Weekly Information about Bright Comets (2018 Feb. 10: South)

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Updated on February 13, 2018
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Best time and the azimuth, altitude (A,h) are at lat. 35 deg in the Southern Hemisphere.
Azimuth indicates 0 for south, 90 for west, 180 for north, 270 for east.

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* 185P/Petriew

Now it is 11.7 mag (Feb. 10, Chris Wyatt). It stays as bright as 11 mag from January to February. In the Northern Hemisphere, it stays observable for a long time in the evening sky. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   0 29.12   -0 39.3   1.334   0.955    45   11.0  20:32 ( 95,  8)  
Feb. 17   1  3.81    1 15.8   1.328   0.981    47   11.1  20:22 ( 99, 10)  

* C/2016 R2 ( PanSTARRS )

Now it is bright as 11.0 mag (Feb. 4, Marco Goiato). It will stay bright as 11 mag for a long time until spring. In the Southern Hemisphere, it will be unobservable in March. In the Northern Hemispehre, it stays observable for a long time after this until the comet fades out.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   3 58.34   25 30.6   2.392   2.766   101   11.3  20:32 (152, 24)  
Feb. 17   3 58.69   27 19.0   2.472   2.742    95   11.3  20:22 (149, 20)  

* C/2017 T1 ( Heinze )

Now it is very bright as 9.8 mag (Feb. 10, Carlos Labordena). It will go far away from Earth after this. But it will approach to Sun down to 0.58 a.u. on Feb. 21. In the Northern Hemisphere, it stays extremely low after this. In the Southern Hemisphere, it is not observable until late March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  21 44.84   22 43.8   1.003   0.637    37   11.5  20:32 ( 92,-39)  
Feb. 17  21 39.41   18 23.8   1.146   0.590    31   11.6   4:04 (269,-33)  

* 62P/Tsuchinshan 1

It brightened up to 9.2 mag from November to December (Nov. 16, Juan Jose Gonzalez). Now it is fading. But it is bright as 12.4 mag still now (Feb. 10, Chris Wyatt). It stays observable in good condition until summer when it fades out.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  14 22.36    1 46.4   1.086   1.673   107   12.4   3:55 (207, 50)  
Feb. 17  14 27.85    2  0.2   1.066   1.715   113   12.7   4:04 (195, 52)  

* C/2016 N6 ( PanSTARRS )

Now it is 13.1 mag (Jan. 17, Toshihiko Ikemura, Hirohisa Sato). It is expected to brighten up to 12 mag from 2018 to 2019. In the Northern Hemisphere, it stays observable in good condition while the comet will be brightening gradually. In the Southern Hemisphere, it is not observable until October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  15 33.98   68 34.3   2.753   3.133   103   12.6   3:55 (193,-17)  
Feb. 17  15 18.21   72  3.0   2.693   3.097   104   12.5   4:04 (187,-18)  

* C/2016 M1 ( PanSTARRS )

Now it is bright as 12.8 mag (Feb. 1, Thomas Lehmann). It is expected to brighten up to 10 mag in summer in 2018. In the Northern Hemisphere, it stays observable until 2018 summer while the comet will be brightening. It is appear in the morning sky also in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  18 56.61    3  9.5   3.653   3.003    42   13.4   3:55 (265,  2)  
Feb. 17  19  3.05    2 24.9   3.545   2.953    46   13.2   4:04 (261,  8)  

* C/2015 V2 ( Johnson )

It brightened up to 7.1 mag from May to June in 2017 (June 21, Juan Jose Gonzalez). Now it is fading. It has already faded down to 12.9 mag (Jan. 17, Chris Wyatt). In the Southern Hemisphere, it stays observable for a long time after this. However, it will be extremely low from January to March. It will never be observable again in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  22 41.18  -49 47.9   4.125   3.400    37   13.9  20:32 ( 40, 16)  
Feb. 17  22 55.94  -48 56.2   4.185   3.467    38   14.0  20:22 ( 40, 15)  

* 29P/Schwassmann-Wachmann 1

It is not observable now. It will appear in the morning sky in late March in the Southern Hemisphere, or in late April in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  22  4.84   -8 57.2   6.766   5.795     9   13.9  20:32 ( 66,-16)  
Feb. 17  22 10.24   -8 23.2   6.779   5.794     4   13.9  20:22 ( 65,-19)  

* C/2015 O1 ( PanSTARRS )

