Weekly Information about Bright Comets (2024 Mar. 2: North)

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Updated on March 1, 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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* 12P/Pons-Brooks

It returns for the first time in 70 years. It will brighten up to 4.5 mag in spring. Now it is 7.0 mag (Feb. 27, Osamu Miyazaki). It will turn to fade out rapidly after brightening. 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)  
Mar.  2  23 43.53   35 30.2   1.685   1.198    44    7.2  19:20 (122, 17)  
Mar.  9   0 19.22   33 35.3   1.654   1.111    40    6.7  19:26 (120, 16)  

* C/2021 S3 ( PanSTARRS )

Now it is 9.7 mag (Feb. 21, Taras Prystavski). 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 May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  18 13.31   -4 45.8   1.322   1.342    69    9.1   5:04 (311, 37)  
Mar.  9  18 32.61    1 25.4   1.303   1.365    71    9.1   4:55 (306, 41)  

* 62P/Tsuchinshan 1

It brightened up to 7.4 mag from December to January (Dec. 24, Osamu Miyazaki). Now it is 8.9 mag (Feb. 13, Chris Wyatt). It will fade out rapidly after this. It will be fainter than 18 mag in June. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  12 35.72   10 17.3   0.541   1.497   154    9.9   1:57 (  0, 65)  
Mar.  9  12 30.26   10 23.3   0.567   1.540   161   10.4   1:24 (  0, 65)  

* 144P/Kushida

Now it is 10.9 mag (Feb. 27, 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)  
Mar.  2   5 36.98   17 27.9   0.874   1.460   102   10.3  19:20 ( 18, 72)  
Mar.  9   5 58.83   17 36.6   0.929   1.484   101   10.5  19:26 ( 26, 71)  

* 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 12.7 mag (Feb. 15, ATLAS Chile). 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)  
Mar.  2  15  5.29   -7 18.1   2.998   3.535   115   12.4   4:26 (  0, 48)  
Mar.  9  15  0.68   -6 56.3   2.803   3.449   123   12.1   3:54 (  0, 48)  

* C/2022 E2 ( ATLAS )

Now it is 12.8 mag (Feb. 18, Ken-ichi Kadota). It stays 13 mag for a while. It will be unobservable in June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   7 31.40   26 15.0   3.367   4.061   128   12.4  20:49 (  0, 81)  
Mar.  9   7 21.94   27 20.4   3.453   4.035   119   12.5  20:12 (  0, 82)  

* 473P/2023 W1 ( NEAT )

First return of a new periodic comet which brightened up to 10 mag in 2001. Now it is 13.1 mag (Feb. 18, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in June. It locates somewhat low 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)  
Mar.  2   0 25.38   31 49.9   1.922   1.407    44   12.7  19:20 (115, 22)  
Mar.  9   0 39.02   35 57.0   1.936   1.414    44   12.7  19:26 (121, 21)  

* C/2022 L2 ( ATLAS )

Now it is 14.0 mag (Feb. 16, Hiroshi Abe). Fading slowly. In the Northern Hemisphere, it will be unobservable in June. In the Southern Hemisphere, 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)  
Mar.  2  14 44.91  -32 46.9   2.165   2.695   111   12.9   4:06 (  0, 22)  
Mar.  9  14 26.01  -34 49.6   2.045   2.693   120   12.8   3:20 (  0, 20)  

* 207P/NEAT

Now it is 13.8 mag (Feb. 12, Hiroshi Abe). 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 was 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)  
Mar.  2   5 32.66  -14  8.0   0.222   1.045    98   12.9  19:20 (  8, 41)  
Mar.  9   6 49.37  -10 12.3   0.224   1.095   111   13.1  19:44 (  0, 45)  

