Weekly Information about Bright Comets (2015 Feb. 14: South)

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Updated on February 14, 2015
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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/2014 Q2 ( Lovejoy )

It brightened up to 3.7 mag and became a naked eye comet in mid January (Jan. 13, Marek Biely). It is bright as 5.0 mag still now (Feb. 13, Maik Meyer). It keeps brightening even after the perihelion passage. However, it will be getting fainter gradually after this. In the Northern Hemisphere, it keeps observable in good condition after this until the comet fades out. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   1 49.08   48  8.9   1.023   1.310    81    5.3  20:27 (143,-11)  
Feb. 21   1 39.38   51 31.7   1.158   1.332    76    5.6  20:17 (143,-16)  

* 88P/Howell

Now it is bright as 12.7 mag (Jan. 24, Chris Wyatt). It will brighten up to 8-9 mag in 2015 spring. In the Southern Hemisphere, it will be getting higher gradually after this. In the Northern Hemisphere, it keeps extremely low and hard to observe until June. It will be observable in good condition after June while the comet will be fading gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  18 52.29  -23 53.0   2.032   1.470    42   10.2   4:00 (285, 22)  
Feb. 21  19 18.28  -23 28.2   1.981   1.443    43   10.0   4:09 (283, 24)  

* 15P/Finlay

It brightened very rapidly in outburst up to 8.8 mag in mid December (Dec. 19, Marco Goiato). Then it faded down to 10.7 mag (Jan. 14, Chris Wyatt). However, it brightened in outburst again on Jan. 16, and brightened up to 7.0 mag (Jan. 17, Maik Meyer). Now it is 11.7 mag and diffuse (Feb. 9, Chris Wyatt). In the Northern Hemisphere, it will be geting higher gradually. In the Southern Hemisphere, it keeps locating extremely low after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   0 57.23   10 11.5   1.515   1.203    52   11.0  20:27 (107,  5)  
Feb. 21   1 25.50   13 28.0   1.576   1.261    53   11.5  20:17 (111,  5)  

* C/2013 A1 ( Siding Spring )

The brightness evolution has slowed down before the perihelion passage, and it faded down to 11.6 mag in late October (Oct. 26, Todd Augustyniak). However, an outburst occured around Nov. 10-12, and it brightened by 2 mag. It is bright as 10.9 mag still now (Jan. 24, Taras Prystavski). In the Northern Hemisphere, it will be observable in excellent condition after this while the comet will be fading. It is observable in the morning low sky until early April also in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  18  4.73   18  8.5   2.340   2.093    63   11.6   4:00 (242,  7)  
Feb. 21  18  2.64   21 43.3   2.291   2.162    69   11.6   4:09 (234, 11)  

* 7P/Pons-Winnecke

Now it is 16.0 mag (Dec. 22, Ken-ichi Kadota). It will brighten very rapidly, and will brighten up to 11 mag from January to February. In the Southern Hemisphere, it will be observable in the morning sky after February while the comet will be fading. It is hardly observable in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  20  4.95  -21 39.9   2.063   1.252    25   12.0   4:00 (292,  6)  
Feb. 21  20 32.42  -21 39.7   2.067   1.267    26   12.2   4:09 (291,  8)  

* C/2012 K1 ( PanSTARRS )

It brightened up to 6.9 mag in autumn (Oct. 17, Marco Goiato). Now it is fading. But it is bright as 12.6 mag still now (Feb. 9, Chris Wyatt). In the Southern Hemisphere, it is getting lower and it will be unobservable temporarily in March. But it will be observable in good condition again after April. It will be observable again in mid June also in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   0 15.06  -23 24.3   3.449   2.715    36   12.1  20:27 ( 72, 15)  
Feb. 21   0 18.09  -22 19.8   3.591   2.796    31   12.3  20:17 ( 71, 12)  

* C/2013 US10 ( Catalina )

It brightened up to 13.6 mag until the end of 2014, brighter than originally expected (Dec. 19, Chris Wyatt). It is expected to brighten up to 4 mag from autumn to winter in 2015. Now it is not observable. In the Southern Hemisphere, it will be observable in good condition again after late March. In the Northern Hemisphere, it is hardly observable until 2015 December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  22 43.02  -22 54.6   4.929   3.990    16   13.0  20:27 ( 60, -2)  
Feb. 21  22 47.13  -22 37.8   4.865   3.913    14   12.9  20:17 ( 58, -5)  

