Weekly Information about Bright Comets (2019 Feb. 2: North)

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Updated on February 3, 2019
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Best time and the azimuth, altitude (A,h) are at lat. 35 deg in the Northern Hemisphere.
Azimuth indicates 0 for south, 90 for west, 180 for north, 270 for east.

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* C/2018 Y1 ( Iwamoto )

Bright new comet. Now it is very bright as 8.3 mag (Jan. 29, Katsumi Yoshimoto). It will approach to Earth down to 0.3 a.u. in February. Then it will brighten up to 7 mag and will be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  12 57.00  -12 11.3   0.516   1.289   114    8.2   4:12 (  0, 42)  
Feb.  9  11 27.05    3 28.5   0.338   1.287   148    7.2   2:19 (  0, 57)  

* 46P/Wirtanen

It approached to Earth down to 0.08 a.u. in mid December, and it brightened up to 3.4 mag (Dec. 14, Seiichi Yoshida). it looked so large as 3 times of Moon. Now it is fading. But it is bright as 7.7 mag still now (Jan. 29, Carlos Labordena). In the Northern Hemisphere, it stays observable in excellent condition. In the Southern Hemisphere, it is not observable until February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   9 25.90   54 37.3   0.321   1.254   142    7.4   0:40 (180, 70)  
Feb.  9   9 30.36   52 28.4   0.374   1.304   142    8.2   0:17 (180, 72)  

* C/2016 M1 ( PanSTARRS )

It brightened up to 7.7 mag in June (June 19, Juan Jose Gonzalez). Now it is fading. But it is still bright as 10.9 mag (Jan. 14, Chris Wyatt). In the Southern Hemisphere, it stays observable in good condition for a long time until the comet will fade out. In the Northern Hemisphere, it is not observable for a long time until autumn when the comet fades out down to 16 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   2 43.33  -74 51.7   3.108   2.964    72   11.4  18:55 (  4,-20)  
Feb.  9   3  2.15  -71 33.0   3.137   3.015    73   11.5  19:01 (  6,-17)  

* 38P/Stephan-Oterma

It brightened up to 9.5 mag from autumn to winter (Dec. 14, Marco Goiato). Now it is fading. But it is bright as 11.3 mag still now (Jan. 25, Carlos Labordena). In the Northern Hemisphere, it stays observable in good condition for a long time until it fades out. It locates low in the Southern Hemispehre.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   8 28.11   47 18.1   0.980   1.894   149   11.4  23:39 (180, 78)  
Feb.  9   8 26.69   47 28.4   1.048   1.940   145   11.8  23:10 (180, 78)  

* 64P/Swift-Gehrels

It brightened up to 9.0 mag from autumn to winter (Nov. 16, Maik Meyer). Now it is fading. But it is bright as 10.8 mag still now (Jan. 25, Carlos Labordena). It is observable in excellent condition in the Northern Hemisphere. It stays low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   4 12.17   26 44.6   1.105   1.747   113   11.6  19:24 (  0, 82)  
Feb.  9   4 27.69   26 16.3   1.204   1.795   109   12.1  19:12 (  0, 81)  

* C/2018 L2 ( ATLAS )

Now it is 10.4 mag (Jan. 3, Ken Harikae). It will be fading gradually after this. In the Northern Hemisphere, it stays observable for a long time until it fades out. But it stays extremely low. It will never be observable again in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  20 39.23   29 50.8   2.415   1.888    47   11.8   5:32 (242, 13)  
Feb.  9  21  3.32   32  5.2   2.454   1.928    47   12.1   5:27 (240, 14)  

* 78P/Gehrels 2

Now it is 13.7 mag (Jan. 2, Toshihiko Ikemura, Hirohisa Sato). It stays at 12-13 mag for a long time until autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  23 53.98    0 26.3   2.628   2.072    46   12.6  18:55 ( 70, 27)  
Feb.  9   0  8.33    1 43.2   2.669   2.060    42   12.5  19:01 ( 75, 24)  

* C/2016 N6 ( PanSTARRS )

