Weekly Information about Bright Comets (2021 Feb. 27: North)

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Updated on March 3, 2021
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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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* P/1999 J6 = P/2004 V9 = P/2010 H3 ( SOHO )

Marsden group's comet. Three apparitions of this comet was confirmed in 1999, 2004 and 2010. It will approach to Sun down to 0.044 a.u. on Feb. 28. After the perihelion passage, it may be observed on the ground from March to April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  22 51.67   -9 32.9   1.081   0.107     3    9.6  19:17 ( 90,-16)  
Mar.  6  21 55.80  -10 21.8   0.963   0.307    17   16.2   4:59 (278, -6)  

* SWAN21D

New bright comet. Now it is very bright as 10.5 mag (Feb. 28, Michael Jager). In the Northern Hemisphere, it stays observable in the evening low sky until early June while the comet will be fading. In the Southern Hemisphere, it will be observable only in the extremely low sky from May to June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  23 22.74   12 20.2   1.697   0.881    23   10.6  19:17 (104,  3)  
Mar.  6  23 55.37   17  9.0   1.651   0.875    25   10.5  19:23 (108,  6)  

* C/2020 R4 ( ATLAS )

It brightened rapidly in December. Now it is bright as 11.4 mag (Feb. 27, Ken-ichi Kadota). It will approach to Earth down to 0.46 a.u. in April, and it is expected to brighten up to 9 mag and to be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  20 41.52  -11 59.6   1.772   1.030    29   10.9   5:08 (287,  4)  
Mar.  6  20 35.31  -10 40.9   1.621   1.031    37   10.7   4:59 (290,  9)  

* 10P/Tempel 2

It will brighten up to 11.5 mag in spring. However, the condition is very bad in this apparition. It will appear in the morning low sky in March 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)  
Feb. 27  20 59.76  -16 41.3   2.264   1.438    25   11.9   5:08 (289, -2)  
Mar.  6  21 23.74  -15 35.9   2.237   1.426    26   11.7   4:59 (287, -3)  

* C/2021 A2 ( NEOWISE )

It brightened up to 10.5 mag in early February (Feb. 6, Marco Goiato). Now it is fading. In the Northern Hemisphere, it stays observable in excellent condition after this. In the Southern Heimsphere, it will be unobservable in mid March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   5 27.99   34 22.2   0.906   1.502   104   12.1  19:17 ( 88, 86)  
Mar.  6   5 13.87   39 22.8   1.090   1.539    95   12.6  19:23 (114, 76)  

* C/2019 N1 ( ATLAS )

Now it is bright as 12.9 mag (Feb. 9, Chris Wyatt). It stays 12 mag until March. In the Southern Hemisphere, it stays observable in good condition after this. In the Northern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  20  9.40  -88 21.7   1.965   2.046    80   12.1   5:08 (358,-34)  
Mar.  6   2 18.65  -85  0.6   2.009   2.095    80   12.2  19:23 (  6,-32)  

* C/2019 L3 ( ATLAS )

Now it is 12.4 mag (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 10 mag in winter in 2022. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it is not observable until November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   1 23.59   52  7.2   4.783   4.540    69   13.1  19:17 (132, 41)  
Mar.  6   1 34.91   51 49.5   4.818   4.503    65   13.1  19:23 (132, 38)  

* C/2020 S3 ( Erasmus )

It brightened up to 5.6 mag in early December (Dec. 9, Marco Goiato). In mid December, it was visible at about 3 mag in the SOHO spacecraft images (Dec. 18, Hirohisa Sato). Now it is not observable. It will appear in the morning sky again in April. But then it will be fainter than 15 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  22 16.76    1 44.1   2.627   1.669    11   13.3   5:08 (263, -7)  
Mar.  6  22 30.84    3 15.5   2.737   1.782    12   13.7   4:59 (262, -6)  