* C/2014 R1 ( Borisov )

It brightened up to 10.6 mag from autumn to winter (Nov. 29, Seiichi Yoshida). Now it is 12.8 mag (Jan. 24, Chris Wyatt). It will be fading graudually after this. But it keeps observable for a long time until the comet fades out.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  16 52.06  -13 56.1   1.885   1.832    71   13.2   4:00 (258, 41)  
Feb. 21  17  3.61  -14 11.2   1.880   1.897    75   13.5   4:09 (253, 46)  

* 19P/Borrelly

Now it is 15.1 mag (Feb. 1, Taras Prystavski). It will brighten up to 10.5 mag in 2015 spring. But the condition of this apparition is bad. It is already unobservable in the Northern Hemisphere. It will be unobservable in mid March also in the Southern Hemisphere. In the Northern Hemisphere, it will be observable after 2015 autumn while the comet will be fading.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  23 49.48  -22 50.2   2.563   1.782    30   13.8  20:27 ( 70, 10)  
Feb. 21   0  5.78  -20 16.3   2.542   1.735    28   13.5  20:17 ( 72,  9)  

* C/2012 F3 ( PanSTARRS )

Now it is 14.5 mag (Jan. 20, Taras Prystavski). In 2015, it keeps 13 mag and will be observable in good condition for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  18  4.07  -13 29.1   3.971   3.490    54   13.9   4:00 (269, 26)  
Feb. 21  18 13.61  -13 16.2   3.886   3.481    59   13.9   4:09 (264, 31)  

* 29P/Schwassmann-Wachmann 1

Outburst occured on Feb. 3, and it is bright as 13.8 mag (Richard Miles). It is getting higher gradually in the morning sky.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  17 37.21  -30 34.3   6.503   6.069    59   13.9   4:00 (283, 39)  
Feb. 21  17 41.53  -30 40.7   6.401   6.067    66   13.9   4:09 (280, 46)  

* 32P/Comas Sola

Now it is 13.8 mag (Jan. 20, Taras Prystavski). It is fainter than originally predicted by 2 mag. In the Northern Hemisphere, it keeps observable at 14 mag in excellent condition from 2014 summer to 2015 spring. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  11 49.42   19 12.1   1.354   2.265   150   13.9   2:16 (180, 36)  
Feb. 21  11 45.34   19 43.7   1.352   2.294   156   14.0   1:45 (180, 35)  

* 17P/Holmes

It brightened up to 2 mag by unusual major outburst in 2007. It brightened up to 12.6 mag in this apparition (June 25, Taras Prystavski). It faded down to 17-18 mag, but it suddenly brightened in outburst on Jan. 26, and brightened up to 13.2 mag (Jan. 29, Uwe Pilz). Now it is 14.7 mag (Feb. 7, Sandor Szabo). In the Northern Hemisphere, it keeps observable in good condition. In the Southern Hemisphere, it keeps extremely low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   4 15.38   40 29.3   2.684   3.071   103   14.1  20:27 (160, 11)  
Feb. 21   4 21.29   39 46.9   2.805   3.102    98   14.6  20:17 (157, 10)  

* 6P/d'Arrest

It will brighten up to 11 mag in spring. But the condition is bad in this apparition. In the Southern Hemisphere, it will become observable in the morning extremely low sky after late April. It will not be observable until late July in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  20 59.50  -14  4.8   2.326   1.375    11   14.6   4:00 (294, -9)  
Feb. 21  21 24.30  -13 19.1   2.313   1.366    12   14.1   4:09 (292, -7)  

* C/2014 Q1 ( PanSTARRS )

It will approach to the sun down to 0.3 a.u. in 2015 July, and it is expected to be bright. Now it is 15.6 mag (Jan. 13, Yasukazu Ikari). Hard to observe for a while after this. In the Southern Hemisphere, it will be observable after mid July in 2015, and keeps observable while the comet will be fading gradually. It will not be observable after this in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  23 24.72  -15  0.3   3.599   2.722    23   14.6  20:27 ( 72,  1)  
Feb. 21  23 31.70  -13 38.2   3.540   2.624    18   14.4  20:17 ( 72, -2)  

