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

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Updated on November 4, 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/2017 T2 ( PanSTARRS )

Now it is 11.0 mag (Nov. 1, Seiichi Yoshida). It is expected to brighten up to 8 mag in 2020. It stays observable in good condition for a long time in the Northern Hemisphere. In the Southern Hemisphere, it will be getting lower gradually, and it will be unobservable in early December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   5 35.42   35 41.1   2.078   2.848   132   10.9   2:53 (180, 89)  
Nov.  9   5 30.24   38  2.4   1.951   2.782   139   10.7   2:21 (180, 87)  

* C/2018 N2 ( ASASSN )

Now it is 11.5 mag (Nov. 1, Seiichi Yoshida). It stays bright as 11 mag until winter. It stays observable in good condition for a long time in the Northern Hemisphere. In the Southern Hemisphere, it locates low, and it will be unobservable in early December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   0 40.96   38 10.7   2.248   3.126   146   11.2  21:54 (180, 87)  
Nov.  9   0 25.60   38 41.3   2.294   3.125   140   11.3  21:12 (180, 86)  

* C/2018 W2 ( Africano )

It brightened up to 8.3 mag in September (Sept. 20, Maik Meyer). Now it is fading. But it is still bright as 11.1 mag (Nov. 2, Chris Wyatt). In the Southern Hemisphere, it stays observable for a long time after this. In the Northern Hemisphere, it will be unobservable in early December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  21 41.15  -38 38.0   1.253   1.664    94   11.3  18:56 (  0, 16)  
Nov.  9  21 36.22  -40 46.2   1.452   1.712    86   11.7  18:25 (  0, 14)  

* 260P/McNaught

Now it is 12.1 mag (Nov. 1, Seiichi Yoshida). It will fade out rapidly after this. It is observable in excellent condition in the Northern Hemisphere. It stays locating extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   2 37.81   49 41.2   0.614   1.535   144   12.2  23:52 (180, 75)  
Nov.  9   2 31.98   50 10.4   0.643   1.566   146   12.5  23:18 (180, 75)  

* 29P/Schwassmann-Wachmann 1

Now it is 14.3 mag (Nov. 2, Chris Wyatt).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   0 31.17   14 19.7   4.882   5.778   152   13.2  21:45 (  0, 69)  
Nov.  9   0 28.94   14  0.5   4.940   5.778   144   13.2  21:16 (  0, 69)  

* 68P/Klemola

Now it is 13.9 mag (Oct. 26, 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)  
Nov.  2  19 34.17  -15 58.6   1.799   1.795    73   13.8  18:31 ( 29, 34)  
Nov.  9  19 52.09  -15 60.0   1.852   1.794    71   13.9  18:25 ( 31, 33)  

* C/2018 A6 ( Gibbs )

Now it is 14.2 mag (Nov. 2, Chris Wyatt). It stays 13-14 mag for a long time in 2019. In the Southern Hemisphere, it is observable in good 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)  
Nov.  2  19  3.22  -83 26.2   3.312   3.172    73   14.3  18:31 (  4,-29)  
Nov.  9  19 58.85  -80 38.3   3.367   3.191    71   14.4  18:25 (  4,-26)  

* 168P/Hergenrother

It has not been observed yet in this apparition. Now it is fainter than 21.5 mag (Aug. 4, Erwin Schwab). It was expected to brighten up to 12 mag from August to September. But actually, it must be much fainter than expected. It is observable in good 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)  
Nov.  2   7 31.21   56 27.1   1.070   1.686   109   14.5   4:49 (180, 69)  
Nov.  9   7 36.87   57 57.0   1.069   1.731   114   15.1   4:27 (180, 67)  

* 78P/Gehrels 2

Now it is 16.3 mag (Nov. 2, Toshihiko Ikemura, Hirohisa Sato). It is fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   9 18.52    9  6.1   2.593   2.608    79   14.6   4:55 (313, 55)  
Nov.  9   9 24.71    8 21.2   2.531   2.640    85   14.7   5:01 (324, 58)  

* 160P/LINEAR

Now it is 14.8 mag (Oct. 30, Toshihiko Ikemura, Hirohisa Sato). It stays at 15 mag until December. 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)  
Nov.  2  20  1.84  -21 16.0   1.711   1.810    79   14.7  18:31 ( 20, 31)  
Nov.  9  20 16.45  -19 30.7   1.764   1.801    75   14.7  18:25 ( 23, 32)  