* 156P/Russell-LINEAR

Brightened rapidly, and it brightened up to 9.7 mag in November (Nov. 15, Chris Wyatt). Now it is fading. But it is bright as 12.0 mag still now (Feb. 9, Chris Wyatt). In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it locates extremely low after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   4  2.32   40 14.4   1.468   1.747    88   13.4  19:17 (112, 69)  
Mar.  6   4 24.13   40 39.6   1.568   1.795    85   13.7  19:23 (113, 67)  

* C/2019 F1 ( ATLAS-Africano )

It will brighten up to 13 mag from spring to summer. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it is not observable until July in 2022.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  17 58.59  -58 37.5   3.921   3.746    72   13.7   5:08 (342, -8)  
Mar.  6  18 12.40  -60 15.4   3.828   3.729    76   13.6   4:59 (343, -9)  

* C/2017 K2 ( PanSTARRS )

Now it is 14.2 mag (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). It is expected to be observable at 5-6 mag for a long time from 2022 to 2023. In the Northern Hemisphere, it is not observable at the high light from 2022 summer to 2023 summer. In the Southern Hemisphere, it stays extremely low for a while. But it will be observable in good condition at the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  18 22.22   36 43.0   7.177   6.991    75   13.7   5:08 (255, 56)  
Mar.  6  18 24.43   37 12.9   7.070   6.935    78   13.7   4:59 (255, 60)  

* 29P/Schwassmann-Wachmann 1

Now it is 13.9 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). In the Southern Hemisphere, it will be unobservable in late February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   2 31.98   24  7.5   6.205   5.861    65   13.7  19:17 ( 89, 47)  
Mar.  6   2 36.21   24 17.1   6.306   5.862    59   13.8  19:23 ( 93, 41)  

* C/2021 A4 ( NEOWISE )

It brightening very rapidly up to 12.5 mag in early February (Feb. 8, Michael Jager). Now it is fading. In the Northern Hemisphere, it stays observable in excellent condition. It will be observable in good condition after this also in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   4 36.90   19 19.6   0.630   1.193    92   13.8  19:17 ( 48, 67)  
Mar.  6   4 24.33    9  7.7   0.796   1.167    80   14.0  19:23 ( 52, 53)  

* 88P/Howell

It brightened up to 8.2 mag in autumn (Oct. 13, Chris Wyatt). Now it is fading. It has already faded down to 13.0 mag (Feb. 14, Sandor Szabo). In the Southern Hemisphere, it is already unobservable. In the Northern Hemisphere, it will be unobservable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   0 28.55    1  2.9   2.880   2.067    28   13.8  19:17 ( 85, 10)  
Mar.  6   0 42.73    2 41.2   2.965   2.114    25   14.1  19:23 ( 89,  7)  

* C/2020 M3 ( ATLAS )

It brightened up to 7.3 mag in November (Nov. 7, Marco Goiato). Now it is fading. It has already faded down to 15.1 mag (Feb. 14, Thomas Lehmann). In the Northern Hemisphere, it stays observable in excellent condition for a long time. In the Southern Hemisphere, it stays locating extremely low after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   6 10.75   47 41.9   1.585   2.154   111   14.0  19:43 (180, 77)  
Mar.  6   6 22.24   47 11.1   1.722   2.226   107   14.4  19:27 (180, 78)  

* C/2020 T2 ( Palomar )

Now it is 14.2 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 12.5 mag from spring to summer, and it stays observable in good condition for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  14  4.08   30 47.7   1.860   2.586   127   14.2   3:37 (  0, 86)  
Mar.  6  14  6.46   31 43.1   1.779   2.539   130   14.0   3:12 (  0, 87)  

* 246P/NEAT

Now it is 15.5 mag (Jan. 19, Slooh.com Chile Observatory, La Dehesa). It stays 13-14 mag from 2020 to 2021. It will be observable in good condition after this in the Southern Hemisphere. It locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  18 18.36  -22 41.2   3.155   2.864    64   14.1   5:08 (320, 21)  
Mar.  6  18 28.28  -22 59.4   3.069   2.865    68   14.0   4:59 (322, 21)  