* C/2006 S3 ( LONEOS )

It brightened up to 11-12 mag in 2012. It has already faded down to 15.5 mag (Jan. 17, Taras Prystavski). It keeps observable at 15 mag in good condition until 2015 summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  11 47.89   -9 48.1   8.185   8.988   142   15.1   2:15 (180, 65)  
Feb. 21  11 43.86   -9 30.7   8.155   9.025   150   15.1   1:43 (180, 65)  

* 201P/LONEOS

Now it is 14.6 mag (Jan. 21, Catalina Sky Survey). It will be observable at 14 mag in excellent condition in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   2 23.23   20 27.3   1.249   1.385    75   15.1  20:27 (128, 14)  
Feb. 21   2 48.00   22 39.7   1.296   1.407    74   15.3  20:17 (131, 14)  

* C/2014 N3 ( NEOWISE )

Now it is 14.5 mag (Dec. 24, Taras Prystavski). It keeps 15 mag for a long time from 2014 to 2015. It is observable in excellent condition in 2014 in the Southern Hemisphere, or in 2015 in the Northern Hemisphere. It becomes unobservable temporarily from March to May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   0 31.45   -5 50.4   4.582   3.890    40   15.2  20:27 ( 89,  9)  
Feb. 21   0 36.09   -4 11.3   4.649   3.886    35   15.2  20:17 ( 89,  5)  

* C/2014 AA52 ( Catalina )

Now it is 15.3 mag (Jan. 17, Taras Prystavski). The brightness evolution is somewhat slow. It keeps 15-16 mag for a long time from 2014 autumn to 2015 autumn. In the Southern Hemisphere, it keeps observable in excellent condition for a long time. In the Northern Hemisphere, it is unobservable until 2015 June.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   0 56.26  -49 56.3   2.444   2.009    52   15.2  20:27 ( 49, 34)  
Feb. 21   0 53.62  -46 25.1   2.511   2.004    48   15.3  20:17 ( 52, 30)  

* 110P/Hartley 3

Now it is 14.3 mag (Feb. 7, Sandor Szabo). It keeps 15 mag until February, and it will be 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. 14   6 19.23   22  3.5   1.752   2.501   129   15.4  20:43 (180, 33)  
Feb. 21   6 20.42   21 33.1   1.828   2.507   122   15.5  20:17 (180, 33)  

* C/2014 A4 ( SONEAR )

Now it is 15.5 mag (Jan. 16, Taras Prystavski). It will brighten up to 14 mag from 2015 to 2016. It is observable in good condition 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. 14   2 50.97  -12 55.3   4.696   4.515    73   15.4  20:27 (105, 41)  
Feb. 21   2 49.17  -11 32.9   4.786   4.493    66   15.4  20:17 (103, 37)  

* C/2014 W11 ( PanSTARRS )

Brightening very rapidly. Now it is so bright as 14.5 mag and visible visually (Feb. 7, Mike Wolle). It keeps observable at 15 mag in good condition from winter to spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   8 58.70   10 28.1   2.576   3.547   167   15.6  23:22 (180, 45)  
Feb. 21   8 54.85   10 25.0   2.588   3.534   160   15.5  22:50 (180, 45)  

* C/2010 S1 ( LINEAR )

Now it is 14.5 mag (Nov. 19, Taras Prystavski). It will be observable at 15-16 mag in good condition again in 2015.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  18 55.86  -16 30.3   8.073   7.365    41   15.5   4:00 (279, 17)  
Feb. 21  18 57.51  -16 43.4   8.014   7.393    48   15.6   4:09 (274, 24)  

* C/2013 V2 ( Borisov )

Now it is 15.3 mag (Jan. 24, Taras Prystavski). In the Northern Hemisphere, it keeps 15-16 mag and observable in excellent condition for a long time until early summer in 2015. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  13 35.62   34  6.4   3.031   3.684   124   15.6   4:00 (180, 21)  
Feb. 21  13 34.01   34 24.2   3.000   3.703   129   15.6   3:33 (180, 21)  

* 218P/LINEAR

Now it is 17.4 mag (Jan. 18, Catalina Sky Survey). It is expected to brighten rapidly and will be observable in good condition at 13 mag from March to May.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  14 24.29  -14 12.3   0.800   1.435   106   16.2   4:00 (212, 66)  
Feb. 21  14 49.58  -15 43.4   0.728   1.390   107   15.7   4:09 (207, 69)  

