Weekly Information about Bright Comets (2014 Jan. 11: South)

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Updated on January 13, 2014
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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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* C/2013 R1 ( Lovejoy )

It passed only 0.4 A.U. from the earth, and 0.8 A.U. from the sun in November and December, and brightened up to 4.7 mag (Nov. 28, Juan Jose Gonzalez). Now it is 6.2 mag (Jan. 11, Katsumi Yoshimoto). In the Northern Hemisphere, it keeps observable in excellent condition for a long time until 2014 autumn when the comet will fade out. In the Southern Hemisphere, it is not be observable from mid November to early February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  17 45.60   15 37.3   1.245   0.890    45    6.4   3:14 (267,-23)  
Jan. 18  17 55.48   12 46.6   1.340   0.950    45    7.0   3:23 (265,-16)  

* C/2012 X1 ( LINEAR )

Although it was predicted to be 14 mag, it brightened up to 8 mag in outburst in mid October. It is bright as 8.9 mag still now (Jan. 11, Katsumi Yoshimoto). Mitsunori Tsumura reported the comet got active again in December.It will be observable in excellent condition in 2014 spring. In the Northern Hemisphere, it will be getting higher gradually in the morning sky. In the Southern Hemisphere, it is not observable until 2014 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  16 59.20    9  6.8   2.187   1.694    47    8.6   3:14 (266,-10)  
Jan. 18  17 20.33    7 45.1   2.152   1.666    48    8.5   3:23 (265, -6)  

* C/2013 V3 ( Nevski )

It brightened very rapidly in mid November, from 15 mag to 9 mag only within a week. Now it is bright as 10.7 mag but diffuse (Jan. 4, Carlos Labordena). It seems to keep 10-11 mag for a while after this. 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)  
Jan. 11  11 18.45   39 53.4   0.906   1.702   128   11.1   3:14 (189, 15)  
Jan. 18  11 22.92   43 31.3   0.938   1.756   132   11.3   3:23 (182, 12)  

* 154P/Brewington

It brightened very rapidly, and brightened up to 10.5 mag from autumn to winter. It is bright as 11.8 mag still now (Dec. 29, J. P. Navarro Pina). It will be fading after this. In the Northern Hemisphere, it keeps observable in excellent condition until May when it becomes fainter than 18 mag. It will not be observable after this in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   0 12.06   21 27.2   1.466   1.641    81   11.6  21:01 (124,  8)  
Jan. 18   0 30.60   23 22.1   1.526   1.658    79   11.9  20:56 (124,  6)  

* C/2012 K1 ( PanSTARRS )

Now it is bright as 12.8 mag (Jan. 7, Taras Prystavski). It is expected to brighten up to 5-6 mag in 2014 autumn. In the Northern Hemisphere, it will be getting higher gradually after this, and it keeps observable in good condition for a long time. In the Southern Hemisphere, it will not be observable until 2014 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  16 25.60   11 19.1   3.825   3.373    55   12.2   3:14 (259, -5)  
Jan. 18  16 28.90   11 57.8   3.658   3.295    61   12.0   3:23 (254,  2)  

* 290P/2013 N1 ( Jager )

First return of a new periodic comet discovered in 1998. It brightened up to 10 mag at the discovery. Now it is 11.8 mag (Jan. 4, Marco Goiato). A bit fainter than originally expected. But in the Northern Hemisphere, it keeps observable in excellent condition from autumn to spring. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   6 22.73   36  7.8   1.281   2.230   159   12.2  22:59 (180, 19)  
Jan. 18   6 17.91   34 35.6   1.288   2.214   153   12.2  22:27 (180, 21)  

* C/2012 V2 ( LINEAR )

It became much brighter than expected, and reached up to 8.5 mag (Aug. 15, Alexandre Amorim). Now it is fading, but it is bright as 12.8 mag still now (Jan. 5, Taras Prystavski). In the Southern Hemisphere, it will keep observable in good condition for a long time until 2014 summer when the comet fades out. It will never be observable again in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  15 41.41  -66 22.2   2.851   2.458    56   13.7   3:14 (331, 37)  
Jan. 18  16  0.89  -66 55.8   2.884   2.527    59   14.0   3:23 (331, 39)  

* C/2011 J2 ( LINEAR )