* 13P/Olbers

It returned for the first time in 68 years. It will brighten up to 7.5 mag in summer. Now it is 13.1 mag (Feb. 14, 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 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)  
Mar.  2   3  5.75    4 30.2   2.303   2.076    64   13.3  19:20 ( 64, 39)  
Mar.  9   3 12.14    7  0.8   2.314   2.003    59   13.0  19:26 ( 72, 36)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. Now it is 12.6 mag (Feb. 2, Chris Wyatt). It stays 14 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  23 45.53  -39 25.8   4.698   3.920    34   13.3  19:20 ( 58,-24)  
Mar.  9  23 50.23  -39 31.0   4.740   3.977    35   13.4  19:26 ( 60,-29)  

* 29P/Schwassmann-Wachmann 1

Now it is 14.7 mag (Feb. 13, Chris Wyatt). In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in July. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   8  7.82   21 29.4   5.411   6.183   137   13.6  21:25 (  0, 76)  
Mar.  9   8  6.02   21 28.7   5.493   6.184   130   13.6  20:56 (  0, 76)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 13.2 mag (Feb. 13, Chris Wyatt). Fading slowly. It will be getting lower gradually after this, and it will be unobservable in May in the Northern Hemisphere, or in June in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   5  6.10    5 58.2   4.978   5.147    94   13.7  19:20 ( 27, 58)  
Mar.  9   5  6.30    6 51.8   5.153   5.208    87   13.8  19:26 ( 41, 55)  

* C/2021 G2 ( ATLAS )

Now it is 14.0 mag (Feb. 16, Hiroshi Abe). It stays 14 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  12 10.43  -38 28.8   4.493   5.194   130   13.9   1:31 (  0, 16)  
Mar.  9  12  8.17  -38  4.3   4.421   5.180   135   13.9   1:02 (  0, 17)  

* 32P/Comas Sola

Now it is 13.8 mag (Feb. 13, Chris Wyatt). It stays 15 mag for a while. In the Northern Hemisphere, it stays observable in good condition. 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)  
Mar.  2   3 45.61   25 37.1   2.031   2.073    78   14.0  19:20 ( 82, 60)  
Mar.  9   3 58.81   26 28.3   2.090   2.060    74   14.0  19:26 ( 87, 56)  

* C/2019 U5 ( PanSTARRS )

Now it is 13.9 mag (Feb. 2, 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)  
Mar.  2   8  8.13  -44 10.4   4.164   4.694   116   14.0  21:24 (  0, 11)  
Mar.  9   7 57.41  -43 13.4   4.235   4.731   114   14.1  20:46 (  0, 12)  

* C/2021 T4 ( Lemmon )

It brightened up to 7.8 mag in late July (July 20, Thomas Lehmann). Now it is 15.8 mag (Feb. 21, Thomas Lehmann). Fading gradually. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  14 25.97    8 59.5   2.432   3.130   127   14.4   3:47 (  0, 64)  
Mar.  9  14 12.68   11 18.2   2.408   3.200   136   14.5   3:06 (  0, 66)  

* C/2019 L3 ( ATLAS )

It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 14.0 mag (Feb. 16, G. Duszanowicz). 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)  
Mar.  2  11  4.07  -54  7.0   6.898   7.423   118   14.5   0:25 (  0,  1)  
Mar.  9  10 59.55  -54  7.1   6.905   7.469   121   14.5  23:49 (  0,  1)  

* 46P/Wirtanen

The condition is bad in this apparition. It brightens up to 10 mag in early summer, however, it is not observable at all. Brightening rapidly. It will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  23 57.28   -7 52.3   2.385   1.460    16   15.1  19:20 ( 84, -5)  
Mar.  9   0 16.30   -5 29.0   2.342   1.403    14   14.6  19:26 ( 88, -7)  

* 479P/2023 WM26 ( Elenin )

First return of a new periodic comet which was discovered in 2011, half a year after the perihelion passage. Now it is 14.6 mag (Feb. 18, Ken-ichi Kadota). It stays 15 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   7 46.38    2 35.6   0.644   1.509   133   14.8  21:04 (  0, 57)  
Mar.  9   7 42.15    0 35.8   0.636   1.460   125   14.7  20:32 (  0, 55)  