* C/2016 M1 ( PanSTARRS )

It brightened up to 7.7 mag in June in 2018 (June 19, Juan Jose Gonzalez). Now it is fading. It has already faded down to 14.2 mag (Sept. 10, Thomas Lehmann). In the Southern Hemisphere, it stays observable for a long time until the comet will fade out. In the Northern Hemisphere, it is appearing in the morning sky, but it stays low for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   6 55.05  -33 50.2   4.875   5.140    99   14.7   4:12 (  0, 21)  
Nov.  9   6 50.72  -34 11.6   4.864   5.197   104   14.8   3:40 (  0, 21)  

* C/2017 B3 ( LINEAR )

Now it is 14.6 mag (Oct. 18, Chris Wyatt). In the Southern Hemisphere, it is observable for a long time. It stays low in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  22 54.05  -36 55.8   4.154   4.565   108   15.0  20:09 (  0, 18)  
Nov.  9  22 52.45  -35 30.7   4.275   4.595   102   15.1  19:40 (  0, 20)  

* 114P/Wiseman-Skiff

Now it is 15.8 mag (Oct. 31, Toshihiko Ikemura, Hirohisa Sato). It will brighten very rapidly, and it will brighten up to 14 mag in winter. 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)  
Nov.  2   2 18.05   46 18.9   0.818   1.741   148   15.4  23:32 (180, 79)  
Nov.  9   2 15.02   45  6.4   0.781   1.714   150   15.1  23:02 (180, 80)  

* 2I/2019 Q4 ( Borisov )

Now it is 15.8 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato). The orbit is extremely hyperbolic with e=3.35. It is the first interstellar comet in history. It brightens up to 15 mag in December. In the Northern Hemisphere, it stays observable in good condition until early December. Then it will be getting lower, and it will be unobservable in mid January. In the Southern Hemisphere, it will be getting higher gradually. Then it will be observable in excellent condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  10 24.85    7 15.5   2.412   2.164    63   15.8   4:55 (296, 43)  
Nov.  9  10 37.32    2 55.0   2.304   2.111    66   15.6   5:01 (305, 43)  

* 155P/Shoemaker 3

Now it is 15.4 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato). It brightens rapidly, and it will be observable at 15 mag in good condition in winter. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   9 21.50   16 25.2   1.667   1.808    81   15.9   4:55 (302, 60)  
Nov.  9   9 37.90   15 37.8   1.607   1.803    84   15.7   5:01 (310, 63)  

* 101P/Chernykh

Now it is 15.3 mag (Oct. 25, Toshihiko Ikemura, Hirohisa Sato). It stays 15.5 mag until December, and it is observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  23 42.78   -9 41.0   1.639   2.425   132   15.7  20:57 (  0, 45)  
Nov.  9  23 43.82   -9 22.7   1.689   2.410   126   15.7  20:31 (  0, 46)  

* C/2018 F4 ( PanSTARRS )

Now it is 15.0 mag (July 21, Taras Prystavski). It stays 16 mag for a long time from 2019 to 2020. It stays observable for a long time 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)  
Nov.  2  12 32.79  -71 38.7   3.847   3.453    59   15.8   4:55 (340,-28)  
Nov.  9  12 46.63  -74  1.4   3.833   3.448    60   15.8   5:01 (343,-28)  

* C/2018 DO4 ( Lemmon )

Now it is 16.0 mag (Sept. 8, Roberto Haver). It is observable at 16 mag in good condition from October to November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   3 48.07    7 49.7   1.582   2.534   158   16.0   1:07 (  0, 63)  
Nov.  9   3 18.58    4 41.5   1.583   2.557   166   16.1   0:11 (  0, 60)  

* C/2019 K7 ( Smith )

Now it is 15.8 mag (Oct. 5, Toshihiko Ikemura, Hirohisa Sato). It stays 15-16 mag for a long time until 2021.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  20  1.42  -24 56.3   4.940   4.839    78   16.3  18:31 ( 19, 28)  
Nov.  9  20  1.24  -24  0.0   5.040   4.818    71   16.3  18:25 ( 25, 27)  

