Weekly Information about Bright Comets (2022 Mar. 12: North)

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Updated on March 14, 2022
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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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* 19P/Borrelly

Now it is bright as 9.7 mag (Mar. 6, Marco Goiato). It stays bright as 9-10 mag until March. In the Northern Hemisphere, it stays observable in excellent condition for a long time. In the Southern Hemisphere, it stays extremely low after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   3 14.82   28 29.0   1.508   1.383    63    9.9  19:28 ( 97, 45)  
Mar. 19   3 37.84   31 45.5   1.567   1.413    62   10.2  19:34 (103, 44)  

* C/2019 L3 ( ATLAS )

Now it is 9.9 mag (Mar. 9, Osamu Miyazaki). In the Northern Hemisphere, it will be getting lower after this, and it will be unobservable in May. In the Southern Hemisphere, it stays observable until July.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6 35.26   19 34.1   3.177   3.598   107   10.4  19:28 ( 11, 74)  
Mar. 19   6 37.05   18 29.5   3.289   3.609   100   10.4  19:34 ( 33, 71)  

* C/2021 F1 ( Lemmon-PanSTARRS )

Brightened very rapidly. Now it is very bright as 10.0 mag (Mar. 9, Michael Jager). It stays 10-11 mag until spring. In the Northern Hemisphere, it is observable only until early March. In the Southern Hemisphere, it is not observable until late May. But it will be observable in good condition after that.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  23 38.47   38 26.0   1.600   1.089    42   10.5  19:28 (130, 10)  
Mar. 19   0  8.54   34 30.0   1.684   1.047    35   10.4  19:34 (128,  7)  

* C/2017 K2 ( PanSTARRS )

Now it is bright as 11.0 mag (Mar. 6, Osamu Miyazaki). The brightness evolution is slower than originally expected. It is expected to be observable at 7 mag for a long time from 2022 to 2023. In the Northern Hemisphere, it stays observable in good condition until autumn. However, it is not observable at the high light from autumn to 2023 summer. In the Southern Hemisphere, it stays observable in good condition after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  18 47.10   11 22.0   3.965   3.764    71   10.9   4:51 (293, 47)  
Mar. 19  18 50.14   11 26.3   3.811   3.701    76   10.7   4:41 (297, 50)  

* 22P/Kopff

Now it is 12.0 mag (Feb. 23, Thomas Lehmann). In the Northern Hemisphere, it stays extremely low until spring. In the Southern Hemisphere, it stays observable at 11 mag until June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  20 34.92  -17 23.9   2.099   1.554    44   10.9   4:51 (298,  8)  
Mar. 19  20 56.67  -16 13.8   2.068   1.552    46   10.9   4:41 (296,  8)  

* C/2021 O3 ( PanSTARRS )

It brightened up to 15.1 mag in February (Feb. 1, Ken-ichi Kadota). Now it is not observable. It is expected to brighten up to 4.5 mag in April. However, it is not observable at the high light. In the Northern Hemisphere, it will appear at 6 mag in mid May, and it stays observable in good condition after that while the comet will be fading. In the Southern Hemisphere, it is not observable until August.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   0  5.48   -0 30.5   2.038   1.074    10   11.9  19:28 ( 96, -9)  
Mar. 19   0 24.42   -0 41.9   1.906   0.930     7   11.1  19:34 ( 98,-12)  

* C/2019 T4 ( ATLAS )

Now it is bright as 11.8 mag (Mar. 7, Marco Goiato). It will brighten up to 11.5 mag in spring. It stas observable in good condition for a long time. In the Northern Hemisphere, it stays somewhat low until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  11 59.34  -25 22.8   3.417   4.307   150   11.6   0:43 (  0, 29)  
Mar. 19  11 56.53  -24  7.5   3.374   4.297   155   11.5   0:13 (  0, 31)  

* C/2021 A1 ( Leonard )

It brightened up to 3 mag from mid December to late December. Now it is fading. It has already faded down to 11.0 mag (Feb. 23, Martin Masek). In the Northern Hemisphere, it will become observable again at 13 mag in late April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  21 18.06  -34 51.4   2.013   1.459    43   11.7   4:51 (305,-10)  
Mar. 19  21 13.92  -34 57.6   2.000   1.565    50   12.0   4:41 (308, -7)  