Now it is very bright as 12.3 mag (Jan. 20, Toshihiko Ikemura, Hirohisa Sato). It will be observable at 13-14 mag for a long time from 2017 to 2018. 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. 10  16 35.40   32 34.5   3.681   3.730    85   14.1   3:55 (221,  8)  
Feb. 17  16 32.90   34 53.2   3.588   3.730    90   14.1   4:04 (213, 11)  

* C/2017 O1 ( ASASSN )

It brightened up to 8.1 mag in autumn (Oct. 3, Juan Jose Gonzalez). Now it is fading. It has already faded down to 14.2 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it will never be observable again after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   5  9.87   80 26.6   1.668   2.188   108   14.1  20:32 (178,-25)  
Feb. 17   5 43.12   78 34.4   1.758   2.253   106   14.5  20:22 (179,-24)  

* C/2017 K6 ( Jacques )

Now it is 13.8 mag (Feb. 10, Chris Wyatt). It stays 14 mag for a while. It stays observable in the evening sky until spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   2 35.64  -16 26.3   2.125   2.055    72   14.5  20:32 (100, 42)  
Feb. 17   2 45.24  -12  7.2   2.207   2.075    69   14.7  20:22 (104, 38)  

* (3200) Phaethon

It approached to Earth down to 0.07 a.u. in mid December, and it brightened up to 10.4 mag (Dec. 15, Thomas Lehmann). It approached to Sun down to 0.14 a.u. on Jan. 25. But it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  22  1.63   -3 29.5   1.451   0.538    13   14.9  20:32 ( 71,-20)  
Feb. 17  22 36.97    1 31.5   1.587   0.697    16   15.6  20:22 ( 78,-20)  

* C/2017 T3 ( ATLAS )

Now it is 15.9 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 9 mag in 2018 summer. However, it is hardly observable when it is bright. In the Northern Hemisphere, it is observable only until March when it brightens up to 14 mag. In the Southern Hemisphere, it is observable from July to September in 2018, but it locates in extremely low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  23 55.03   45 17.7   2.858   2.649    67   15.5  20:32 (130,-24)  
Feb. 17   0  8.38   43 37.1   2.856   2.562    62   15.4  20:22 (128,-24)  

* 174P/(60558) 2000 EC98 ( Echeclus )

Brian Skiff found a bright outburst on Dec. 7. It brightened up to 13.2 mag (Dec. 11, Seiichi Yoshida). It stays bright as 14.6 mag still now (Jan. 19, Sandor Szabo). This is the 4th outburst following those in January 2006, May 2011 and August 2016. It stays observable in good condition for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   2 40.06   11 51.9   7.559   7.458    80   15.4  20:32 (127, 25)  
Feb. 17   2 42.20   12  4.3   7.689   7.476    73   15.7  20:22 (124, 22)  

* 37P/Forbes

Now it is 17.2 mag (Jan. 14, iTelescope Observatory, Siding Spring). It will be observable at 14 mag in good condition from spring to summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  17 40.65  -30 34.9   2.167   1.802    55   15.8   3:55 (286, 35)  
Feb. 17  18  2.57  -30 40.4   2.091   1.773    57   15.6   4:04 (284, 38)  

* 240P/NEAT

It brightened very rapidly up to 13.8 mag in August (Aug. 22, kunihiro Shima). After that, it is fading gradually. Now it is 15.5 mag (Jan. 20, Kunihiro Shima). It will be unobservable in March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   1 10.32   -6 41.8   2.697   2.259    53   15.8  20:32 ( 96, 20)  
Feb. 17   1 21.12   -4 34.2   2.744   2.242    50   15.9  20:22 ( 97, 17)  

* C/2015 V1 ( PanSTARRS )

Now it is 16.2 mag (Jan. 12, Toshihiko Ikemura, Hirohisa Sato). It will be unobservable temporarily soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   0 15.43   -3 20.1   4.980   4.291    41   15.8  20:32 ( 91,  6)  
Feb. 17   0 17.69   -3 39.9   5.070   4.297    34   15.9  20:22 ( 88,  3)  

* C/2014 B1 ( Schwartz )

Now it is 16.4 mag (Jan. 12, Toshihiko Ikemura, Hirohisa Sato). It stays 16-17 mag for a long time from 2016 to 2019. It stays near by the equator.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  10 28.92    5 34.5   8.643   9.594   163   15.8   1:11 (180, 50)  
Feb. 17  10 27.41    5 53.8   8.621   9.598   170   15.8   0:42 (180, 49)  

* C/2017 M4 ( ATLAS )