* C/2023 V4 ( Camarasa-Duszanowicz )

It is expected to brighten up to 12 mag in early summer. Now it is 14.8 mag (Feb. 24, ATLAS South Africa). Brightening gradually. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, 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)  
Mar.  2   2 15.30   -4 52.2   2.236   1.780    50   15.0  19:20 ( 65, 24)  
Mar.  9   2 21.14   -1  3.7   2.238   1.703    45   14.8  19:26 ( 73, 21)  

* 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 14.5 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). Fading rapidly. 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)  
Mar.  2   7 59.85   -2 52.0   1.208   2.040   135   14.8  21:18 (  0, 52)  
Mar.  9   8  1.57   -1 26.6   1.315   2.101   130   15.2  20:52 (  0, 54)  

* C/2023 S3 ( Lemmon )

It must have brightened up to 11 mag in winter. However, it was too low to observe at the high light. Now it is 13.7 mag (Feb. 19, Michael Mattiazzo). Fading rapidly. It will be fainter than 18 mag in April. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  19 33.75  -29 45.4   1.434   1.128    51   14.9   5:04 (312,  5)  
Mar.  9  19 19.00  -27 50.4   1.320   1.211    61   15.6   4:55 (317, 12)  

* C/2023 C2 ( ATLAS )

It is expected to brighten up to 12.5 mag in summer. Now it is 15.8 mag (Feb. 7, Thomas Lehmann). 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)  
Mar.  2  16  6.01  -69 44.7   3.559   3.647    87   15.4   5:04 (358,-15)  
Mar.  9  16 17.92  -70 52.4   3.444   3.594    90   15.2   4:55 (359,-16)  

* C/2020 K1 ( PanSTARRS )

It brightened up to 12.1 mag in 2023 spring (May 20, Jose Guilherme de S. Aguiar). Now it is 15.0 mag (Feb. 13, 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)  
Mar.  2   4  8.73  -62  6.0   4.263   4.181    78   15.3  19:20 ( 13,-10)  
Mar.  9   4 15.50  -59 41.3   4.313   4.224    78   15.4  19:26 ( 17, -9)  

* C/2024 C4 ( ATLAS )

Now it is 15.7 mag (Feb. 16, Taras Prystavski). It will fade out rapidly after this. It will be fainter than 18 mag in June. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  17  5.96  -39 42.6   1.314   1.542    82   15.5   5:04 (344, 13)  
Mar.  9  17  6.43  -35  4.5   1.224   1.573    89   15.4   4:55 (346, 18)  

* 227P/Catalina-LINEAR

Now it is 14.7 mag (Feb. 12, Yukihiro Sugiyama). It will fade out rapidly after this. 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. But it will become high in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   7 37.09   36 23.9   0.823   1.625   126   15.5  20:56 (180, 89)  
Mar.  9   7 45.65   35 10.7   0.859   1.624   122   15.5  20:37 (180, 90)  

* 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 15.0 mag (Feb. 16, Hiroshi Abe). 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)  
Mar.  2  17 40.15   22 37.7   6.643   6.575    81   15.5   5:04 (288, 62)  
Mar.  9  17 42.71   23 31.4   6.607   6.615    86   15.6   4:55 (291, 65)  

* 65P/Gunn

It will be observable at 15-16 mag from 2024 to 2025. Now it is 17.0 mag (Feb. 20, ATLAS-HKO, Haleakala). It stays 16 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  13 16.11    2 31.9   2.782   3.629   143   15.8   2:37 (  0, 57)  
Mar.  9  13 13.29    2 54.9   2.712   3.614   151   15.7   2:07 (  0, 58)  