Now it is 12.8 mag and visible visually (Dec. 5, Juan Jose Gonzalez). It keeps 13-14 mag and observable in good condition in the Northern Hemisphere for a long time from 2013 to 2014. In the Southern Hemisphere, it is not observable until 2014 autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  22 28.90   73 57.4   3.134   3.447   100   13.7  21:01 (161,-33)  
Jan. 18  22 50.51   70 54.9   3.202   3.450    96   13.8  20:56 (157,-32)  

* 17P/Holmes

It brightened up to 2 mag by unusual major outburst in 2007. It will return in 2014. It will be 14 mag at best by normal prediction. But actually, it is already very bright as 13.5 mag (Nov. 25, Hidetaka Sato). It will be unobservable soon, and keeps unobservable until May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  21  0.40  -18 11.7   3.021   2.140    21   14.0  21:01 ( 63, -6)  
Jan. 18  21 15.06  -16 29.9   3.035   2.125    18   13.9  20:56 ( 63, -8)  

* C/2006 S3 ( LONEOS )

It brightened up to 11-12 mag in 2012. Now it is 14.0 mag (Dec. 31, Taras Prystavski). It will be observable in good condition at 14 mag until 2014 early summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  13 26.93  -14 35.4   6.966   6.950    84   13.9   3:14 (253, 46)  
Jan. 18  13 24.88  -14 36.4   6.870   6.983    92   13.9   3:23 (244, 54)  

* 29P/Schwassmann-Wachmann 1

Appearing in the morning sky. Now it is faint as 16.9 mag (Dec. 22, Martin Masek).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  15 35.65  -28  4.0   6.718   6.171    52   14.1   3:14 (287, 27)  
Jan. 18  15 39.99  -28 24.6   6.623   6.170    58   14.0   3:23 (284, 34)  

* C/2010 S1 ( LINEAR )

Now it is 12.9 mag (Nov. 27, Sandor Szabo). It keeps bright at 13-14 mag for a long time until 2014. It keeps observable for a long time in the Northern Hemisphere, although it becomes unobservable temporarily in January. In the Southern Hemisphere, it keeps unobservable until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  19 37.11    5 38.0   6.985   6.130    27   14.0  21:01 ( 68,-37)  
Jan. 18  19 39.92    5 19.6   7.010   6.144    26   14.1   3:23 (289,-33)  

* C/2013 V1 ( Boattini )

Now it is 14.2 mag and visible visually (Jan. 4, Chris Wyatt). It keeps 14 mag for a long time until 2014 summer. It keeps observable in good condition in the Northern Hemisphere. It is observable only until February in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   2 58.91    7 33.2   1.517   2.114   113   14.2  21:01 (151, 43)  
Jan. 18   2 51.04   11  5.2   1.560   2.061   105   14.1  20:56 (144, 36)  

* C/2013 A1 ( Siding Spring )

Now it is 14.3 mag and visible visually (Dec. 25, Alan Hale). It is expected to brighten up to 7.5 mag and to be observable in excellent condition from summer to autumn in 2014 in the Southern Hemisphere. The condition is bad in the Northern Hemisphere. It will pass extremely close to Mars in 2014 October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   3 14.11  -38  2.9   3.653   3.873    95   14.4  21:01 ( 73, 75)  
Jan. 18   3  5.15  -37 13.4   3.674   3.803    89   14.3  20:56 ( 77, 69)  

* 4P/Faye

It reaches up to 12 mag in 2014 spring. But the condition in this apparition is bad. It locates low around the brightest days. Now it is 15.5 mag (Dec. 20, F. Garcia). It is already unobservable in the Southern Hemisphere. It will be unobservable in late January also in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  21 35.46   -9 37.6   2.887   2.128    32   14.7  21:01 ( 75, -4)  
Jan. 18  21 49.87   -8 42.4   2.890   2.089    29   14.5  20:56 ( 75, -6)  

* 134P/Kowal-Vavrova

Now it is 16.0 mag (Nov. 30, Ken-ichi Kadota). It is expected to brighten up to 13 mag and to be observable in excellent condition from spring to summer in 2014.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  13 27.30  -10 43.1   2.666   2.781    86   14.7   3:14 (249, 44)  
Jan. 18  13 35.09  -11 22.5   2.555   2.761    91   14.6   3:23 (243, 50)  