Now it is 12.8 mag (Jan. 23, Thomas Lehmann). It stays 12 mag for a long time until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   6 14.16  -22 12.4   2.717   3.363   123   13.0  21:24 (  0, 33)  
Feb.  9   6  3.52  -22 15.1   2.835   3.406   117   13.2  20:46 (  0, 33)  

* C/2016 R2 ( PanSTARRS )

Now it is 13.6 mag (Jan. 16, Thomas Lehmann). It will be fading slowly after this. It is observable in good condition in the Northern Hemisphere. In the Southern Hemisphere, it will appear in the morning sky soon. But it stays extremely low for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  15 55.70   42 23.6   3.627   3.785    91   13.2   5:32 (242, 70)  
Feb.  9  15 59.84   43  1.7   3.627   3.834    94   13.3   5:27 (237, 73)  

* C/2018 N2 ( ASASSN )

Now it is 14.6 mag (Jan. 22, Thomas Lehmann). It will brighten up to 10-11 mag in autumn. It will be unobservable temporarily in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   1  4.84  -25 31.4   4.562   4.111    57   13.4  18:55 ( 38, 19)  
Feb.  9   1  6.97  -23 40.3   4.603   4.071    52   13.4  19:01 ( 45, 16)  

* 29P/Schwassmann-Wachmann 1

Now it is bright as 12.9 mag (Jan. 2, Toshihiko Ikemura, Hirohisa Sato).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  23 18.27    1 55.1   6.500   5.767    38   13.8  18:55 ( 78, 20)  
Feb.  9  23 23.09    2 25.5   6.566   5.767    33   13.8  19:01 ( 83, 15)  

* 123P/West-Hartley

Now it is 12.6 mag (Jan. 21, Sandor Szabo). It is observable in excellent condition in the Northern Hemisphere. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 40.52   30 23.7   1.268   2.127   141   13.9   2:54 (  0, 85)  
Feb.  9  11 38.96   31  0.4   1.236   2.127   146   13.9   2:25 (  0, 86)  

* 60P/Tsuchinshan 2

Now it is 13.5 mag (Jan. 28, Thomas Lehmann). It is observable at 14 mag in excellent condition until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 46.71   -5 37.8   0.871   1.703   133   13.9   3:01 (  0, 49)  
Feb.  9  11 47.33   -6  9.1   0.851   1.725   139   14.0   2:34 (  0, 49)  

* C/2017 M4 ( ATLAS )

Now it is 13.9 mag (Jan. 19, Martin Masek). It stays 13-14 mag until summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  17 26.84  -15 52.6   3.784   3.255    50   14.0   5:32 (310, 22)  
Feb.  9  17 29.39  -17  6.9   3.685   3.258    57   14.0   5:27 (315, 24)  

* C/2015 O1 ( PanSTARRS )

Now it is 14.6 mag (Jan. 10, Toshihiko Ikemura, Hirohisa Sato). It will be fading slowly after this. It is observable in excellent condition until spring in the Northern Hemispehre. In the Southern Hemisphere, it will be hardly observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  10 46.16   43 30.3   3.959   4.802   145   14.5   2:01 (180, 82)  
Feb.  9  10 32.49   44  0.2   3.975   4.839   147   14.5   1:20 (180, 81)  

* C/2018 A6 ( Gibbs )

Now it is bright as 14.8 mag (Dec. 12, Kunihiro Shima). It stays 14 mag for a long time in 2019. In the Southern Hemisphere, it is observable in excellent condition. In the Northern Hemisphere, it is not observasble until summer in 2020.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  10 52.96  -52 59.0   2.930   3.337   105   14.6   2:07 (  0,  2)  
Feb.  9  10 38.12  -55 12.3   2.866   3.312   108   14.5   1:25 (  0,  0)  

* (944) Hidalgo

Now it is 14.3 mag (Nov. 30, Seiichi Yoshida). It stays at 14 mag until winter. It is observable in excellent condition in the Northern Hemisphere. In the Southern Hemisphere, it is not observable until summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  12  8.80   81 21.9   1.596   2.177   112   14.6   3:24 (180, 44)  
Feb.  9  11 23.42   80 57.0   1.629   2.207   112   14.7   2:12 (180, 44)  

* C/2017 B3 ( LINEAR )