* 125P/Spacewatch

It is expected to brighten up to 15.5 mag from March to April. Now it is 16.8 mag (Feb. 12, ATLAS-HKO, Haleakala). Fading 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)  
Mar.  2  18 17.15  -13 53.8   1.599   1.528    67   15.9   5:04 (316, 29)  
Mar.  9  18 38.28  -13 21.5   1.560   1.527    69   15.8   4:55 (315, 29)  

* C/2022 QE78 ( ATLAS )

Now it is 15.9 mag (Feb. 19, ATLAS Chile). It stays 16 mag for a while. It will be getting lower gradually after this, and it will be unobservable in May in the Northern Hemisphere, or in June in the Southern Hemisphere. But it will be observable again in June in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   4 31.34   -6 14.5   6.826   6.797    84   15.8  19:20 ( 32, 44)  
Mar.  9   4 33.21   -5 31.1   6.897   6.768    78   15.8  19:26 ( 42, 40)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.8 mag (Feb. 8, Thomas Lehmann). 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)  
Mar.  2   2 56.97  -62 52.8  16.936  16.636    70   15.9  19:20 ( 20,-15)  
Mar.  9   2 59.13  -62 36.0  16.914  16.611    70   15.8  19:26 ( 23,-17)  

* 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 17.0 mag (Feb. 13, ATLAS South Africa). It will fade out rapidly after this. It will be fainter than 18 mag in May. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition. Thomas Lehmann reported it was bright as 14.1 mag on Feb. 4.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   8 50.92  -51 19.8   2.534   3.099   115   15.9  22:07 (  0,  4)  
Mar.  9   8 37.03  -48 54.5   2.625   3.190   116   16.1  21:26 (  0,  6)  

* 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). Fading gradually. 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)  
Mar.  2   0 27.60  -44 19.6   2.820   2.195    42   16.0  19:20 ( 49,-19)  
Mar.  9   0 37.37  -44 44.1   2.893   2.283    43   16.2  19:26 ( 51,-23)  

* C/2022 S4 ( Lemmon )

Now it is 16.1 mag (Feb. 22, ATLAS Chile). It stays 16 mag for a while. It stays extremely low in the Northern Hemisphere. It locates somewhat low in the Southern Hemisphere. But it will become high in summer. The brightness evolution is slower than originally expected.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   1 53.81  -30 47.7   3.671   3.105    48   16.0  19:20 ( 49,  2)  
Mar.  9   1 58.88  -30 54.2   3.678   3.074    46   16.0  19:26 ( 53, -2)  

* C/2022 T1 ( Lemmon )

Now it is 16.4 mag (Feb. 12, Ken-ichi Kadota). 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)  
Mar.  2  14 13.19  -28 49.5   2.848   3.447   119   16.3   3:34 (  0, 26)  
Mar.  9  14 14.85  -28 43.9   2.771   3.450   126   16.3   3:08 (  0, 26)  

* C/2023 F3 ( ATLAS )

Now it is 17.4 mag (Feb. 20, ATLAS Chile). 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)  
Mar.  2  16 50.76  -47 26.0   5.778   5.775    84   16.4   5:04 (349,  6)  
Mar.  9  16 47.20  -48 12.1   5.636   5.753    91   16.4   4:55 (352,  6)  

* 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)  
Mar.  2  16 36.74  -47 46.1   3.893   3.969    87   16.4   5:04 (351,  6)  
Mar.  9  16 36.30  -47 37.9   3.843   4.029    93   16.4   4:55 (354,  7)  

* 150P/LONEOS

Now it is 15.8 mag (Feb. 13, Yukihiro Sugiyama). Fading gradually. 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)  
Mar.  2   8 38.22  -16 29.4   0.873   1.749   139   16.5  21:55 (  0, 38)  
Mar.  9   8 37.28  -16 40.3   0.897   1.746   134   16.6  21:27 (  0, 38)  

