114   13.4  19:50 (  0, 58)  

* 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 14.6 mag (Jan. 24, ATLAS Chile). It will fade out rapidly after this. It will be fainter than 18 mag in May. It stays observable in good condition. Vladimir Bezugly reported it is visible at around 12 mag in the SOHO LASCO images in late January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   2  5.72  -16 30.0   0.360   0.939    71   13.5  18:56 ( 29, 33)  
Feb. 10   2 40.35  -16 57.0   0.315   0.949    73   13.3  19:02 ( 28, 33)  

* C/2022 L2 ( ATLAS )

Now it is 14.2 mag (Jan. 16, Ken-ichi Kadota). It stays 13 mag for a while. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition. It is expected to brighten up to 12.5 mag in 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)  
Feb.  3  15 24.48  -24 55.4   2.746   2.722    78   13.5   5:31 (343, 28)  
Feb. 10  15 18.76  -26 44.1   2.594   2.713    86   13.3   5:26 (351, 28)  

* 29P/Schwassmann-Wachmann 1

Now it is 12.5 mag (Jan. 30, Osamu Miyazaki). It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   8 19.26   21 17.4   5.206   6.175   168   13.5  23:27 (  0, 76)  
Feb. 10   8 15.92   21 22.4   5.236   6.177   160   13.5  22:56 (  0, 76)  

* C/2019 U5 ( PanSTARRS )

Now it is 13.7 mag (Jan. 21, Chris Wyatt). Fading slowly. In the Northern Hemisphere, it will be unobservable in May. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   9  2.57  -45 50.2   4.009   4.546   117   13.7   0:14 (  0,  9)  
Feb. 10   8 47.84  -45 49.5   4.026   4.582   118   13.7  23:26 (  0,  9)  

* 26P/Grigg-Skjellerup

Now it is 15.1 mag (Jan. 23, Ken-ichi Kadota). Fading rapidly. It will be fainter than 18 mag soon. It locates somewhat low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  18 41.98  -13 24.4   1.881   1.201    34   14.1   5:31 (296, 12)  
Feb. 10  19  6.35  -11 34.4   1.907   1.241    35   15.1   5:26 (294, 12)  

* C/2021 G2 ( ATLAS )

Now it is 14.5 mag (Jan. 24, ATLAS Chile). It stays 14 mag for a while. It stays extremely 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)  
Feb.  3  12 14.89  -38 47.1   4.861   5.259   108   14.1   3:26 (  0, 16)  
Feb. 10  12 14.62  -38 53.5   4.759   5.242   114   14.1   2:58 (  0, 16)  

* C/2021 T4 ( Lemmon )

It brightened up to 7.8 mag in late July (July 20, Thomas Lehmann). Now it is 15.6 mag (Jan. 28, Thomas Lehmann). Fading gradually. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  15  2.72    0 44.6   2.670   2.851    90   14.2   5:31 (342, 54)  
Feb. 10  14 56.04    2 33.9   2.597   2.921    99   14.2   5:26 (354, 57)  

* 13P/Olbers

It returned for the first time in 68 years. It will brighten up to 7.5 mag in summer. Now it is 13.6 mag (Feb. 2, Alan Hale). It will brighten rapidly after this. 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 April. 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)  
Feb.  3   2 52.03   -5 16.2   2.232   2.373    85   14.5  18:56 ( 21, 48)  
Feb. 10   2 53.59   -2 53.1   2.252   2.299    80   14.2  19:02 ( 33, 47)  

* C/2019 L3 ( ATLAS )

It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 15.7 mag (Jan. 31, ATLAS Chile). It stays 15 mag for a while. In the Northern Hemisphere, it will be unobservable in May. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  11 20.23  -52 56.9   6.937   7.242   104   14.3   2:31 (  0,  2)  
Feb. 10  11 16.72  -53 24.7   6.918   7.288   108   14.4   2:00 (  0,  1)  

* 32P/Comas Sola

Now it is 14.7 mag (Jan. 27, Thomas Lehmann). It stays 15 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 winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   3  3.67   22  3.0   1.793   2.140    96   14.7  18:56 ( 39, 74)  
Feb. 10   3 12.35   22 55.9   1.852   2.121    91   14.8  19:02 ( 56, 71)  

* C/2023 H2 ( Lemmon )

It approached to Earth down to 0.2 a.u. in early November, and brightened up to 6.2 mag (Nov. 11, Marco Goiato). Now it is 13.2 mag (Jan. 3, Chris Wyatt). It will fade out rapidly after this. It will be fainter than 18 mag in May. 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)  
Feb.  3  23 50.42  -43 20.4   2.412   1.838    44   14.8  18:56 ( 39, -5)  
Feb. 10  23 59.45  -43 30.9   2.533   1.928    42   15.1  19:02 ( 42, -8)  