* 2P/Encke

It brightened rapidly as expected. It passed the perihelion on Nov. 21, and brightened up to 7.8 mag (Nov. 18, Todd Augustyniak). It will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  19 16.05  -27 14.9   2.102   1.129     6   14.7   3:14 (316,-12)  
Jan. 18  19 38.90  -26 24.4   2.206   1.237     7   15.5   3:23 (313,-11)  

* 117P/Helin-Roman-Alu 1

It keeps bright as 13-14 mag for a long time from 2013 to 2014. Now it is not observable. But it will appear in the morning sky again in 2014 February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  18  7.84  -26 29.1   3.992   3.079    18   14.8   3:14 (305, -2)  
Jan. 18  18 20.13  -26 35.6   3.954   3.075    23   14.8   3:23 (301,  2)  

* (596) Scheila

Big asteroid discovered in 1906. It suddenly showed the cometary activity on Dec. 11, 2010, probably due to an impact of a small object. It has already turned to be stellar.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   0 29.91   -8 34.2   3.354   3.212    73   15.0  21:01 (102, 31)  
Jan. 18   0 35.59   -7 26.4   3.458   3.221    67   15.0  20:56 (100, 26)  

* 169P/NEAT

It will pass the perihelion on Feb. 15, and will brighten up to 12 mag. Now it is not observable. It will appear in the evening sky in mid February in the Northern Hemisphere, or in early March in the Southern Hemisphere. Then it keeps observable while the comet will fade out very rapidly.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  20 24.97  -15 55.8   1.804   0.887    14   16.0  21:01 ( 60,-13)  
Jan. 18  20 56.58  -14 52.7   1.714   0.804    14   15.1  20:56 ( 62,-12)  

* 52P/Harrington-Abell

Now it is 14.8 mag (Dec. 31, Taras Prystavski). It keeps 15 mag until March, and will be 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)  
Jan. 11   4  6.30   38 30.6   1.026   1.849   133   15.4  21:01 (176, 16)  
Jan. 18   4  9.76   37 34.2   1.053   1.832   128   15.4  20:56 (172, 17)  

* C/2012 K6 ( McNaught )

It brightened up to 14.0 mag from spring to summer (June 11, Sandor Szabo). Now it is 15.0 mag, much brighter than origianlly predicted (Dec. 11, Hidetaka Sato). In the Northern Hemisphere, it will be observable at 15-16 mag in excellent condition until spring. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  13 51.52    8 14.9   3.907   3.992    87   15.5   3:14 (237, 27)  
Jan. 18  13 50.12    9 55.7   3.812   4.027    95   15.5   3:23 (228, 32)  

* C/2013 N4 ( Borisov )

Now it is 15.7 mag (Jan. 5, Taras Prystavski). It will be fading slowly until May when it becomes fainter than 18 mag. It keeps observable in good condition in the Southern Hemisphere. It keeps locating extremely low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  13 23.95  -39  8.5   2.371   2.358    77   15.5   3:14 (290, 56)  
Jan. 18  13 27.27  -41 29.5   2.366   2.434    82   15.7   3:23 (294, 63)  

* C/2009 F4 ( McNaught )

Now it is 14.6 mag (Dec. 29, Taras Prystavski). It will be fading after this, but it keeps brighter than 18 mag until 2015 spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   3  7.78  -20 31.2   7.301   7.592   103   15.8  21:01 (126, 68)  
Jan. 18   3  6.18  -19 39.7   7.427   7.624    97   15.9  20:56 (118, 63)  

* C/2012 F6 ( Lemmon )

It approached to the sun down to 0.73 A.U. on Mar. 24, and brightened up to 4.7 mag (Mar. 11, Michael Mattiazzo). Now it is fading. It has already faded down to 15.1 mag (Dec. 15, F. Garcia). In the Northern Hemisphere, it keeps observable in good condition while fading gradually. In the Southern Hemisphere, it will never be observable again.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  20  5.17   49 24.8   4.436   4.232    71   16.1  21:01 (128,-48)  
Jan. 18  20 13.25   49 56.1   4.532   4.307    70   16.3  20:56 (128,-50)  