* C/2020 J1 ( SONEAR )

Now it is 14.4 mag (Jan. 20, iTelescope Observatory, Siding Spring). It will brighten up to 13.5 mag in spring. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it will be getting higher and becoming observable slowly.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  17 48.21  -40  6.4   3.570   3.389    71   14.6   5:08 (335,  9)  
Mar.  6  17 44.73  -39 53.7   3.428   3.380    78   14.5   4:59 (339, 11)  

* C/2019 T4 ( ATLAS )

Now it is 14.2 mag and visible visually (Jan. 25, Chris Wyatt). It is expected to brighten up to 11.5 mag in 2022. It is observable in excellent condition in the Southern Hemisphere. In the Northern Hemisphere, it is observable from autumn to winter, but it locating extremely low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   8  2.12  -38 14.7   5.116   5.684   120   14.6  21:32 (  0, 17)  
Mar.  6   8  0.41  -37 24.2   5.101   5.648   118   14.6  21:03 (  0, 18)  

* 398P/2020 P2 ( Boattini )

First return of a new periodic comet which brightened up to 13 mag in 2009. It brightened up to 11.7 mag in January (Jan. 10, Marco Goiato). Now it is fading. It has already faded down to 14.7 mag (Feb. 14, Thomas Lehmann). It stays observable in good condition while the comet will be fading after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   6 46.94   26  7.3   0.695   1.482   122   14.6  20:19 (  0, 81)  
Mar.  6   7  5.20   27  9.9   0.766   1.519   119   15.1  20:10 (  0, 82)  

* C/2018 U1 ( Lemmon )

Now it is 15.9 mag (Nov. 10, Toshihiko Ikemura, Hirohisa Sato). It will stay at 14 mag for a long time from 2021 to 2022. It stays observable in good condition after this while brightening gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  18 22.05    2 33.4   5.684   5.345    65   15.0   5:08 (300, 39)  
Mar.  6  18 23.07    2 23.5   5.564   5.326    71   14.9   4:59 (305, 42)  

* P/2020 U2 ( PanSTARRS )

Brightened very rapidly. Now it is 15.0 mag (Feb. 4, Michael Jager). It stays observable at 15-16 mag in good condition for a while. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   4 12.58   27 56.1   1.696   1.934    88   15.1  19:17 ( 77, 69)  
Mar.  6   4 28.37   28  6.4   1.780   1.953    84   15.0  19:23 ( 81, 66)  

* 17P/Holmes

Now it is 15.8 mag (Jan. 16, Slooh.com Canary Islands Observatory). It is not observable until June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  23  6.68    0 39.2   3.043   2.081    11   15.1  19:17 ( 96, -7)  
Mar.  6  23 20.73    2 42.8   3.056   2.083     9   15.1  19:23 (101,-10)  

* C/2017 T2 ( PanSTARRS )

It had been observed as 8-9 mag for a long time in 2020. Now it is fading. It has already faded down to 16.6 mag (Jan. 23, Slooh.com Chile Observatory, La Dehesa). It will be observable in good condition after this in the Southern Hemisphere. It locates extremely low after this in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  17 40.13  -33 57.3   4.101   3.924    72   15.1   5:08 (333, 15)  
Mar.  6  17 43.20  -34 55.3   4.057   3.990    79   15.1   4:59 (337, 16)  

* 141P/Machholz 2

It brightened very rapidly in early December, and it brightened up to 10.0 mag in January (Jan. 7, Michael Jager). Now it is fading. It has already faded down to 13.3 mag (Feb. 9, Chris Wyatt). Two more components, H and I, are also observed. It stays observable for a long time in this apparition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   5  3.13    2 33.5   0.837   1.363    96   15.1  19:17 ( 19, 56)  
Mar.  6   5 30.13    3 34.5   0.937   1.438    96   16.0  19:23 ( 22, 57)  

* C/2020 F5 ( MASTER )