* C/2020 K1 ( PanSTARRS )

It brightened up to 12.1 mag in 2023 spring (May 20, Jose Guilherme de S. Aguiar). Now it is 14.8 mag (Jan. 21, Chris Wyatt). Fading slowly. 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)  
Feb.  3   3 47.78  -72  6.7   4.111   4.013    77   15.0  18:56 (  0,-17)  
Feb. 10   3 51.62  -69 35.4   4.143   4.054    78   15.1  19:02 (  3,-15)  

* 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 16.4 mag (Jan. 19, Hidetaka Sato). It will fade out rapidly after this. It will be fainter than 18 mag in May. 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)  
Feb.  3  10 20.47  -57 25.6   2.308   2.720   104   15.2   1:33 (  0, -3)  
Feb. 10   9 54.01  -56 42.4   2.345   2.817   108   15.3   0:39 (  0, -2)  

* 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 15.1 mag (Jan. 20, Thomas Lehmann). It stays 16 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)  
Feb.  3  17 25.52   19 26.4   6.779   6.418    64   15.4   5:31 (279, 47)  
Feb. 10  17 29.77   20  9.9   6.748   6.457    68   15.5   5:26 (281, 51)  

* C/2023 C2 ( ATLAS )

It is expected to brighten up to 12.5 mag in summer. Now it is 17.1 mag (Dec. 20, E. Cortes). Brightening gradually. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition. 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)  
Feb.  3  15 15.08  -64 57.5   4.022   3.860    73   15.9   5:31 (354,-11)  
Feb. 10  15 28.01  -66 11.3   3.906   3.806    76   15.8   5:26 (355,-12)  

* C/2022 QE78 ( ATLAS )

Now it is 15.6 mag (Jan. 11, 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 May. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   4 28.51   -9  3.9   6.555   6.914   107   15.8  19:37 (  0, 46)  
Feb. 10   4 28.50   -8 23.1   6.619   6.884   101   15.8  19:09 (  0, 47)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 16.6 mag (Jan. 23, 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)  
Feb.  3   2 52.07  -64  6.7  16.983  16.734    73   15.9  18:56 (  6,-10)  
Feb. 10   2 52.69  -63 47.8  16.978  16.709    72   15.9  19:02 ( 10,-10)  

* 226P/Pigott-LINEAR-Kowalski

Now it is 15.4 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). It will fade out rapidly after this. It will be fainter than 18 mag in April. In the Northern Hemisphere, it will be getting lower gradually. In the Southern Hemisphere, it will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   1 26.34    9 16.2   1.889   1.809    70   15.9  18:56 ( 60, 49)  
Feb. 10   1 36.30   12 36.2   1.975   1.823    66   16.1  19:02 ( 70, 47)  

* P/2023 WM26 ( Elenin )

First return of a new periodic comet which was discovered in 2011, half a year after the perihelion passage. It is expected to brighten up to 14.5 mag in spring. Now it is 16.3 mag (Jan. 14, ATLAS-MLO, Mauna Loa). Brightening slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   8 21.88   10 25.0   0.753   1.730   168   16.3  23:29 (  0, 65)  
Feb. 10   8 11.66    8 34.1   0.711   1.672   159   16.0  22:51 (  0, 63)  

* C/2022 S4 ( Lemmon )

Now it is 16.0 mag (Jan. 1, Ken-ichi Kadota). It stays 16 mag for a while. In the Northern Hemisphere, it will be unobservable in March. In the Southern Hemisphere, it will be getting lower gradually. But it will be getting higher again after May. The brightness evolution is slower than originally expected.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   1 41.16  -30 39.9   3.548   3.243    64   16.1  18:56 ( 28, 18)  
Feb. 10   1 43.07  -30 41.2   3.593   3.207    59   16.1  19:02 ( 34, 15)  

* 65P/Gunn

It will be observable at 15-16 mag from 2024 to 2025. Now it is 17.3 mag (Jan. 24, ATLAS South Africa). 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)  
Feb.  3  13 18.76    1 34.9   3.160   3.692   115   16.2   4:29 (  0, 56)  
Feb. 10  13 19.40    1 42.8   3.054   3.676   122   16.1   4:03 (  0, 57)  

* 150P/LONEOS

Now it is 16.1 mag (Jan. 29, ATLAS Chile). Fading slowly. It will be fainter than 18 mag in May. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   8 56.56  -12 21.7   0.858   1.784   150   16.3   0:08 (  0, 43)  
Feb. 10   8 50.72  -13 57.8   0.849   1.772   149   16.3  23:30 (  0, 41)  