* 84P/Giclas

Now it is 15.4 mag (Dec. 30, Taras Prystavski). It tends to be brightest 4 months after the perihelion passage. It will reach up to 15.5 mag from autumn to winter, and will be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   6  1.81   20 31.9   1.399   2.347   159   16.1  22:38 (180, 34)  
Jan. 18   5 57.81   21  2.3   1.468   2.381   151   16.3  22:06 (180, 34)  

* C/2012 F3 ( PanSTARRS )

It is expected to brighten up to 13 mag and to be observable in good condition in 2015. Now it is 16.7 mag (Dec. 11, Hidetaka Sato). In 2014, it will be observable at 15 mag in good condition from winter to summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  13 48.58   -4 47.4   5.298   5.279    83   16.3   3:14 (247, 36)  
Jan. 18  13 51.97   -4 51.3   5.145   5.236    89   16.2   3:23 (240, 42)  

* C/2012 S1 ( ISON )

It was expected to be a great comet as it approached to the sun down to only 0.01 A.U. on Nov. 28. It brightened up to -2.5 mag at best. However, the comet's nucleus disrupted at the perihelion passage. After that, the dust remnant had been visible until Dec. 6 on the STEREO spacecraft images. However, the dust remnant has not been detected by CCD observations on the ground. The nucleus is not detected, fainter than 18 mag (Dec. 13, Lorenzo Comolli). But visual observers reported it was visible at 7.5 mag on Dec. 6 (Piotr Guzik), 7.2 mag on Dec. 7 (Juan Jose Gonzalez), and 9.6 mag on Dec. 9 (Jakub Cerny). It approached to the earth down to 0.4 A.U. from mid December to early January, but it was not detected. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   2 56.72   81 42.5   0.590   1.342   114   16.4  21:01 (177,-26)  
Jan. 18   3 48.13   70 23.3   0.738   1.485   118   17.8  20:56 (175,-15)  

* C/2013 V2 ( Borisov )

Now it is 16.3 mag (Dec. 31, Taras Prystavski). It keeps 16 mag for a long time until 2015 summer. It keeps observable in good condition in the Northern Hemisphere. It becomes observable only after 2015 in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   4 46.72   53 32.3   3.544   4.305   135   16.6  21:23 (180,  1)  
Jan. 18   4 42.22   53 32.9   3.567   4.270   130   16.6  20:56 (179,  1)  

* P/2012 B1 ( PanSTARRS )

It will be observable at 14-16 mag for a long time from 2013 to 2014. Now it is getting higher in the morning sky again.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  15 34.97  -20 18.0   4.439   3.945    54   16.7   3:14 (279, 23)  
Jan. 18  15 42.08  -20 50.4   4.360   3.954    59   16.6   3:23 (276, 30)  

* C/2011 L4 ( PanSTARRS )

It passed the perihelion on Mar. 10, and brightened up to 0-1 mag. Now it is fading. It has already faded down to 15.6 mag (Jan. 7, Taras Prystavski). In the Northern Hemisphere, it is getting higher in the morning sky again. But it will be fainter than 18 mag in late January. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  17  4.05   26 26.3   5.142   4.722    59   16.7   3:14 (251,-20)  
Jan. 18  17  8.32   26 52.9   5.165   4.798    62   16.8   3:23 (247,-14)  

* C/2012 L2 ( LINEAR )

It brightened up to 9-10 mag in 2013 spring. Now it is fading. It has faded down to 15.8 mag in October (Oct. 7, Hidetaka Sato). In the Southern Hemisphere, it keeps observable for a long time until the comet fades out, although it keeps locating low. However, it has not been observed after November. It will never be observable again in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  16 33.55  -66 13.4   3.955   3.443    52   16.7   3:14 (332, 32)  
Jan. 18  16 49.01  -66 34.2   3.984   3.512    54   16.8   3:23 (332, 34)  

* C/2012 J1 ( Catalina )

It brightened up to 12-13 mag from autumn to winter in 2012. Now it is fading. It has already faded down to 16.8 mag (Dec. 23, J. Lozano). It keeps observable for a long time until March when the comet becomes fainter than 18 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   5 39.77   -2 22.6   4.035   4.865   144   17.0  22:16 (180, 57)  
Jan. 18   5 37.09   -2 25.1   4.132   4.911   138   17.1  21:46 (180, 57)  