* 22P/Kopff

Now it is 15.6 mag (Jan. 19, Catalina Sky Survey). It will brighten up to 11 mag in 2015 autumn. In this apparition, it is observable until the highlight while the comet is brightening.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  13 13.87   -1 50.2   2.038   2.746   126   16.1   3:40 (180, 57)  
Feb. 21  13 14.29   -1 31.9   1.924   2.704   133   15.8   3:13 (180, 57)  

* (3200) Phaethon

Now it is 16.6 mag (Jan. 29, Catalina Sky Survey). It will pass the perihelion on Mar. 15. In the Northern Hemispehre, it keeps observable in good condition until late February. In the Southern Hemisphere, it keeps observable until mid February, but it locates low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   1  4.33    6  2.0   0.886   0.832    52   16.1  20:27 (104,  9)  
Feb. 21   0 58.45    3 32.7   0.866   0.690    43   15.9  20:17 ( 98,  6)  

* 70P/Kojima

Now it is 15.7 mag (Jan. 17, Taras Prystavski). It will brighten up to 16 mag and will be observable in excellent condition in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  12 21.45    6 21.6   1.352   2.213   141   15.9   2:48 (180, 49)  
Feb. 21  12 19.66    7  7.9   1.329   2.236   149   15.9   2:19 (180, 48)  

* C/2013 V4 ( Catalina )

Now it is 15.8 mag (Jan. 11, Y. Sugiyama). It keeps observable at 15-16 mag for a long time from 2015 to 2016. In the Northern Hemisphere, it is observable in excellent condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   2 55.70   29 56.7   5.467   5.480    85   16.1  20:27 (140, 11)  
Feb. 21   2 56.82   30 26.9   5.564   5.464    79   16.1  20:17 (137,  9)  

* C/2013 X1 ( PanSTARRS )

Now it is 15.7 mag (Jan. 16, Taras Prystavski). It will pass close to the earth from spring to summer in 2016, and it is expected to be observable at 6-7 mag in good condition. In the Northern Hemispehre, it keeps observable in good condition until 2015 spring when the comet will brighten up to 15.5 mag. In the Southern Hemisphere, it keeps low for a long time until 2016 spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   5  1.05   35 33.7   4.829   5.285   112   16.2  20:27 (167, 18)  
Feb. 21   4 56.08   35 14.4   4.885   5.221   104   16.1  20:17 (162, 17)  

* 4P/Faye

Now it is 14.7 mag (Jan. 20, Taras Prystavski). It keeps observable for a long time after this while the comet will be fading gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   9 27.79    2 57.6   1.880   2.854   168   16.2  23:50 (180, 52)  
Feb. 21   9 22.16    3 45.8   1.929   2.896   165   16.3  23:17 (180, 51)  

* C/2013 V5 ( Oukaimeden )

It brightened up to 6.5 mag in September (Sept. 21, Marco Goiato). Now it is fading. It has already faded down to 15.6 mag (Jan. 20, Taras Prystavski). It keeps observable in good condition after this, while the comet will be fading gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  15 45.01    7 56.8   2.222   2.472    92   16.3   4:00 (222, 37)  
Feb. 21  15 36.93   10 23.8   2.181   2.565   101   16.4   4:09 (209, 40)  

* 116P/Wild 4

Now it is 17.5 mag (Jan. 11, F. Garcia). It will brighten up to 13 mag in 2016. In the Northern Hemisphere, it will be observable in excellent condition in this winter. It locates somewhat low in the Southern Hemisphere. It is fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   5 41.13   27 51.7   2.421   3.049   120   16.3  20:27 (175, 27)  
Feb. 21   5 41.22   27 43.5   2.484   3.023   113   16.3  20:17 (170, 27)  

* 269P/2012 R2 ( Jedicke )

Now it is 15.4 mag (Jan 17, Mt. Lemmon Survey). It will brighten up to 16 mag in winter, and will be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   7 58.37   13 27.5   3.206   4.112   153   16.4  22:21 (180, 42)  
Feb. 21   7 55.84   13 36.8   3.261   4.117   145   16.4  21:52 (180, 41)  