* C/2023 V4 ( Camarasa-Duszanowicz )

It is expected to brighten up to 13 mag in early summer. Now it is 15.9 mag (Jan. 28, ATLAS Chile). Brightening gradually. 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 April. At the high light, it is not observable in the Southern Hemisphere, or it locates low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   2  1.62  -19 56.7   2.213   2.097    70   16.4  18:56 ( 29, 30)  
Feb. 10   2  3.40  -16 12.7   2.219   2.017    65   16.3  19:02 ( 39, 30)  

* C/2021 Y1 ( ATLAS )

It brightened up to 13 mag in early 2023. 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)  
Feb.  3  16 26.42  -48  5.5   4.061   3.731    63   16.4   5:31 (340,  2)  
Feb. 10  16 30.72  -48  1.6   4.026   3.790    69   16.4   5:26 (342,  3)  

* 227P/Catalina-LINEAR

Now it is 15.4 mag (Jan. 31, ATLAS-MLO, Mauna Loa). Fading slowly. It will be fainter than 18 mag in May. 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)  
Feb.  3   7 25.24   39 19.1   0.733   1.658   149   16.5  22:33 (180, 86)  
Feb. 10   7 24.70   38 56.9   0.746   1.645   143   16.5  22:05 (180, 86)  

* 471P/2023 KF3

Now it is 16.3 mag (Jan. 28, ATLAS-HKO, Haleakala). Fading gradually. It will be fainter than 18 mag in April. In the Northern Hemisphere, it will be getting lower gradually. In the Southern Hemisphere, it will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   0 42.03    8 41.8   2.484   2.164    59   16.5  18:56 ( 70, 41)  
Feb. 10   0 56.20    9 59.3   2.561   2.177    56   16.7  19:02 ( 75, 38)  

* C/2022 T1 ( Lemmon )

Now it is 16.9 mag (Jan. 20, ATLAS Chile). It stays 16 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in summer. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  13 57.90  -28  2.7   3.206   3.447    95   16.6   5:09 (  0, 27)  
Feb. 10  14  2.95  -28 23.7   3.111   3.446   101   16.5   4:46 (  0, 26)  

* C/2023 F3 ( ATLAS )

It stays 16 mag in the Southern sky for a long time from 2024 to 2025. 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)  
Feb.  3  16 55.36  -44 37.8   6.324   5.868    58   16.7   5:31 (333,  3)  
Feb. 10  16 55.42  -45 16.7   6.195   5.844    64   16.6   5:26 (337,  4)  

* 125P/Spacewatch

It is expected to brighten up to 15.5 mag from March to April. Now it is 16.9 mag (Jan. 27, ATLAS-HKO, Haleakala). Brightening slowly. It locates somewhat low in the Northern Hemisphere. But it will become high in spring. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  16 49.26  -14 24.0   1.783   1.562    60   17.0   5:31 (318, 29)  
Feb. 10  17 11.46  -14 32.3   1.732   1.549    62   16.7   5:26 (318, 29)  

* C/2022 U3 ( Bok )

Now it is 17.0 mag (Jan. 9, Toshihiko Ikemura, Hirohisa Sato). It stays 17 mag for a while. It will be unobservable in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   4 34.22   30 24.1   4.484   5.019   117   16.8  19:43 (  0, 85)  
Feb. 10   4 35.16   29 44.2   4.567   5.005   110   16.8  19:16 (  0, 85)  

* C/2021 S4 ( Tsuchinshan )

Now it is 17.3 mag (Jan. 28, Thomas Lehmann). 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 April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   4 31.80   40 27.4   6.179   6.693   117   16.8  19:41 (180, 85)  
Feb. 10   4 32.49   40 13.9   6.276   6.694   111   16.8  19:14 (180, 85)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 16.9 mag (Jan. 15, 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)  
Feb.  3   2 13.33  -70 55.0  10.616  10.322    70   16.8  18:56 (  8,-17)  
Feb. 10   2 12.17  -70  4.9  10.627  10.323    69   16.8  19:02 ( 11,-18)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.5 mag (Jan. 25, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it will be unobservable in April. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   4 45.79  -37 23.3   7.366   7.581    98   17.0  19:54 (  0, 18)  
Feb. 10   4 45.74  -36 35.5   7.398   7.558    95   17.0  19:26 (  0, 19)  

* C/2023 K1 ( ATLAS )