Now it is 15.8 mag (Jan. 14, Slooh.com Chile Observatory, La Dehesa). It stays 14-15 mag until the end of 2021. In the Southern Hemisphere, it stays observable in good condition for a long time, although it becomes extremely low temporarily from January to February. In the Northern Hemisphere, it is not observable until June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  22 13.23  -45 53.5   5.070   4.331    37   15.2   5:08 (307,-30)  
Mar.  6  22 22.54  -44 45.5   5.040   4.329    40   15.2   4:59 (307,-28)  

* C/2020 K5 ( PanSTARRS )

It will brighten up to 13 mag from spring to summer. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it locates extremely low now, and it will be unobservable soon. Then it is not observable until September when it fades down to 15 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  19 37.71  -29  9.0   2.568   2.033    47   15.6   5:08 (310,  4)  
Mar.  6  19 55.15  -30 54.0   2.438   1.975    51   15.4   4:59 (312,  3)  

* C/2019 T2 ( Lemmon )

Now it is 16.3 mag (Nov. 9, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 14.5 mag from spring to summer. In the Southern Hemisphere, it stays observable in excellent condition for a long time, although it becomes extremely low temporarily from January to February. In the Northern Hemisphere, it is not observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  22 33.65  -40 22.4   3.496   2.707    31   15.5   5:08 (300,-32)  
Mar.  6  22 43.81  -41 24.5   3.432   2.693    35   15.4   4:59 (301,-31)  

* 409P/2020 V1 ( LONEOS-Hill )

First return of a new periodic comet which brightened up to 14-15 mag in 2006. Now it is 15.5 mag (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 15-16 mag from February to March, and will be observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13 13.42   11 32.5   0.896   1.784   142   15.4   2:47 (  0, 66)  
Mar.  6  13 17.58   13 38.6   0.886   1.799   146   15.5   2:23 (  0, 68)  

* C/2020 N1 ( PanSTARRS )

Now it is 15.7 mag (Feb. 14, Thomas Lehmann). It stays 15-16 mag until spring. In the Northern Hemisphere, it stays observable in excellent condition. In the Southern Hemisphere, it stays extremely low until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   3  8.79   20 33.3   1.250   1.335    72   15.5  19:17 ( 77, 53)  
Mar.  6   3 34.96   18 42.5   1.266   1.324    70   15.6  19:23 ( 76, 50)  

* 7P/Pons-Winnecke

Now it is 18.1 mag, much fainter than predicted (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 11 mag from May to August. In the Southern Hemisphere, it stays observable in excellent condition for a long time. In the Northern Hemisphere, it stays observable in good condition for a while. But it becomes extremely low after July.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  16 16.99    9 46.5   1.172   1.624    97   15.8   5:08 (337, 63)  
Mar.  6  16 35.81    9 44.9   1.087   1.575    98   15.5   4:59 (337, 63)  

* C/2019 K7 ( Smith )

Now it is 15.5 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). It stays 15-16 mag until spring. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it will be observable in the extremely low sky only in next spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  19 18.37   31 43.0   5.301   4.925    62   15.6   5:08 (257, 44)  
Mar.  6  19 20.21   33 20.9   5.265   4.948    66   15.6   4:59 (257, 48)  

* 28P/Neujmin 1

Now it is not observable. It will be observable in June. But it will fade down to 17 mag at that time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  22 15.40  -14 12.1   2.559   1.586     8   15.7   5:08 (276,-16)  
Mar.  6  22 35.31  -11 35.0   2.550   1.580     9   15.7   4:59 (274,-15)  

* 117P/Helin-Roman-Alu 1

Now it is 15.5 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 13 mag in 2022. In 2021, it is observable at 15-16 mag in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13 44.66   -2 37.6   3.041   3.782   132   15.8   3:18 (  0, 52)  
Mar.  6  13 43.06   -2 24.1   2.952   3.766   139   15.7   2:49 (  0, 52)  

* C/2021 A7 ( NEOWISE )