* 104P/Kowal 2

It brightened very rapidly up to 9.2 mag in winter (Jan. 31, Chris Wyatt). Now it is fading. But it is still bright as 11.3 mag (Mar. 9, Osamu Miyazaki). It will be fainter than 18 mag in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   5 37.03   14 28.8   0.824   1.327    93   11.7  19:28 ( 41, 64)  
Mar. 19   6  7.34   15 10.7   0.892   1.379    93   12.4  19:34 ( 44, 64)  

* 9P/Tempel 1

Now it is 14.7 mag (Feb. 3, Giuseppe Pappa). It stays 12-13 mag for a while. But actually, it is fainter than this ephemeris recently. It is observable in excellent condition in the Southern Hemisphere. It locates low until May in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  19 16.49  -22 54.2   1.707   1.546    63   12.1   4:51 (315, 17)  
Mar. 19  19 38.32  -22 54.8   1.670   1.550    65   12.1   4:41 (314, 16)  

* 67P/Churyumov-Gerasimenko

It brightened up to 8.5 mag from autumn to winter (Dec. 2, Toshihiko Ikemura, Hirohisa Sato). Now it is fading. It has already faded down to 11.8 mag (Mar. 9, Osamu Miyazaki). It stays observable in good condition for a long time. It locates somewhat low in the Southern Hemisphere,

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   8 27.77   25 35.7   1.124   1.933   131   12.7  21:08 (  0, 80)  
Mar. 19   8 32.22   24 50.2   1.233   1.988   125   13.1  20:45 (  0, 80)  

* C/2021 E3 ( ZTF )

Now it is 14.9 mag (Nov. 28, Thomas Lehmann). It is expected to brighten up to 11 mag from spring to summer. In the Southen Hemisphere, it stays observable in good condition for a long time after this. In the Northern Hemisphere, it is hardly observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  20 26.30  -20  0.0   2.675   2.126    47   13.4   4:51 (301,  8)  
Mar. 19  20 34.05  -21 53.0   2.526   2.080    52   13.2   4:41 (304,  8)  

* C/2020 Y2 ( ATLAS )

Now it is 15.7 mag (Feb. 21, P. Camilleri, J. Oey, R. Groom, A. Pearce). It was expected to brighten up to 13 mag in spring. But actually, it is fainter than this ephemeris recently. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it is not observable until autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   8 29.49  -69  5.4   2.928   3.272   101   13.5  21:06 (  0,-14)  
Mar. 19   7 54.60  -67 13.6   2.920   3.253   100   13.4  20:04 (  0,-12)  

* 116P/Wild 4

Now it is 12.7 mag (Feb. 27, Jose Guilherme de S. Aguiar). It is observable at 13 mag in good condition until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   9 29.53   19 28.2   1.470   2.367   147   13.7  22:09 (  0, 74)  
Mar. 19   9 26.54   19 25.5   1.502   2.350   139   13.7  21:39 (  0, 74)  

* 29P/Schwassmann-Wachmann 1

Now it is bright as 12.7 mag (Feb. 27, Toshihiko Ikemura, Hirohisa Sato). It is observable until April in the Southern Hemisphere, or until May in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   4 24.84   29  9.4   6.089   5.966    78   13.7  19:28 ( 89, 59)  
Mar. 19   4 28.28   29  6.1   6.199   5.968    72   13.8  19:34 ( 93, 53)  

* C/2020 V2 ( ZTF )

Now it is 13.4 mag (Feb. 28, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 10 mag in 2023. In the Northern Hemisphere, it stays observable in good condition until 2023 autumn. In the Southern Hemipshere, it stays unobservable until 2023 summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  12 10.63   58 10.9   4.297   4.930   124   14.1   0:55 (180, 67)  
Mar. 19  11 56.57   59 23.7   4.280   4.873   121   14.0   0:13 (180, 66)  

* C/2019 U5 ( PanSTARRS )

Now it is 14.1 mag (Mar. 2, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 11 mag in 2023. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it locates extremely low in 2022, but it will be observable in good condition in 2023.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  16 32.51   37 48.8   4.621   4.940   102   14.2   4:51 (239, 84)  
Mar. 19  16 27.14   38 53.0   4.516   4.901   107   14.1   4:41 (183, 86)  