* C/2014 R4 ( Gibbs )

It brightened up to 15.4 mag in autumn (Nov. 19, Taras Prystavski). But it was extremely diffuse. It was reported so faint as 20 mag after December. It keeps observable in excellent condition in the Southern Hemisphere. But it locates low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   8 42.51  -38 59.3   1.601   2.319   125   16.7  23:05 (  0, 86)  
Feb. 21   8 35.02  -39 14.1   1.664   2.371   124   16.9  22:30 (  0, 86)  

* 40P/Vaisala 1

Now it is 15.8 mag (Jan. 2, Ken-ichi Kadota). It will be observable at 16-17 mag in good condition from winter to spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  16 49.13  -11 11.6   2.089   2.030    72   16.7   4:00 (254, 40)  
Feb. 21  17  1.53  -11  9.4   2.049   2.061    76   16.8   4:09 (249, 45)  

* C/2013 G9 ( Tenagra )

Now it is 16.4 mag (Jan. 20, Taras Prystavski). It keeps 17-18 mag for a long time from 2014 to 2016.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  12 48.22  -23 59.2   4.748   5.342   122   16.9   3:15 (180, 79)  
Feb. 21  12 40.06  -24  4.5   4.651   5.345   130   16.8   2:39 (180, 79)  

* C/2014 W2 ( PanSTARRS )

Now it is 16.8 mag (Jan. 23, Catalina Sky Survey). It keeps 13 mag for a long time from 2015 to 2016, and will be observable in excellent condition in the Northern Hemisphere. In the Southern Hemisphere, it is observable only until mid 2015 March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   3 40.94   22 45.2   4.521   4.685    93   17.0  20:27 (144, 23)  
Feb. 21   3 40.05   23 22.5   4.591   4.634    86   17.0  20:17 (141, 20)  

* C/2013 G3 ( PanSTARRS )

Now it is 17.7 mag (Jan. 20, Taras Prystavski). It was observed at 17 mag in 2014 summer. In the Northern Hemisphere, it is observable at 17.5 mag in excellent condition also in 2015. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  19 56.19   34  4.1   4.427   3.933    54   17.2   4:00 (243,-23)  
Feb. 21  20  7.91   34 59.8   4.432   3.946    54   17.2   4:09 (240,-19)  

* C/2014 W6 ( Catalina )

Now it is 18.0 mag (Jan. 23, K. Hills). It keeps observable at 17 mag from winter to spring. It is observable in excellent condition in the Southern Hemisphere. But it locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  11 32.75  -22 16.4   2.330   3.118   136   17.3   2:00 (180, 77)  
Feb. 21  11 24.67  -24  7.0   2.280   3.113   141   17.2   1:24 (180, 79)  

* C/2012 K8 ( Lemmon )

It keeps observable at 17-18 mag for a long time from 2013 to 2016. It keeps locating high in the Northern Hemisphere. It keeps locating very low in the Southern Hemipshere. No observations have been reported since 2014 November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  17 26.91   50 52.3   6.578   6.575    85   17.3   4:00 (213,-10)  
Feb. 21  17 26.87   52  9.7   6.546   6.584    87   17.3   4:09 (208, -7)  

* C/2013 U2 ( Holvorcem )

Now it is 17.8 mag (Jan. 6, B. Lutkenhoner). It was observed around 17-18 mag in early 2014. It will be observable around 17-18 mag again from 2014 autumn to 2015 spring, in excellent condition in the Northern Hemisphere. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  10 28.22   57 12.7   4.436   5.185   135   17.4   0:56 (180, -2)  
Feb. 21  10 21.71   56 57.4   4.460   5.194   133   17.4   0:22 (180, -2)  

* (347449) 2012 TW236

First return of a peculiar asteroid 1998 HO121. It keeps observable at 17-18 mag from 2015 to 2016.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   6 53.04    8 22.5   2.375   3.168   136   17.4  21:16 (180, 47)  
Feb. 21   6 52.26    8 56.5   2.423   3.152   130   17.5  20:48 (180, 46)  

* 108P/Ciffreo

It brightened up to 13.3 mag in November (Nov. 19, Taras Prystavski). Now it is fading rapidly. It has already faded down to 16.2 mag (Jan. 25, J. L. Martin). It keeps 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. 14   5 23.52   39  3.2   1.395   2.040   116   17.5  20:27 (172, 15)  
Feb. 21   5 32.81   38 49.4   1.493   2.075   111   17.8  20:17 (171, 15)  