It brightened very rapidly up to 14.9 mag in early summer (July 13, Taras Prystavski). Now it is 17.2 mag (Jan. 16, Ken-ichi Kadota). Fading gradually. It will be fainter than 18 mag in April. 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)  
Feb.  3  14 58.38   10  1.3   2.423   2.679    93   17.1   5:31 (339, 63)  
Feb. 10  14 53.22   13 27.6   2.343   2.730   102   17.1   5:26 (353, 68)  

* 30P/Reinmuth 1

Now it is 17.3 mag (Jan. 15, ATLAS-HKO, Haleakala). It stays 17 mag for a while. It will be unobservable in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   1 49.03    3 31.7   2.569   2.475    73   17.2  18:56 ( 48, 49)  
Feb. 10   1 56.86    4 37.7   2.620   2.439    68   17.1  19:02 ( 56, 45)  

* C/2022 A3 ( Lemmon-ATLAS )

Now it is 17.6 mag (Jan. 22, Jean-Claude Merlin). It stays 18 mag for a while. 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)  
Feb.  3   5 59.56  -72 22.9   3.818   3.872    85   17.3  21:04 (  0,-17)  
Feb. 10   5 31.39  -71 34.2   3.850   3.890    84   17.3  20:09 (  0,-16)  

* P/2023 Y3 ( ATLAS )

Now it is 17.5 mag (Jan. 29, D. Buczynski). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   6 49.23   18 18.1   1.570   2.462   148   17.3  21:57 (  0, 73)  
Feb. 10   6 46.68   19  9.0   1.609   2.452   140   17.3  21:27 (  0, 74)  

* C/2023 T3 ( Fuls )

Now it is 17.3 mag (Jan. 27, ATLAS-HKO, Haleakala). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   7 55.18   -9 32.2   3.883   4.753   148   17.4  23:03 (  0, 45)  
Feb. 10   7 51.86   -9 27.5   3.868   4.714   145   17.4  22:32 (  0, 45)  

* 170P/Christensen

Now it is 16.7 mag (Jan. 30, ATLAS Chile). Fading slowly. It will be fainter than 18 mag in March. It will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   3 24.91    7 40.1   3.033   3.308    97   17.4  18:56 ( 12, 62)  
Feb. 10   3 28.98    8 20.7   3.147   3.324    91   17.5  19:02 ( 27, 61)  

* C/2022 V2 ( Lemmon )

Now it is 17.0 mag (Jan. 27, ATLAS South Africa). Fading gradually. It will be fainter than 18 mag in March. 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)  
Feb.  3   9 35.27  -33 25.9   1.573   2.325   129   17.4   0:48 (  0, 22)  
Feb. 10   9  5.77  -35 14.5   1.606   2.362   129   17.5  23:43 (  0, 20)  

* 216P/LINEAR

Now it is 17.4 mag (Jan. 10, ATLAS Chile). Fading gradually. It will be fainter than 18 mag in March. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  12 16.26    3  0.1   1.361   2.138   130   17.5   3:27 (  0, 58)  
Feb. 10  12 16.39    2 28.4   1.311   2.144   137   17.5   3:00 (  0, 57)  

* C/2022 E3 ( ZTF )

It approached to Earth down to 0.29 a.u. in early last February, and it brightened up to 4.5 mag (Feb. 1, Juan Jose Gonzalez). Now it is 19.2 mag (Jan. 12, ATLAS South Africa). 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)  
Feb.  3   3  2.43  -55 38.9   5.105   4.961    76   17.5  18:56 (  6, -1)  
Feb. 10   3  0.59  -54 28.8   5.215   5.028    73   17.6  19:02 ( 12, -1)  

* C/2020 Y2 ( ATLAS )

It brightened up to 14.1 mag in 2022 spring (Mar. 22, 2022, Chris Wyatt). Now it is 17.2 mag (Jan. 13, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. It will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   1 16.83    3 26.3   6.510   6.172    65   17.5  18:56 ( 57, 43)  
Feb. 10   1 17.83    4  3.5   6.667   6.220    59   17.6  19:02 ( 65, 38)  

* 117P/Helin-Roman-Alu 1

Now it is 16.9 mag (Jan. 22, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will be unobservable in March. It is brighter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   0 38.73   -1  6.9   4.437   3.960    55   17.5  18:56 ( 61, 33)  
Feb. 10   0 44.76   -0 16.6   4.538   3.976    49   17.6  19:02 ( 67, 29)  

* C/2020 F2 ( ATLAS )

Now it is 17.3 mag (Jan. 20, ATLAS-HKO, Haleakala). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  12 20.61   16 41.5   8.709   9.407   132   17.5   3:32 (  0, 72)  
Feb. 10  12 17.26   17 15.8   8.643   9.421   140   17.5   3:01 (  0, 72)  