* C/2020 J1 ( SONEAR )

It brightened up to 12.3 mag from spring to summer (June 15, Marco Goiato). Now it is fading. It has already faded down to 14.7 mag (Feb. 27, Toshihiko Ikemura, Hirohisa Sato).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  13 50.38   21  4.0   3.676   4.493   141   14.1   2:34 (  0, 76)  
Mar. 19  13 41.25   22 58.3   3.677   4.533   145   14.2   1:57 (  0, 78)  

* 117P/Helin-Roman-Alu 1

Now it is 15.3 mag (Feb. 23, Thomas Lehmann). It will brighten up to 13 mag in summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  18 24.32  -26  1.3   3.188   3.095    75   14.4   4:51 (327, 21)  
Mar. 19  18 32.53  -26 12.9   3.088   3.089    80   14.3   4:41 (329, 22)  

* C/2020 R7 ( ATLAS )

Now it is 15.7 mag (Feb. 2, Thomas Lehmann). It will brighten up to 12.5 mag in summer. In the Southern Hemisphere, it stays observable in excellent condition for a long time, although it became low temporarily in February. In the Northern Hemisphere, it is not observable until August.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  22 40.04  -54 45.9   4.011   3.490    52   14.4   4:51 (317,-32)  
Mar. 19  22 42.78  -54 22.5   3.920   3.455    55   14.4   4:41 (318,-30)  

* 45P/Honda-Mrkos-Pajdusakova

It has not been observed yet in this apparition. It will brighten very rapidly up to 9 mag in May. The condition is very bad in this apparition. It is observable only in the extremely low sky from mid May to mid July in the Northern Hemisphere, or from early June to early August in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  22 41.76  -10 18.1   1.958   1.016    13   15.8   4:51 (274,-13)  
Mar. 19  23 11.27   -7 19.3   1.866   0.918    12   14.7   4:41 (270,-13)  

* C/2021 P4 ( ATLAS )

Now it is 14.6 mag (Feb. 28, Thomas Lehmann). It is expected to brighten up to 11 mag in summer. In the Northern Hemisphere, it stays observable in good condition until June when it brightens up to 11 mag. But it is not observable after the high light. In the Souther Hemisphere, it is not observable until October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   0 25.05   53 26.7   2.726   2.359    58   14.9  19:28 (139, 25)  
Mar. 19   0 43.15   54 20.4   2.678   2.278    56   14.7  19:34 (142, 23)  

* C/2020 M5 ( ATLAS )

Now it is 14.3 mag (Mar. 2, Toshihiko Ikemura, Hirohisa Sato). It became brighter after the perihelion passage. It stays observable at 14-15 mag for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  11 46.05    9 45.2   2.618   3.605   172   14.8   0:30 (  0, 65)  
Mar. 19  11 33.04    9 10.9   2.657   3.642   170   14.9  23:44 (  0, 64)  

* 4P/Faye

It brightened up to 10.6 mag in autumn (Oct. 10, Osamu Miyazaki). Now it is fading. It has already faded down to 13.7 mag (Feb. 26, Toshihiko Ikemura, Hirohisa Sato). It stays observable in good condition for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6 39.68   13 32.2   1.879   2.387   108   14.8  19:28 (  5, 68)  
Mar. 19   6 46.54   13 57.2   2.001   2.430   103   15.1  19:34 ( 22, 68)  

* C/2020 K1 ( PanSTARRS )

Now it is 15.2 mag (Mar. 2, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 11 mag in 2023. In the Northern Hemisphere, it stays observable in good condition until November. But it becomes unobservable after that. In the Southern Hemisphere, it stays observable in good condition after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  18 57.41   17 36.0   5.250   4.994    69   15.0   4:51 (284, 49)  
Mar. 19  18 59.64   17 46.4   5.121   4.947    74   14.9   4:41 (287, 52)  

* C/2018 U1 ( Lemmon )

Now it is 15.8 mag (Feb. 20, J. L. Virlichie, P. Traverse, H. Roy). It stays at 15-16 mag for a long time. In the Southern Hemisphere, it stays observable in excellent condition for a long time. In the Northern Hemiphere, it locates extremely low in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  17 19.83  -38 56.5   5.006   5.090    89   15.1   4:51 (346, 14)  
Mar. 19  17 17.79  -40  8.6   4.897   5.101    96   15.0   4:41 (350, 14)  