Now it is 16.1 mag (Jan. 8, Alexander Baransky). It is expected to brighten up to 13-14 mag from 2018 to 2019. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it is not observable until summer in 2018.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  19 26.53   38 32.5   4.933   4.534    60   16.0   3:55 (238,-23)  
Feb. 17  19 30.07   38 39.6   4.874   4.492    61   16.0   4:04 (235,-17)  

* 74P/Smirnova-Chernykh

Now it is 16.1 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). It will be observable at 16 mag in good condition from winter to spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  11 58.15    9 45.9   2.688   3.537   144   16.0   2:40 (180, 45)  
Feb. 17  11 55.55   10 14.5   2.636   3.537   151   16.0   2:10 (180, 45)  

* C/2017 B3 ( LINEAR )

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. 10  14 11.47  -55 32.3   4.877   4.962    89   16.1   3:55 (339, 67)  
Feb. 17  14 11.88  -57  4.8   4.762   4.927    93   16.0   4:04 (352, 68)  

* C/2016 A1 ( PanSTARRS )

Now it is 15.3 mag (Jan. 19, Sandor Szabo). It stays 16 mag for a long time from 2017 to 2018. It is observable in excellent condition in the Northern Hemisphere. It locates very low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   7 55.00   40 43.1   4.512   5.360   146   16.1  22:33 (180, 14)  
Feb. 17   7 46.05   41 32.6   4.586   5.366   138   16.1  21:56 (180, 13)  

* 24P/Schaumasse

It brightened up to 9.7 mag in November (Nov. 16, Juan Jose Gonzalez). Now it is fading rapidly. It has already faded down to 13.0 mag (Feb. 10, Chris Wyatt).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  16 10.95  -10 32.2   1.492   1.614    78   16.2   3:55 (250, 43)  
Feb. 17  16 21.92  -11  5.2   1.479   1.670    82   16.6   4:04 (244, 48)  

* C/2011 KP36 ( Spacewatch )

Now it is 16.9 mag (Jan. 15, Alexander Baransky). It stays 17 mag in 2018.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   3 16.84    0 33.1   6.558   6.566    86   16.3  20:32 (126, 39)  
Feb. 17   3 19.02    0 55.4   6.697   6.597    80   16.3  20:22 (122, 36)  

* C/2016 N4 ( MASTER )

Now it is 15.8 mag (Jan. 14, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this. In the Northern Hemisphere, it stays observable in the northern sky for a long time. It is not observable at all after this in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  20 54.87   67 56.9   3.475   3.491    82   16.3   3:55 (207,-41)  
Feb. 17  21  5.38   69 32.6   3.511   3.518    82   16.3   4:04 (205,-39)  

* (3552) Don Quixote

It will brighten up to 16 mag in spring. In the Southern Hemisphere, it stays observable until August, but it will be unobservable after that. In the Northern Hemisphere, it stays unobservable until June, but it will be observable in good condition after that.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  17 58.59  -47  1.2   2.000   1.646    54   16.9   3:55 (306, 37)  
Feb. 17  18 32.57  -47 35.6   1.921   1.593    55   16.8   4:04 (307, 38)  

* C/2010 U3 ( Boattini )

Now it is 16.4 mag (Jan. 19, Kunihiro Shima). It will pass the perihelion in 2019. However, it has not been brightening since the discovery in 2010. It is observable in good conditioin in the Northern Hemisphere. It is not observable for a long time in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   5 41.47   76  6.9   8.330   8.740   111   16.8  20:32 (179,-21)  
Feb. 17   5 39.08   75 47.3   8.379   8.730   107   16.8  20:22 (178,-21)  

* C/2016 T3 ( PanSTARRS )

Now it is 17.4 mag (Jan. 12, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and will be fainter than 18 mag in April.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   9 41.91  -15 50.4   2.209   3.100   149   16.8   0:24 (180, 71)  
Feb. 17   9 37.63  -15 58.2   2.234   3.137   151   16.9  23:47 (180, 71)  

* C/2014 OE4 ( PanSTARRS )

Now it is 16.3 mag (Jan. 18, Toshihiko Ikemura, Hirohisa Sato). It will be fading gradually after this, and 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 will never be observable again.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  20 46.77   60 25.9   7.068   6.888    75   17.0   3:55 (217,-41)  
Feb. 17  20 58.05   60 54.5   7.112   6.908    74   17.0   4:04 (216,-38)  

* 30P/Reinmuth 1

Now it is 17.3 mag (Jan. 20, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 17 mag in good condition for a while. It will be fainter than 18 mag in May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  15  7.03   -8  0.2   2.105   2.391    94   17.0   3:55 (231, 53)  
Feb. 17  15 12.73   -7 58.1   2.051   2.425    99   17.1   4:04 (220, 57)  