Now it is 14.5 mag (Aug. 16, P. Camilleri, H. Williams). It stays 15 mag from 2018 to 2019, and it will be observable for a long time in the Southern Hemisphere. In the Northern Hemisphere, it will never be observable again.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  21 21.45  -60 22.4   4.577   3.921    43   14.9  18:55 ( 36,-32)  
Feb.  9  21 38.56  -59  8.7   4.567   3.922    44   14.9  19:01 ( 38,-34)  

* C/2018 A3 ( ATLAS )

Now it is 14.6 mag (Jan. 21, Sandor Szabo). It stays 15 mag until March. It is observable in excellent condition in the Northern Hemisphere. It is not observable at all in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   5 24.18   74 28.0   2.733   3.282   115   15.3  20:33 (180, 51)  
Feb.  9   4 42.52   71 55.3   2.818   3.287   109   15.4  19:25 (180, 53)  

* C/2017 T2 ( PanSTARRS )

Now it is 15.5 mag (Jan. 25, Artyom Novichonok). It is expected to brighten up to 7-8 mag in 2020. It will be unobservable temporarily in April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   2 58.79   -1 15.7   5.302   5.381    89   15.4  18:55 ( 19, 52)  
Feb.  9   2 58.78   -0 29.8   5.353   5.319    82   15.4  19:01 ( 32, 50)  

* 240P/NEAT

Although it was faint as 16-17 mag in November, it brightened up to 14.7 mag in December (Dec. 12, Toshihiko Ikemura, Hirohisa Sato). Now it is 15.5 mag (Jan. 21, Sandor Szabo). In the Northern Hemisphere, it stays observable in excellent condition after this. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 20.15   40  2.0   2.033   2.874   142   15.9   2:34 (180, 85)  
Feb.  9  11 15.28   41  7.1   2.041   2.905   145   16.1   2:02 (180, 84)  

* 21P/Giacobini-Zinner

It brightened up to 6.8 mag in September (Sept. 17, Seiichi Yoshida). Now it is fading rapidly. It has already faded down to 13.8 mag (Jan. 6, Toshihiko Ikemura, Hirohisa Sato). It is observable in excellent condition in the Southern Hemisphere. It locates low after this in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   6  4.77  -27  4.8   1.420   2.081   118   16.4  21:15 (  0, 28)  
Feb.  9   6  5.40  -24 34.9   1.512   2.144   116   16.8  20:49 (  0, 31)  

* P/2014 C1 ( TOTAS )

First return of a new periodic comet discovered in 2014. It has not been recovered yet. Now it is not detected, fainter than 20.0 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). The condition of this apparition is excelllent. It will brighten rapidly, and will be observable at 15.5 mag in excellent condition in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  10 28.99    7 11.0   0.938   1.882   156   16.6   1:43 (  0, 62)  
Feb.  9  10 26.69    7 36.6   0.888   1.857   163   16.4   1:13 (  0, 62)  

* C/2018 W2 ( Africano )

It is expected to brighten up to 10 mag in autumn. Now it is 17.2 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable for a long time while the comet is brightening. In the Southern Hemisphere, it it not observable until mid September.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  14 22.57   69 20.2   2.681   3.146   109   16.6   5:32 (181, 56)  
Feb.  9  14 33.72   73 12.9   2.622   3.076   108   16.5   5:18 (180, 52)  

* C/2017 T3 ( ATLAS )

It brightened up to 8.7 mag in July (July 18, Marco Goiato). Then it faded down to 12.3 mag in August (Aug. 29, Chris Wyatt). It stays observable in good condition after this while the comet will be fading.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  16 24.04  -16 59.8   3.391   3.116    65   16.6   5:32 (325, 30)  
Feb.  9  16 26.39  -16  3.7   3.357   3.199    72   16.7   5:27 (329, 33)  

* C/2010 U3 ( Boattini )

Now it is 16.4 mag (Jan. 6, Toshihiko Ikemura, Hirohisa Sato). It stays 16-17 mag for a long time until 2020. It is observable in good condition in the Northern Hemisphere. It is not observable at all in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 52.24   73 36.4   7.931   8.447   118   16.6   3:06 (180, 52)  
Feb.  9  11 47.56   73 55.4   7.940   8.446   117   16.6   2:34 (180, 51)  