Now it is 16.5 mag (Feb. 5, Thomas Lehmann). It brightens up to 15 mag from spring to summer. In the Southern Hemisphere, it stays observable in good condition until June. In the Northern Hemisphere, it is observable in the low sky from March to May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   5 55.86  -51 59.9   2.291   2.570    94   15.9  19:26 (  0,  3)  
Mar.  6   5 59.16  -48 24.0   2.241   2.519    94   15.8  19:23 (  4,  7)  

* C/2018 N2 ( ASASSN )

Now it is 14.9 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable for a long time while it is getting fainter slowly. In the Southern Hemisphere, it will never be observable again.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  16 32.30   65 43.9   5.113   5.349    98   15.9   5:08 (191, 58)  
Mar.  6  16 26.81   66 37.1   5.149   5.397    99   15.9   4:59 (186, 58)  

* C/2020 M5 ( ATLAS )

Now it is 16.4 mag (Jan. 17, D. Buczynski). In the Northern Hemisphere, it stays observable at 15 mag for a long time from spring to early 2022. In the Southern Hemisphere, it is not observable until the end of 2021.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  20 12.15   51 44.6   3.700   3.454    68   16.4   5:08 (228, 39)  
Mar.  6  20 15.26   53 39.7   3.643   3.421    69   16.3   4:59 (226, 42)  

* C/2020 Y2 ( ATLAS )

Now it is 17.0 mag (Feb. 6, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 13 mag in 2022. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it stays observable until June when it brightens up to 16 mag. But it will not be observable at the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13 58.69  -18 57.6   4.742   5.357   123   16.7   3:32 (  0, 36)  
Mar.  6  13 53.73  -19 24.5   4.598   5.310   131   16.6   3:00 (  0, 36)  

* P/2020 T3 ( PanSTARRS )

It brightened very rapidly up to 16.5 mag in January (Jan. 2, D. Buczynski). However, it is fading very rapidly in February. It has already faded down to 18.3 mag (Feb. 11, Toshihiko Ikemura, Hirohisa Sato). It is observable in excellent condition in the Northern Hemisphere. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   3 34.51   22 34.7   1.335   1.494    78   16.6  19:17 ( 75, 59)  
Mar.  6   3 57.30   24 15.1   1.394   1.517    76   16.7  19:23 ( 80, 58)  

* 277P/LINEAR

It brightened rapidly and became brighter than expected. Now it is 16.7 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). It is observable in good condition in the Northern Hemisphere. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   4 12.23   21 32.8   1.764   1.974    86   16.6  19:17 ( 63, 66)  
Mar.  6   4 26.72   21 10.3   1.851   1.991    82   16.8  19:23 ( 68, 62)  

* C/2020 H6 ( ATLAS )

Now it is 16.8 mag (Feb. 6, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 16-17 mag from 2021 to 2022.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  14 29.35  -23 57.6   4.498   5.003   115   16.8   4:03 (  0, 31)  
Mar.  6  14 28.05  -23  4.7   4.376   4.984   122   16.7   3:34 (  0, 32)  

* C/2017 Y2 ( PanSTARRS )

Now it is 16.3 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). It is observable at 16.5 mag from spring in 2020 to summer in 2021.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  17 52.02  -11 17.9   4.954   4.721    70   16.7   5:08 (318, 33)  
Mar.  6  17 51.14  -11 41.3   4.841   4.732    77   16.7   4:59 (324, 36)  

* C/2019 O3 ( Palomar )

Now it is 16.6 mag (Nov. 9, Toshihiko Ikemura, Hirohisa Sato). It stays at 16-17 mag from 2020 to 2021. In the Northern Hemisphere, it stays observable in good condition for a long time. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  19 39.73   34 56.1   9.261   8.820    60   16.7   5:08 (251, 41)  
Mar.  6  19 41.85   35 47.8   9.220   8.819    63   16.7   4:59 (252, 44)  

* C/2017 U7 ( PanSTARRS )