* 226P/Pigott-LINEAR-Kowalski

Now it is 16.1 mag (Feb. 11, ATLAS-MLO, Mauna Loa). 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 soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   2  9.88   21 34.0   2.233   1.876    56   16.5  19:20 ( 92, 38)  
Mar.  9   2 22.25   24 14.4   2.318   1.898    53   16.7  19:26 ( 97, 35)  

* C/2024 A2 ( ATLAS )

Now it is 17.2 mag (Feb. 24, ATLAS Chile). Fading slowly. In the Northern Hemisphere, it is not observable now, but it will be observable soon. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in June. But it will be observable again in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   6 20.35  -74 33.7   1.768   2.008    88   16.8  19:34 (  0,-19)  
Mar.  9   5 51.06  -67 11.2   1.730   1.980    89   16.7  19:26 (  5,-12)  

* 130P/McNaught-Hughes

It will brighten up to 15 mag from summer to autumn. Brightening slowly. In the Northern Hemisphere, it is not observable now, but it will appear in April. 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)  
Mar.  2  20 57.25  -20 23.1   2.643   1.862    30   16.8   5:04 (293, -3)  
Mar.  9  21 16.06  -19 15.3   2.600   1.850    33   16.7   4:55 (292, -2)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 17.0 mag (Jan. 27, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   2 13.67  -67 43.4  10.640  10.329    69   16.8  19:20 ( 20,-21)  
Mar.  9   2 15.41  -67  0.6  10.638  10.331    69   16.8  19:26 ( 23,-23)  

* C/2022 U3 ( Bok )

Now it is 17.0 mag (Feb. 24, D. Buczynski). 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)  
Mar.  2   4 42.18   27 59.0   4.843   4.964    91   16.9  19:20 ( 73, 72)  
Mar.  9   4 45.81   27 28.7   4.938   4.952    84   16.9  19:26 ( 80, 66)  

* 30P/Reinmuth 1

Now it is 17.0 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). Brightening slowly. It will be unobservable in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   2 25.01    8  7.2   2.749   2.332    55   17.0  19:20 ( 75, 34)  
Mar.  9   2 35.81    9 19.0   2.785   2.297    51   16.9  19:26 ( 80, 30)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.9 mag (Feb. 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)  
Mar.  2   4 48.70  -34  1.2   7.507   7.491    85   17.0  19:20 ( 16, 19)  
Mar.  9   4 50.67  -33  8.5   7.546   7.470    81   17.0  19:26 ( 23, 18)  

* C/2021 S4 ( Tsuchinshan )

Now it is 16.8 mag (Feb. 22, ATLAS-HKO, Haleakala). It stays 17 mag for a while. It will be unobservable in April in the Southern Hemisphere, or in June in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   4 38.25   39 38.0   6.593   6.700    91   17.1  19:20 (112, 73)  
Mar.  9   4 41.30   39 28.1   6.702   6.703    85   17.2  19:26 (110, 67)  

* 471P/2023 KF3

Now it is 16.8 mag (Feb. 16, Catalina Sky Survey). It will fade out rapidly after this. It will be fainter than 18 mag in April. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will be unobservable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   1 39.73   13 46.6   2.789   2.228    46   17.2  19:20 ( 88, 28)  
Mar.  9   1 54.50   14 58.5   2.864   2.248    43   17.3  19:26 ( 92, 25)  

* 299P/Catalina-PanSTARRS

Now it is 17.1 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). 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)  
Mar.  2  15 52.23  -29  2.0   2.855   3.171    99   17.3   5:04 (358, 26)  
Mar.  9  15 56.56  -29 20.4   2.758   3.168   105   17.2   4:49 (  0, 26)  

* 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. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  14 25.29   25 11.6   2.192   2.889   126   17.2   3:46 (  0, 80)  
Mar.  9  14 11.34   29 12.2   2.184   2.944   132   17.3   3:05 (  0, 84)  

* C/2023 T3 ( Fuls )