* 119P/Parker-Hartley

Now it is 17.7 mag (Dec. 16, E. Cozzi). It keeps 17 mag for a long time from 2013 summer to early 2015.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   1 48.20   12 51.2   2.742   3.058    99   17.0  21:01 (135, 30)  
Jan. 18   1 53.08   13  5.8   2.834   3.053    93   17.0  20:56 (132, 27)  

* P/2013 TL117 ( Lemmon )

Now it is 17.8 mag (Dec. 1, J. De Queiroz, R. Behrend). It keeps close to the earth around 0.7 a.u. until spring. It will brighten up to 16.5 mag in February and March, and will be 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)  
Jan. 11   0 57.64   23 16.5   0.705   1.229    91   17.1  21:01 (132, 14)  
Jan. 18   1 12.85   24 59.5   0.695   1.193    88   17.0  20:56 (132, 11)  

* C/2013 V5 ( Oukaimeden )

Now it is 17.6 mag (Dec. 7, J. F. Hernandez). It is expected to brighten up to 6 mag in 2014 autumn. At this time, it keeps observable while brightening gradually until April when it becomes 16 mag.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   6 13.39   22 37.9   2.999   3.948   162   17.3  22:49 (180, 32)  
Jan. 18   6  0.75   22 23.8   2.970   3.869   152   17.2  22:09 (180, 33)  

* 124P/Mrkos

Now it is 17.8 mag (Dec. 17, E. Cozzi). It will approach to the earth down to 0.68 a.u., brighten up to 16 mag, and will be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  12 29.44   33 12.7   1.211   1.841   113   17.5   3:14 (205, 17)  
Jan. 18  12 33.78   32 26.3   1.127   1.814   118   17.4   3:23 (198, 20)  

* C/2013 V4 ( Catalina )

Now it is 17.5 mag (Dec. 7, Catalina Sky Survey). It keeps 15-16 mag for a long time from 2015 to 2016. In this winter, it is observable at 17.5 mag until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   2 53.45   -4 13.5   6.608   6.973   107   17.5  21:01 (141, 53)  
Jan. 18   2 52.07   -3 31.8   6.682   6.940   101   17.5  20:56 (133, 49)  

* 266P/2012 P1 ( Christensen )

Now it is 19.3 mag (Dec. 14, W. Hasubick). In this winter, it is observable at 17.5 mag in good condition until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  10 58.24   10  3.7   1.746   2.481   128   17.7   3:14 (188, 45)  
Jan. 18  10 57.63   10  6.5   1.695   2.496   135   17.6   3:10 (180, 45)  

* C/2013 G7 ( McNaught )

It keeps 17-18 mag for a long time from 2013 to 2014. It is observable in excellent condition in the Southern Hemisphere. It is not observable in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11  14 42.20  -42 52.4   5.087   4.707    62   17.8   3:14 (299, 42)  
Jan. 18  14 42.15  -44 22.4   4.978   4.701    68   17.7   3:23 (300, 49)  

* 291P/2013 N2 ( NEAT )

Now it is 16.8 mag (Dec. 23, Mt. Lemmon Survey). It will be observable at 17 mag in excellent condition from autumn to winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   2 48.02   15 41.3   2.039   2.598   113   17.7  21:01 (152, 34)  
Jan. 18   2 52.73   15 47.6   2.126   2.602   107   17.8  20:56 (147, 32)  

* C/2010 U3 ( Boattini )

Now it is 17.9 mag (Dec. 8, Hidetaka Sato). It will brighten up to 14 mag around the perihelion passage in 2019. In 2013, it will be observable in good condition at 18 mag from summer to winter. It locates low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   2 42.25   27  0.6  13.053  13.506   115   17.9  21:01 (155, 23)  
Jan. 18   2 41.67   27  0.7  13.135  13.477   108   17.9  20:56 (150, 21)  

* C/2012 A1 ( PanSTARRS )

Now it is 18.6 mag (Nov. 24, A. Maury, J.-F Soulier, J. G Bosch). It keeps 18-19 mag for a long time until 2015. It is observable at 18 mag in good condition in this winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Jan. 11   5 49.72    9 15.6   6.716   7.607   153   17.9  22:26 (180, 46)  
Jan. 18   5 44.87    8 54.5   6.775   7.608   145   18.0  21:53 (180, 46)  

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