* C/2021 U5 ( Catalina )

Now it is 15.3 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It continues brightening even after the perihelion passage. It is observable at 15 mag in good condition for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  10 17.07  -13 33.4   1.474   2.414   155   15.2  22:57 (  0, 42)  
Mar. 19  10 17.23  -10 30.2   1.499   2.431   153   15.2  22:30 (  0, 45)  

* C/2020 T2 ( Palomar )

It brightened up to 9.5 mag in early summer in 2021 (June 27, Marco Goiato). Now it is fading. It has faded down to 12.7 mag in autumn (Nov. 22, Thomas Lehmann). In the Southern Hemisphere, it is appearing in the morning sky. In the Northern Hemisphere, it is not observable until June when the comet will fade down to 17 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  21 47.32  -31 17.8   4.184   3.435    36   15.6   4:51 (299,-13)  
Mar. 19  21 57.73  -31  5.3   4.186   3.493    40   15.7   4:41 (300,-12)  

* C/2020 PV6 ( PanSTARRS )

Now it is 16.2 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this. In the Northern Hemisphere, it stays observable in good condition for a long time. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  14 50.67   40 38.2   2.275   2.916   121   15.7   3:34 (180, 85)  
Mar. 19  14 27.56   42 44.4   2.269   2.961   125   15.8   2:44 (180, 82)  

* 73P/Schwassmann-Wachmann 3

Now it is 16.9 mag (Mar. 2, K. Sarneczky). It is expected to brighten up to 11 mag from summer to autumn. It stays observable in good condition in the Southern Hemisphere. In the Northern Hemisphere, it becomes extremely low from August to September.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  10 16.07   31 12.0   1.332   2.235   147   16.1  22:55 (  0, 86)  
Mar. 19  10  6.08   31 45.6   1.316   2.176   140   15.9  22:18 (  0, 87)  

* 70P/Kojima

Now it is 16.0 mag (Mar. 9, Toshihiko Ikemura, Hirohisa Sato). It is bright as 14.8 mag visually (Mar. 1, Sandor Szabo). It will be fading after this, and it will be fainter than 18 mag in June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  11 38.39   12 20.9   1.271   2.257   170   15.9   0:22 (  0, 67)  
Mar. 19  11 33.76   13  1.4   1.301   2.282   166   16.0  23:45 (  0, 68)  

* C/2020 H6 ( ATLAS )

Now it is 15.9 mag (Mar. 6, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 16 mag from 2021 to 2022.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  16 20.23   24 55.7   4.495   4.874   106   16.1   4:51 (345, 80)  
Mar. 19  16 20.67   26 50.2   4.446   4.889   110   16.1   4:36 (  0, 82)  

* 110P/Hartley 3

It brightened rapidly. Now it is 15.8 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It stays observable in good condition for a while. But it will fade out rapidly after this, and it will be fainter than 18 mag in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   7 51.53   13 14.8   1.899   2.609   125   16.2  20:32 (  0, 68)  
Mar. 19   7 53.08   13  2.4   1.987   2.623   119   16.4  20:06 (  0, 68)  

* 325P/Yang-Gao

Now it is 19.2 mag (Feb. 28, Hidetaka Sato). It was expected to be observable at 16 mag in good condition in spring. But actually, it is fainter than predicted by 3 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  18 12.78  -32 28.1   1.266   1.445    78   16.4   4:51 (333, 16)  
Mar. 19  18 37.69  -30 57.6   1.223   1.437    80   16.3   4:41 (331, 17)  

* 402P/2020 Q3 ( LINEAR )

First return of a new periodic comet observed at 16 mag from 2003 to 2004. Now it is 16.3 mag (Feb. 26, Toshihiko Ikemura, Hirohisa Sato). It stays 16 mag until March, and it stays observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6  4.59   12 27.6   3.677   3.970    99   16.3  19:28 ( 26, 66)  
Mar. 19   6  7.60   13 17.3   3.784   3.975    93   16.4  19:34 ( 42, 63)  

* C/2020 O2 ( Amaral )