Now it is 16.3 mag (Oct. 17, ATLAS-MLO, Mauna Loa). It will be fading slowly.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  18 28.73  -18 46.0   7.767   7.347    61   17.0   5:08 (315, 22)  
Mar.  6  18 28.79  -18 25.9   7.674   7.370    68   17.0   4:59 (319, 25)  

* C/2020 O2 ( Amaral )

Now it is 17.7 mag (Sept. 14, Slooh.com Chile Observatory, La Dehesa). It will brighten up to 16.5 mag in summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  17 30.27  -35  2.4   5.234   5.066    74   17.1   5:08 (336, 15)  
Mar.  6  17 33.14  -34 32.4   5.108   5.052    81   17.1   4:59 (339, 17)  

* 402P/2020 Q3 ( LINEAR )

First return of a new periodic comet which brightened up to 16 mag from 2003 to 2004. Now it is 17.6 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 16 mag in next winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   2 54.83  -11 46.7   4.628   4.266    62   17.2  19:17 ( 49, 28)  
Mar.  6   3  0.14  -10 40.9   4.692   4.252    58   17.2  19:23 ( 56, 24)  

* 162P/Siding Spring

Now it is 16.0 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and will be fainter than 18 mag in April. In the Northern Hemisphere, it stays observable in good condition for a long time after this. In the Southern Hemisphere, it will never be unobservable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   2 21.10   37 21.6   1.632   1.577    69   17.2  19:17 (109, 49)  
Mar.  6   2 44.39   39 28.5   1.713   1.620    67   17.3  19:23 (113, 48)  

* A/2019 U5

Now it is 17.3 mag (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). Although it is an asteroid, it is brightening rapidly. It may 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 is not observable now. It will appear in mid March, but it stays extremely low after that.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  18 35.75   40  4.8   7.489   7.282    74   17.3   5:08 (248, 54)  
Mar.  6  18 36.43   40 50.3   7.394   7.237    77   17.2   4:59 (247, 58)  

* C/2020 R7 ( ATLAS )

Now it is 18.2 mag (Feb. 2, Thomas Lehmann). It is expected to brighten up to 12 mag in 2022. In the Southern Hemisphere, it stays observable in good condition for a long time. In the Northern Hemisphere, it is not observable until 2022 autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   2 41.97  -45  4.7   6.353   5.976    63   17.3  19:17 ( 31,  0)  
Mar.  6   2 42.73  -44 28.2   6.345   5.926    60   17.2  19:23 ( 36, -3)  

* C/2020 Y3 ( ATLAS )

Now it is 17.0 mag (Feb. 15, Michael Jager). It stays 17.5 mag and observable in good condition until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  15  0.20   13 30.7   1.627   2.246   116   17.3   4:33 (  0, 68)  
Mar.  6  14 59.90   19  4.3   1.602   2.284   121   17.3   4:05 (  0, 74)  

* 413P/2020 W4 ( Larson )

First return of a new periodic comet which brightened up to 16 mag in 2014. Now it is 18.3 mag (Feb. 14, Michael Jager). It will brighten up to 17 mag in spring, and it will be observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  12 59.87   12 40.9   1.510   2.392   145   17.6   2:33 (  0, 68)  
Mar.  6  12 56.78   12 51.3   1.449   2.370   151   17.4   2:03 (  0, 68)  

* C/2019 C1 ( ATLAS )

It brightened up to 16.1 mag in last winter (Mar. 18, 2020, Toshihiko Ikemura, Hirohisa Sato). Now it is 17.6 mag (Feb. 9, Toshihiko Ikemura, Hirohisa Sato). In 2021, it stays observable at 17-18 mag in good condition until early summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13 13.78  -19 46.5   6.161   6.872   132   17.5   2:47 (  0, 35)  
Mar.  6  13 12.70  -19 27.1   6.097   6.885   139   17.5   2:19 (  0, 35)  