* C/2016 A1 ( PanSTARRS )

It brightened up to 14.7 mag in early 2018 (Jan. 25, Catalina Sky Survey). Now it is fading slowly. Now it is 16.4 mag (Jan. 3, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable in good condition for a long time until the comet fades out. It is never observable again in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   4 51.97   72  7.1   5.742   6.217   114   16.9  20:03 (180, 53)  
Feb.  9   4 38.24   71 30.1   5.842   6.243   109   17.0  19:22 (180, 54)  

* 59P/Kearns-Kwee

Now it is 17.0 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 17 mag in good condition until February. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   8  3.01   22 54.2   1.616   2.582   165   17.0  23:13 (  0, 78)  
Feb.  9   7 58.30   22 34.9   1.664   2.603   157   17.1  22:41 (  0, 78)  

* 171P/Spahr

Now it is 16.5 mag (Jan. 3, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   4 31.52   20  3.1   1.106   1.781   116   17.0  19:43 (  0, 75)  
Feb.  9   4 39.01   22 26.2   1.171   1.789   111   17.2  19:23 (  0, 78)  

* C/2018 F4 ( PanSTARRS )

Now it is 17.4 mag (Jan. 3, Toshihiko Ikemura, Hirohisa Sato). It stays 16 mag for a long time from 2019 to 2020. It is observable in excellent condition in the Southern Hemisphere. It is hardly observable in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  14 18.08  -42 22.3   4.370   4.413    86   17.1   5:32 (  0, 13)  
Feb.  9  14 17.16  -44  5.2   4.230   4.375    91   17.0   5:03 (  0, 11)  

* 164P/Christensen

Now it is 17.0 mag (Jan. 6, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in March. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 12.88   28 15.0   1.850   2.733   147   17.2   2:27 (  0, 83)  
Feb.  9  11  7.59   29 22.5   1.858   2.774   152   17.2   1:54 (  0, 84)  

* C/2014 B1 ( Schwartz )

Now it is 17.1 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). Fading slowly. It stays observable at 17 mag in good condition until summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 42.69    7  2.1   9.200   9.966   139   17.2   2:57 (  0, 62)  
Feb.  9  11 41.82    7 20.2   9.140   9.977   146   17.2   2:28 (  0, 62)  

* 74P/Smirnova-Chernykh

Now it is 16.5 mag (Jan. 10, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17 mag in good condition in 2019. It locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  15 37.67  -15 29.3   3.856   3.756    76   17.3   5:32 (336, 36)  
Feb.  9  15 42.73  -15 45.7   3.760   3.763    82   17.2   5:27 (341, 37)  

* C/2017 K2 ( PanSTARRS )

Now it is 16.3 mag (Jan. 6, Toshihiko Ikemura, Hirohisa Sato). It is expected to be observable at 5-6 mag for a long time from 2022 to 2023. It will be observable in good condition for a long time in the Southern Hemisphere. In the Northern Hemisphere, it is not observable at the highlight from 2022 summer to 2023 summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  18  2.28   52 16.0  12.483  12.338    79   17.4   5:32 (228, 47)  
Feb.  9  18  4.95   52 33.3  12.418  12.293    80   17.4   5:27 (228, 50)  

* 247P/LINEAR

Now it is 17.8 mag (Jan. 5, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in late February. It locates very low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 24.98   38  8.9   0.744   1.637   141   17.4   2:39 (180, 87)  
Feb.  9  11 21.42   38 30.9   0.759   1.670   145   17.6   2:08 (180, 87)  

* 239P/LINEAR

Now it is 17.2 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   8  6.26   -1 52.9   0.715   1.667   156   17.5  23:17 (  0, 53)  
Feb.  9   8  5.18   -2 21.0   0.739   1.680   153   17.6  22:48 (  0, 53)  

* C/2015 XY1 ( Lemmon )

Now it is 17.2 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   4 26.20    3 57.4   7.692   8.108   111   17.6  19:37 (  0, 59)  
Feb.  9   4 23.44    3 54.8   7.817   8.117   104   17.7  19:07 (  0, 59)  