* 299P/Catalina-PanSTARRS

Now it is 17.7 mag (Jan. 11, Ken-ichi Kadota). It stays 17 mag for a while. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  15 26.90  -27 17.2   3.257   3.187    77   17.6   5:31 (344, 26)  
Feb. 10  15 34.28  -27 47.9   3.157   3.183    82   17.5   5:26 (347, 26)  

* C/2023 T2 ( Borisov )

Now it is 17.3 mag (Jan. 22, ATLAS-HKO, Haleakala). Fading gradually. 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)  
Feb.  3   3 18.61   69  8.4   1.542   2.060   107   17.6  18:56 (176, 56)  
Feb. 10   3 54.06   65 54.5   1.586   2.082   105   17.7  19:02 (175, 59)  

* C/2023 H5 ( Lemmon )

Now it is 17.7 mag (Jan. 31, ATLAS-HKO, Haleakala). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3  10 58.45    2 20.4   5.102   5.962   148   17.7   2:10 (  0, 57)  
Feb. 10  10 54.65    3 24.5   5.007   5.925   156   17.6   1:38 (  0, 58)  

* C/2023 R2 ( PanSTARRS )

Now it is 18.0 mag (Jan. 14, Toshihiko Ikemura, Hirohisa Sato). It will brighten rapidly after this. In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in April. In the Southern Hemisphere, it will be getting lower gradually. It will brighten up to 11 mag in summer. But it is not observable at the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   2 15.06   -7 54.9   3.081   3.004    76   17.7  18:56 ( 31, 42)  
Feb. 10   2 18.48   -7 17.3   3.097   2.922    70   17.6  19:02 ( 40, 39)  

* C/2024 A1 ( ATLAS )

Now it is 17.8 mag (Jan. 19, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in March. In the Southern Hemisphere, it stays observable in good condition. It stays 15 mag for a long time from late 2024 to early 2026.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   6 22.66  -61 51.2   5.520   5.694    95   17.8  21:29 (  0, -7)  
Feb. 10   6 15.86  -60 28.5   5.476   5.654    95   17.7  20:55 (  0, -5)  

* C/2021 A9 ( PanSTARRS )

Now it is 18.5 mag (Jan. 29, Yasukazu Ikari). 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)  
Feb.  3   6 27.11    9 15.1   6.976   7.770   141   17.7  21:35 (  0, 64)  
Feb. 10   6 22.10    9 19.0   7.060   7.772   133   17.8  21:02 (  0, 64)  

* 126P/IRAS

It brightened up to 13.6 mag in summer (July 16, Mitsunori Tsumura). Now it is 17.1 mag (Jan. 10, Thomas Lehmann). Fading gradually. 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)  
Feb.  3   0 58.31   62 52.1   2.540   2.754    91   17.8  18:56 (150, 52)  
Feb. 10   1 16.50   62 50.2   2.643   2.803    88   18.0  19:02 (149, 50)  

* 408P/2020 M7 ( Novichonok-Gerke )

Now it is 17.2 mag (Jan. 19, ATLAS-HKO, Haleakala). Fading slowly. It will be fainter than 18 mag soon. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  3   8 30.37   -3 24.5   3.166   4.098   158   17.8  23:38 (  0, 52)  
Feb. 10   8 26.46   -2 50.7   3.191   4.113   156   17.9  23:06 (  0, 52)  

* (468861) 2013 LU28

Far asteroid moving along a cometary orbit. It brightens up to 18 mag from 2024 to 2025. 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)  
Feb.  3   8 23.25   50 53.1   7.953   8.778   145   17.9  23:31 (180, 74)  
Feb. 10   8 15.89   50 42.5   7.987   8.775   140   17.9  22:56 (180, 74)  

* C/2020 S4 ( PanSTARRS )

It brightened up to 13.9 mag in early 2023 (Jan. 21, Hidenori Nohara). Now it is 19.1 mag (Jan. 11, 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)  
Feb.  3  14 40.03    7 10.2   4.452   4.685    97   17.9   5:31 (350, 62)  
Feb. 10  14 42.37    7 31.5   4.396   4.727   103   17.9   5:25 (  0, 62)  

* 244P/Scotti

Now it is 18.9 mag (Jan. 13, ATLAS-MLO, Mauna Loa). 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)  
Feb.  3  10  5.95   13 11.3   3.297   4.254   164   17.9   1:17 (  0, 68)  
Feb. 10  10  1.97   13 31.0   3.284   4.264   172   17.9   0:46 (  0, 68)  

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