* 99P/Kowal 1

Now it is 18.0 mag (Feb. 6, Toshihiko Ikemura, Hirohisa Sato). It stays 17-18 mag for a long time from 2021 to 2023.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  10 57.31   11  0.2   3.961   4.948   174   17.6   0:31 (  0, 66)  
Mar.  6  10 53.82   11 18.8   3.953   4.940   173   17.6   0:00 (  0, 66)  

* C/2020 V2 ( ZTF )

Now it is 17.2 mag (Feb. 8, 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 extremely low until mid July, then it becomes unobservable for a while. But it becomes observable in good condition after 2023 summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13  8.11   33 28.7   7.102   7.863   137   17.7   2:42 (  0, 88)  
Mar.  6  13  4.26   34 21.3   7.020   7.811   140   17.7   2:10 (  0, 89)  

* A/2020 F7

Now it is 17.0 mag (Feb. 7, Toshihiko Ikemura, Hirohisa Sato). Although it is an asteroid, it is brightening rapidly. It stays 17-18 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 is observable only until May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   8 48.23   -6 34.3   4.800   5.667   148   17.7  22:18 (  0, 48)  
Mar.  6   8 42.13   -6 43.7   4.835   5.650   141   17.7  21:44 (  0, 48)  

* C/2020 S8 ( Lemmon )

Now it is 18.0 mag (Feb. 8, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 17 mag from April to May, and it will be observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  16 43.91   16  7.8   2.175   2.412    91   18.0   5:08 (316, 66)  
Mar.  6  16 36.12   16 12.2   2.037   2.397    98   17.8   4:59 (330, 69)  

* C/2019 E3 ( ATLAS )

It stays 17-18 mag for a long time until 2026. In the Southern Hemisphere, it stays sobservable in good condition for a long time. It is not observable in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   9 18.41  -57 23.3  11.166  11.575   112   17.9  22:48 (  0, -2)  
Mar.  6   9 13.42  -57 18.1  11.136  11.558   112   17.9  22:15 (  0, -2)  

* C/2021 A1 ( Leonard )

Now it is 18.0 mag (Feb. 9, Katsumi Yoshimoto). It will approach to Earth down to 0.2 a.u. in December, and it is expected to brighten up to 4 mag. In the Northern Hemisphere, it stays observable in good condition for a long time until December while the comet is brightening gradually. In the Southern Hemisphere, it is not observable until mid December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  13 49.94   53 22.4   3.917   4.509   121   18.0   3:23 (180, 72)  
Mar.  6  13 41.20   55 12.0   3.832   4.434   121   17.9   2:47 (180, 70)  

* C/2020 F2 ( ATLAS )

It stays observable at 18 mag for a long time until 2024.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  15 35.53  -12 44.1   9.004   9.286   103   18.0   5:08 (  0, 42)  
Mar.  6  15 33.52  -12 25.8   8.870   9.274   111   17.9   4:39 (  0, 42)  

* 414P/2021 A3 ( STEREO )

New periodic comet discovered in 2016. It had been predicted to return in 2024. But actually, it returned much earlier than predicted. It brightened very rapidly up to 11 mag in January (Jan. 16, Giuseppe Pappa). Now it is fading very rapidly. It has already faded out, fainter than 19.5 mag (Feb. 21, Katsumi Yoshimoto). In the Southern Hemisphere, it stays observable in excellent condition after this. In the Northern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27  19 36.76  -52 21.8   0.615   0.839    57   18.9   5:08 (327,-12)  
Mar.  6  19 16.80  -52 33.1   0.648   0.939    66   21.0   4:59 (331, -8)  

* 323P/SOHO

Five apparitions of this comet was confirmed in 1999, 2004, 2008, 2012 and 2016. It approached to Sun down to 0.04 a.u. on Jan. 17. It may be observed on the ground in December and February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 27   3 59.41   23 37.3   0.755   1.183    84   20.1  19:17 ( 71, 65)  
Mar.  6   4 37.38   24 40.5   0.934   1.313    85   21.0  19:23 ( 72, 66)  

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