* C/2015 XY1 ( Lemmon )

Now it is 17.0 mag (Jan. 18, Toshihiko Ikemura, Hirohisa Sato). It stays observable at 18 mag for a long time until 2019.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   5 43.10   17  0.8   7.339   7.943   124   17.3  20:32 (177, 38)  
Feb. 17   5 39.35   16 50.4   7.445   7.940   116   17.4  20:22 (170, 38)  

* 145P/Shoemaker-Levy 5

It brightened up to 14.8 mag from autumn to winter (Nov. 21, Hiroshi Abe). Now it is fading. It has already faded down to 16.2 mag (Jan. 18, Toshihiko Ikemura, Hirohisa Sato). It is observable in good 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. 10   5  9.08   37 47.1   1.755   2.379   117   17.4  20:32 (171, 17)  
Feb. 17   5 15.35   37 21.7   1.862   2.414   112   17.6  20:22 (169, 17)  

* 90P/Gehrels 1

Now it is 16.8 mag (Jan. 15, Alexander Baransky). It will be fading after this, and will be fainter than 18 mag in March. 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. 10   5  2.57   34 12.5   2.840   3.396   116   17.5  20:32 (169, 20)  
Feb. 17   5  5.36   33 56.7   2.952   3.419   110   17.6  20:22 (166, 19)  

* 217P/LINEAR

It brightened up to 12.2 mag in August (Aug. 21, Juan Jose Gonzalez). It is fading now. It has already faded down to 16.8 mag (Jan. 24, Alexander Baransky).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10   7 15.01   20 16.8   1.730   2.610   146   17.5  21:53 (180, 35)  
Feb. 17   7 12.20   20 54.6   1.841   2.665   138   17.8  21:23 (180, 34)  

* 103P/Hartley 2

Now it is 18.4 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato). It will be fading slowly after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  11 51.78  -13 49.7   2.466   3.244   135   17.6   2:33 (180, 69)  
Feb. 17  11 46.69  -13 24.8   2.446   3.292   143   17.6   2:01 (180, 69)  

* 66P/du Toit

Now it is 19.1 mag (Jan. 24, Observatoire Chante-Perdrix, Dauban). It will brighten rapidly after this, and will brighten up to 12 mag from April to June. In the Southern Hemisphere, it stays observable in excellent condition. In the Northern Hemisphere, it will be unobservable from April to June when the comet becomes brightest.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  15 56.68  -23  7.4   1.709   1.805    79   18.0   3:55 (263, 53)  
Feb. 17  16 15.99  -25 14.9   1.595   1.747    81   17.6   4:04 (263, 57)  

* C/2017 D3 ( ATLAS )

Now it is 17.4 mag (Jan. 17, Toshihiko Ikemura, Hirohisa Sato). It was observed at 17 mag in former 2017. It will be observable at 18 mag in good condition from winter to spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  12 41.61   10 50.3   4.711   5.443   134   17.7   3:23 (180, 44)  
Feb. 17  12 36.98   12 21.6   4.653   5.465   141   17.7   2:51 (180, 43)  

* 235P/LINEAR

It is observable at 17.5 mag in good condition from February to April. However, now it is 19.2 mag (Jan. 15, Toshihiko Ikemura, Hirohisa Sato), fainter than predicted.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  12  2.91   -8 11.9   1.939   2.740   136   17.8   2:44 (180, 63)  
Feb. 17  12  1.66   -7 57.5   1.877   2.737   143   17.7   2:16 (180, 63)  

* C/2017 E3 ( PanSTARRS )

Now it is 17.0 mag (Jan. 20, Toshihiko Ikemura, Hirohisa Sato). It was observed at 17 mag in 2017. It will be observable at 18 mag in 2018.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  15  4.16  -19 42.7   6.072   6.182    91   17.8   3:55 (245, 61)  
Feb. 17  15  5.19  -19 11.8   5.969   6.197    98   17.8   4:04 (231, 67)  

* C/2018 A3 ( ATLAS )

Now it is 17.4 mag (Jan. 20, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 15.5 mag in January, 2019. It stays observable in excellent condition in the Northern Hemispehre. It is observable only until June, 2018, in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 10  12 47.86   14 20.7   3.775   4.506   132   17.9   3:29 (180, 41)  
Feb. 17  12 41.62   16 14.3   3.654   4.464   140   17.8   2:56 (180, 39)  

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