Now it is 16.3 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It was observed at 15 mag in 2021. Now it is fading. It stays observable at 16-17 mag for a while in 2022.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  18 40.15    8 27.8   5.303   5.094    72   16.6   4:51 (298, 46)  
Mar. 19  18 42.77    9 53.8   5.227   5.111    77   16.6   4:41 (301, 50)  

* 81P/Wild 2

Now it is 17.0 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 11.5 mag in 2022 winter. It stays observable while the comet will be brightening slowly.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   3 28.95   16 12.4   3.197   2.883    62   16.8  19:28 ( 80, 42)  
Mar. 19   3 36.71   16 46.3   3.245   2.843    57   16.7  19:34 ( 85, 37)  

* C/2020 S4 ( PanSTARRS )

Now it is 16.9 mag (Mar. 1, M. Iozzi). It will brighten up to 14 mag in early 2023. It stays observable in good condition until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   4 29.07    8 57.5   4.673   4.540    76   16.7  19:28 ( 59, 49)  
Mar. 19   4 33.19    9 37.8   4.733   4.500    70   16.7  19:34 ( 67, 44)  

* P/2021 N2 ( Fuls )

Brightened rapidly. Now it is 16.5 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It becomes too low to observe in mid March in the Southern Hemisphere, or in mid April in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   2 55.72   13 23.8   4.354   3.861    54   16.7  19:28 ( 83, 34)  
Mar. 19   3  3.33   13 47.3   4.443   3.869    49   16.8  19:34 ( 87, 29)  

* C/2020 F7 ( Lemmon )

Now it is 17.2 mag (Jan. 18, J. Drummond). It brightened rapidly. It stays 17 mag for a long time from 2021 to 2022. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it locates extremely low, and it is observable only until April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6 56.42  -45 46.5   5.097   5.403   102   16.9  19:36 (  0,  9)  
Mar. 19   6 51.15  -45 11.2   5.155   5.412    99   16.9  19:34 (  6, 10)  

* 430P/2021 Q2 ( Scotti )

First return of a new periodic comet which brightened up to 17 mag in 2011. Now it is extremely faint as 20.4 mag (Feb. 4, J.-G. Bosch, F. Kugel, A. Klotz, J. Nicolas). It brightened up to 16.8 mag in October (Oct. 10, Ken-ichi Kadota), however, it has been fading after that.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  15 30.48  -15 20.9   1.139   1.819   116   16.9   4:13 (  0, 40)  
Mar. 19  15 33.06  -15 42.4   1.109   1.852   123   16.9   3:49 (  0, 39)  

* 152P/Helin-Lawrence

It will brighten up to 16 mag from spring to summer. It locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  19  3.55  -21 57.7   3.373   3.111    66   17.0   4:51 (317, 20)  
Mar. 19  19 12.31  -21 56.4   3.287   3.115    71   16.9   4:41 (319, 21)  

* C/2019 O3 ( Palomar )

Now it is 16.9 mag (Mar. 6, Toshihiko Ikemura, Hirohisa Sato). Fading slowly. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it is not observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  19 21.40   54 44.0   9.246   9.074    76   16.9   4:51 (224, 52)  
Mar. 19  19 23.06   55 44.6   9.235   9.084    78   17.0   4:41 (221, 54)  

* C/2020 F2 ( ATLAS )

Now it is 16.9 mag (Feb. 28, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 17-18 mag for a long time until 2024.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  14 23.92   -1 47.4   8.111   8.847   135   17.0   3:07 (  0, 53)  
Mar. 19  14 20.23   -1 14.8   8.028   8.844   143   17.0   2:36 (  0, 54)  

* 8P/Tuttle

It brightened very rapidly, and brightened up to 8.9 mag (Sept. 11, Chris Wyatt). Now it is fading. It has already faded down to 18.5 mag (Feb. 11, J. L. Virlichie, P. Traverse, H. Roy). In the Southern Hemisphere, it stays observable after this while the comet will be fading. It is not observable after this in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  17 57.38  -55 59.1   2.662   2.723    82   17.0   4:51 (345, -4)  
Mar. 19  17 59.83  -56 17.4   2.634   2.789    88   17.2   4:41 (347, -3)  