* 299P/2014 D2 ( Catalina-PanSTARRS )

Now it is 17.6 mag (Jan. 22, A. Maury, J.-F. Soulier, J.-G. Bosch, T. Noel). It keeps observable at 17 mag from spring to summer. It locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  16 35.74  -28 18.2   3.276   3.140    73   17.5   4:00 (273, 51)  
Feb. 21  16 44.00  -28 32.3   3.182   3.140    78   17.5   4:09 (270, 57)  

* 119P/Parker-Hartley

Now it is 17.2 mag (Jan. 10, Toshiyuki Takahashi). It was observed at 17 mag from 2013 to early 2014. It will be observable at 17.5 mag in good condition again from autumn to winter in 2014.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   8  4.16   13 54.7   2.518   3.437   154   17.5  22:27 (180, 41)  
Feb. 21   8  0.84   14  8.7   2.581   3.452   147   17.6  21:56 (180, 41)  

* 65P/Gunn

Now it is 17.6 mag (Jan. 21, Catalina Sky Survey). Now it is around the aphelion. In the Northern Hemisphere, it is observable at 18 mag in good condition from winter to spring. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   8 47.30   28 58.5   3.659   4.594   158   17.6  23:10 (180, 26)  
Feb. 21   8 42.79   29 11.1   3.690   4.585   151   17.6  22:38 (180, 26)  

* C/2014 W9 ( PanSTARRS )

Now it is 16.2 mag (Jan. 20, Taras Prystavski). It is observable at 17 mag until spring. It locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  14 58.38  -13 14.5   1.109   1.593    98   17.7   4:00 (226, 61)  
Feb. 21  15 13.82  -15 28.8   1.068   1.595   101   17.7   4:09 (220, 66)  

* C/2013 C2 ( Tenagra )

Now it is 18.8 mag (Dec. 20, K. Hills). It keeps 18 mag for a very long time from 2013 to 2018. It locates high in the Southern Hemisphere. But it locates somewhat low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  12 21.28  -23 50.8   8.529   9.161   127   17.8   2:48 (180, 79)  
Feb. 21  12 20.05  -23 51.8   8.447   9.159   133   17.8   2:19 (180, 79)  

* C/2013 TW5 ( Spacewatch )

Now it is 17.0 mag (Dec. 30, Space Surveillance Telescope, Atom Site). It keeps 18 mag from 2014 to 2015. In 2015, it keeps observable in good condition from winter to spring.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  10 49.21  -10 31.1   5.079   5.968   151   17.8   1:16 (180, 66)  
Feb. 21  10 46.13  -10 43.4   5.055   5.978   157   17.8   0:45 (180, 66)  

* P/2014 X1 ( Elenin )

Now it is 16.3 mag (Jan. 27, F. Limon). It will be fading after this, and will be fainter than 18 mag in late February.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   5 12.27   55  7.4   1.237   1.858   112   17.8  20:27 (173, -1)  
Feb. 21   5 26.20   55 13.1   1.305   1.876   108   18.0  20:17 (172, -1)  

* C/2014 F2 ( Tenagra )

It was observed at 18 mag from spring to summer in 2014. In the Northern Hemisphere, it will be observable at 18 mag in good conditionn from winter to spring in 2015 again. It is not observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14  15 35.60   57  1.7   4.001   4.328   102   17.9   4:00 (196, -5)  
Feb. 21  15 30.57   59 44.4   3.971   4.333   104   17.9   4:09 (190, -6)  

* C/2014 Y1 ( PanSTARRS )

It will brighten up to 14 mag in 2016 spring. Now it is 17.1 mag (Jan. 22, Mt. Lemmon Survey). In 2015, it is observable in good condition until spring in the Northern Hemisphere. In the Southern Hemisphere, it is not observable in 2015. But it will be observable in good condition at the high light in 2016.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Feb. 14   7 24.59   40 34.8   3.465   4.254   138   18.0  21:48 (180, 14)  
Feb. 21   7 20.82   40 20.7   3.476   4.198   131   17.9  21:17 (180, 15)  

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