Now it is 17.1 mag (Feb. 13, Ken-ichi Kadota). It stays 17 mag for a while. In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in June. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   7 44.46   -8 44.8   3.892   4.599   130   17.3  21:02 (  0, 46)  
Mar.  9   7 43.18   -8 23.9   3.920   4.561   124   17.3  20:33 (  0, 47)  

* C/2023 H5 ( Lemmon )

Now it is 17.1 mag (Feb. 20, ATLAS South Africa). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  10 41.38    6 58.2   4.826   5.816   177   17.4   0:03 (  0, 62)  
Mar.  9  10 36.68    8 12.9   4.803   5.781   169   17.3  23:26 (  0, 63)  

* 478P/2023 Y3 ( ATLAS )

Now it is 18.0 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). 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)  
Mar.  2   6 47.80   21 21.9   1.779   2.426   119   17.4  20:06 (  0, 76)  
Mar.  9   6 51.15   21 57.8   1.849   2.419   113   17.4  19:42 (  0, 77)  

* C/2022 A3 ( Lemmon-ATLAS )

Now it is 17.6 mag (Feb. 5, ATLAS South Africa). 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)  
Mar.  2   4 37.85  -67 42.8   3.965   3.951    81   17.5  19:20 (  8,-14)  
Mar.  9   4 28.54  -66 17.1   4.007   3.973    80   17.6  19:26 ( 13,-14)  

* C/2024 A1 ( ATLAS )

Now it is 17.5 mag (Feb. 9, Jean-Claude Merlin). It stays 17 mag for a while. In the Northern Hemisphere, it will be unobservable soon. In the Southern Hemisphere, it stays observable in good condition. 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)  
Mar.  2   6  3.58  -55 34.6   5.378   5.535    93   17.6  19:21 (  0,  0)  
Mar.  9   6  2.02  -53 46.2   5.357   5.496    92   17.5  19:26 (  5,  1)  

* C/2020 F2 ( ATLAS )

Now it is 17.7 mag (Feb. 18, Ken-ichi Kadota). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2  12  5.37   18 58.8   8.533   9.463   158   17.6   1:26 (  0, 74)  
Mar.  9  12  0.99   19 31.1   8.530   9.478   161   17.6   0:55 (  0, 74)  

* 216P/LINEAR

Now it is 18.3 mag (Feb. 12, Toshihiko Ikemura, Hirohisa Sato). It will fade out rapidly after this. 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)  
Mar.  2  12  8.03    1 25.3   1.212   2.171   160   17.6   1:29 (  0, 56)  
Mar.  9  12  2.99    1 12.6   1.201   2.182   168   17.6   0:57 (  0, 56)  

* 362P/(457175) 2008 GO98

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)  
Mar.  2  15 26.81  -11 41.9   2.485   2.961   109   18.0   4:47 (  0, 43)  
Mar.  9  15 30.38  -11 10.5   2.388   2.952   115   17.8   4:23 (  0, 44)  

* 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 17.7 mag (Feb. 7, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag soon. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   3  1.57  -51 16.3   5.529   5.228    67   17.9  19:20 ( 27, -5)  
Mar.  9   3  3.53  -50 20.5   5.626   5.294    65   18.0  19:26 ( 31, -7)  

* 170P/Christensen

Now it is 17.2 mag (Feb. 11, ATLAS Chile). Fading slowly. In the Northern Hemisphere, it will be getting lower gradually. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar.  2   3 45.46   10 25.8   3.491   3.375    75   17.9  19:20 ( 60, 51)  
Mar.  9   3 52.03   11  6.6   3.602   3.392    69   18.0  19:26 ( 67, 46)  

* C/2022 V2 ( Lemmon )

Now it is 17.2 mag (Feb. 11, ATLAS South Africa). Fading gradually. 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)  
Mar.  2   7 49.30  -35 55.1   1.845   2.484   119   17.9  21:05 (  0, 19)  
Mar.  9   7 31.31  -35  9.1   1.959   2.528   113   18.1  20:20 (  0, 20)  

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