* 99P/Kowal 1

Now it is 16.5 mag (Feb. 28, Toshihiko Ikemura, Hirohisa Sato). It will be observable at 17 mag in good condition in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  13 40.36   -9 35.1   3.865   4.708   144   17.1   2:24 (  0, 45)  
Mar. 19  13 37.97   -9 25.1   3.805   4.707   151   17.1   1:54 (  0, 45)  

* 132P/Helin-Roman-Alu 2

It brightened up to 13.1 mag in autumn (Oct. 28, Toshihiko Ikemura, Hirohisa Sato). Now it is fading. But it is still bright as 16.2 mag (Feb. 28, Toshihiko Ikemura, Hirohisa Sato). Sandor Szabo reported it is 15.0 mag visually on Mar. 1. It stays observable in good condition for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   4  1.26   15 26.4   2.149   2.042    70   17.1  19:28 ( 73, 48)  
Mar. 19   4 16.38   16 18.2   2.252   2.078    67   17.4  19:34 ( 78, 45)  

* C/2021 G2 ( ATLAS )

Now it is 16.9 mag (Mar. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 13-14 mag from 2024 to 2025.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   7  9.62  -29 33.8   7.909   8.304   110   17.2  19:50 (  0, 25)  
Mar. 19   7  9.35  -29  2.5   7.933   8.267   106   17.2  19:34 (  3, 26)  

* C/2020 U5 ( PanSTARRS )

Now it is 17.1 mag (Mar. 4, A. Diepvens). It started fading before the perihelion passage. It was predicted to stay at 16 mag for a long time, but actually, it will be fainter than 18 mag in autumn. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it is not observable until 2023.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  23 43.79   75 37.2   3.837   3.779    79   17.2  19:28 (164, 30)  
Mar. 19  23 50.81   75 12.3   3.888   3.773    75   17.2   4:41 (196, 29)  

* 52P/Harrington-Abell

It brightened up to 16.4 mag from autumn to winter (Oct. 6, ATLAS-MLO, Mauna Loa). Now it is fading. It has already faded down to 18.0 mag (Feb. 28, Toshihiko Ikemura, Hirohisa Sato).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  12 39.11  -13  2.6   1.338   2.280   155   17.4   1:23 (  0, 42)  
Mar. 19  12 32.55  -13  4.4   1.347   2.317   163   17.5   0:49 (  0, 42)  

* 254P/McNaught

Now it is 17.8 mag (Feb. 25, Catalina Sky Survey). It continued brightening for a while even after the perihelion passage. It stays observable at 17 mag in good condition for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   4 35.78   -2 43.8   4.210   4.103    77   17.5  19:28 ( 46, 41)  
Mar. 19   4 40.27   -1 42.2   4.322   4.121    71   17.5  19:34 ( 54, 38)  

* (3200) Phaethon

In the Northern Hemisphere, it is observable until April when it brightens up to 16 mag. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   2 25.50   18 18.0   1.796   1.368    49   17.6  19:28 ( 92, 30)  
Mar. 19   2 35.38   18 16.5   1.785   1.277    44   17.5  19:34 ( 95, 25)  

* C/2021 Y1 ( ATLAS )

Now it is 17.6 mag (Mar. 4, A. Diepvens). It is expected to brighten up to 12 mag from winter to summer in 2023. In the Northern Hemisphere, it stays observable in good condition until 2023 spring. In the Southern Hemisphere, it is not observable until summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   2  2.76   44 35.6   5.322   4.891    59   17.5  19:28 (123, 36)  
Mar. 19   2  9.63   43 58.8   5.347   4.832    54   17.5  19:34 (124, 32)  

* 274P/Tombaugh-Tenagra

Now it is 17.8 mag (Feb. 27, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17 mag from November to March. It is observable in good condition in the Northern Hemisphere, but it locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   5 43.58   32 19.5   2.161   2.461    95   17.6  19:28 ( 83, 77)  
Mar. 19   5 52.32   32 35.0   2.242   2.458    90   17.7  19:34 ( 89, 72)  

* C/2018 N2 ( ASASSN )

Now it is 17.8 mag (Mar. 2, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable for a long time while it is getting fainter slowly. It locates extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  14 42.26   46 11.3   7.388   7.932   120   17.6   3:25 (180, 79)  
Mar. 19  14 38.18   46 35.8   7.411   7.979   121   17.7   2:54 (180, 79)  