* C/2019 B1 ( Africano )

Now it is 17.5 mag (Jan. 19, Catalina Sky Survey). In the Northern Hemisphere, it is observable at 17.5 mag in good condition in February. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  11 37.50   69 59.7   0.980   1.718   121   17.8   2:56 (180, 55)  
Feb.  9   8 52.57   71 47.4   0.934   1.687   122   17.6  23:22 (180, 54)  

* 361P/2017 S4 ( Spacewatch )

Now it is 16.7 mag (Jan. 5, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in late February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   6 52.72    3 25.7   2.261   3.126   145   17.7  22:03 (  0, 58)  
Feb.  9   6 50.46    3 57.0   2.329   3.146   139   17.8  21:34 (  0, 59)  

* C/2018 X2 ( Fitzsimmons )

Now it is 17.9 mag (Jan. 3, Toshihiko Ikemura, Hirohisa Sato). It stays 17 mag from spring to summer. But it is hardly observable. In the Northern Hemisphere, it is observable only until May. In the Southern Hemisphere, it stays locating extremely low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   3 44.31   48  7.2   2.282   2.777   109   17.7  18:56 (180, 77)  
Feb.  9   3 49.74   47 12.6   2.309   2.728   104   17.7  19:01 (160, 77)  

* 159P/LONEOS

Now it is 16.9 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in March. It locates very low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   5 46.15   43 51.3   3.165   3.887   131   17.7  20:57 (180, 81)  
Feb.  9   5 44.73   43 42.1   3.253   3.900   124   17.8  20:28 (180, 81)  

* 373P/2018 R2 ( Rinner )

Now it is 17.6 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). First return of a new periodic comet which brightened up to 16 mag in 2011. It will be fading after this, and it will be fainter than 18 mag in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   3  1.67   11 44.7   2.081   2.360    93   17.8  18:55 ( 25, 65)  
Feb.  9   3  9.80   11 57.6   2.157   2.351    88   17.8  19:01 ( 38, 62)  

* 232P/Hill

It was expected to be observable at 17.5 mag in good condition in winter in the Northern Hemisphere. But actually, it is so faint as 19.7 mag (Dec. 29, Kunihiro Shima). It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   5  8.44   34 58.8   2.323   3.007   125   17.8  20:20 (180, 90)  
Feb.  9   5  9.12   34 58.3   2.397   3.002   118   17.8  19:53 (  0, 90)  

* 375P/2018 T1 ( Hill )

Now it is 17.9 mag (Jan. 3, Toshihiko Ikemura, Hirohisa Sato). It is observable at 18 mag in good condition from January to February. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  10 43.12   31 34.6   1.015   1.943   152   17.9   1:57 (  0, 87)  
Feb.  9  10 36.98   30 45.7   1.011   1.960   157   17.9   1:24 (  0, 86)  

* 31P/Schwassmann-Wachmann 2

Now it is 17.9 mag (Dec. 31, Toshihiko Ikemura, Hirohisa Sato). It is observable at 18 mag in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   6 31.01   22 27.6   2.632   3.482   144   17.9  21:42 (  0, 77)  
Feb.  9   6 28.48   22 37.5   2.691   3.477   136   18.0  21:12 (  0, 78)  

* C/2016 X1 ( Lemmon )

Now it is 17.8 mag (Jan. 6, Toshihiko Ikemura, Hirohisa Sato). It is observable at 18 mag in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2   7 12.31    3 52.7   6.710   7.583   150   17.9  22:23 (  0, 59)  
Feb.  9   7 10.52    3 53.1   6.757   7.580   144   17.9  21:54 (  0, 59)  

* (6478) Gault

Main-belt asteroid. But it shows a straight tail like a comet. Now it is 17.2 mag (Jan. 12, Toshihiko Ikemura, Hirohisa Sato). It stays observable in excellent condition until early summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb.  2  10 42.77  -11 58.1   1.571   2.421   141   18.1   1:57 (  0, 43)  
Feb.  9  10 38.41  -11 10.6   1.509   2.407   148   17.9   1:25 (  0, 44)  

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