* A/2021 X1

Now it is 17.2 mag (Mar. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 15-16 mag in 2023. Cometary activity was detected by Cristovao Jacques on Dec. 12, and by Luca Buzzi and Andrea Aletti on Feb. 23.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6 33.77  -19 17.1   4.817   5.155   104   17.7  19:28 (  4, 36)  
Mar. 19   6 29.00  -18 17.5   4.869   5.109    98   17.7  19:34 ( 15, 35)  

* C/2020 U4 ( PanSTARRS )

Now it is 17.9 mag (Mar. 5, E. Bryssinck). It stays 17-18 mag for a long time from 2021 to 2022. It is observable in excellent condition in the Northern Hemisphere, In the Southern Hemisphere, it is not observable until June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   2 36.98   26 43.6   5.867   5.357    54   17.7  19:28 (100, 37)  
Mar. 19   2 37.25   26 36.7   5.969   5.356    48   17.7  19:34 (103, 30)  

* C/2017 Y2 ( PanSTARRS )

Now it is 17.1 mag (Feb. 28, Hidetaka Sato). It was observed at 16 mag from 2020 to 2021. Now it is fading. It will be fainter than 18 mag in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  15 23.82  -40 20.7   5.594   6.015   110   17.7   4:07 (  0, 15)  
Mar. 19  15 17.64  -40 56.7   5.521   6.048   117   17.7   3:34 (  0, 14)  

* C/2021 C5 ( PanSTARRS )

Now it is 17.4 mag (Mar. 3, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 16 mag in 2023. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it is observable only until May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  10  2.03  -16  9.8   3.594   4.490   151   17.8  22:41 (  0, 39)  
Mar. 19   9 56.43  -16 18.9   3.583   4.448   146   17.8  22:08 (  0, 39)  

* 440P/2021 W2 ( Kobayashi )

First return of a new periodic comet which brightened up to 16.5 mag in 1997. Now it is 17.7 mag (Feb. 27, Toshihiko Ikemura, Hirohisa Sato). It was fainter than originally predicted at the recovery, but it brightened very rapidly. It is observable in good condition from January to March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   8 25.17   20 55.6   1.259   2.065   132   17.8  21:06 (  0, 76)  
Mar. 19   8 27.86   19 38.4   1.306   2.059   126   17.8  20:41 (  0, 74)  

* P/2020 V4 ( Rankin )

Now it is 17.6 mag (Feb. 20, ATLAS-MLO, Mauna Loa). It will be fainter than 18 mag soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   7 37.45    5 29.3   4.683   5.286   122   17.8  20:18 (  0, 60)  
Mar. 19   7 37.65    5 49.6   4.780   5.294   116   17.9  19:50 (  0, 61)  

* C/2021 D2 ( ZTF )

Now it is 17.1 mag (Feb. 23, Thomas Lehmann). It was expected to brighten up to 15.5 mag in winter. But actually, it is fading even before the perihelion passage. In the Northern Hemisphere, it stays observable in good condition for a long time. It is not observable at all in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12   6 18.40   74 36.0   2.682   2.968    96   17.9  19:28 (177, 51)  
Mar. 19   6 23.72   70 50.2   2.750   2.978    93   18.0  19:34 (172, 54)  

* C/2019 T2 ( Lemmon )

Now it is 18.2 mag (Mar. 6, ATLAS Chile, Rio Hurtado). In the Southern Hemisphere, it stays observable for a long time. In the Northern Hemisphere, it is observable in low sky in spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  10  6.23  -46 17.9   3.520   4.194   127   18.5  22:45 (  0,  9)  
Mar. 19   9 57.69  -44  5.1   3.555   4.245   128   18.6  22:09 (  0, 11)  

* C/2021 O1 ( Nishimura )

Now it is 18.7 mag (Feb. 13, Giuseppe Pappa). It was observed at 9-10 mag from late July to early August. Although it had been unobservable for a long time, it is appearing in the morning sky now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Mar. 12  16 42.98  -30 15.4   2.996   3.281    97   19.6   4:51 (352, 24)  
Mar. 19  16 42.01  -30 54.5   2.969   3.362   104   19.8   4:41 (356, 24)  

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