* A/2017 U7

It looks cometary on the LCO (CTIO) image on Aug. 21. Now it is 16.2 mag (Oct. 2, ATLAS-MLO, Mauna Loa). It is observable in excellent condition in the Southern Hemisphere. In the Northern Hemisphere, it locates extremely low for a while.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  19 46.69  -38 17.7   6.640   6.427    73   16.4  18:31 ( 18, 14)  
Nov.  9  19 45.76  -37 42.3   6.760   6.430    66   16.4  18:25 ( 22, 13)  

* C/2017 K2 ( PanSTARRS )

Now it is 16.2 mag (Oct. 4, 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 unobservable 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)  
Nov.  2  17 18.85   47 54.9  10.776  10.533    73   16.4  18:31 (125, 45)  
Nov.  9  17 21.88   47 23.9  10.748  10.486    72   16.4  18:25 (125, 42)  

* 261P/Larson

Now it is 17.1 mag (Oct. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and it will be fainter than 18 mag in late December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   3 35.75   28 47.1   1.317   2.269   158   16.4   0:54 (  0, 84)  
Nov.  9   3 29.81   28 19.2   1.320   2.293   165   16.5   0:21 (  0, 83)  

* C/2019 K5 ( Young )

Now it is 16.4 mag (Oct. 30, Toshihiko Ikemura, Hirohisa Sato). It stays observable in good condition while the comet will be fading slowly after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   3 25.85   -0 21.3   1.606   2.558   159   16.5   0:44 (  0, 55)  
Nov.  9   3 22.19   -1  3.6   1.649   2.606   161   16.7   0:13 (  0, 54)  

* C/2019 N1 ( ATLAS )

Now it is 16.7 mag (Oct. 4, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 10.5 mag from 2020 December to 2021 January. In the Northern Hemisphere, it stays observable in good condition while the comet will be brightening gradually, but it is not observable at the high light. In the Southern Hemisphere, it is not observable for a long time, but it will be observable in good condition after the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  16 42.90   66  2.2   4.793   4.800    84   16.7  18:31 (150, 40)  
Nov.  9  16 49.68   64 53.8   4.730   4.737    84   16.6  18:25 (149, 39)  

* (3200) Phaethon

Now it is 16.7 mag (Aug. 9. Grorudalen Optical Observatory). It passed the perihelion on July 2. Then it must have brightened up to 13 mag, but it was not observable around that time. In the Northern Hemisphere, it stays observable in excellent condition until December when it becomes fainter than 18 mag. In the Southern Hemisphere, it stays locating low.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   0 54.06   43 10.8   1.027   1.927   145   16.7  22:07 (180, 82)  
Nov.  9   0 38.32   39 27.3   1.095   1.977   142   16.9  21:24 (180, 86)  

* 246P/NEAT

It will brighten up to 13.5-14 mag from 2020 to 2021. It stays observable in good condition for a long time after this until 2020 summer.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  12  3.10   14 30.1   4.330   3.707    45   16.9   4:55 (271, 28)  
Nov.  9  12 10.91   13 55.6   4.238   3.689    50   16.7   5:01 (276, 32)  

* C/2010 U3 ( Boattini )

It stays 16-17 mag for a long time until 2020. It is observable in good condition in the Northern Hemisphere. It is hardly observable in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  12 53.33   51 57.1   8.870   8.572    69   16.9   4:55 (226, 33)  
Nov.  9  12 58.55   51 47.8   8.818   8.579    72   16.9   5:01 (228, 38)  

* C/2015 O1 ( PanSTARRS )

Fading. Now it is 17.3 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato). It stays 17 mag from autumn to winter. 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)  
Nov.  2   9 19.23   23 52.2   6.425   6.401    84   16.9   4:55 (290, 65)  
Nov.  9   9 17.62   23 46.0   6.343   6.445    91   16.9   5:01 (304, 72)  

* C/2018 A3 ( ATLAS )

Now it is 17.7 mag (Oct. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it stays extremely low for a long time.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   2  4.63   43 44.5   3.359   4.250   150   16.9  23:18 (180, 81)  
Nov.  9   1 50.91   41 49.6   3.394   4.290   151   17.0  22:37 (180, 83)  

* 289P/Blanpain

It brighted rapidly from 20.5 mag up to 18.5 mag in September. It was 18.7 mag on Oct. 22 (Geisei Observatory). However, it was not detected, fainter than 19 mag, in late October. It will approaches to Earth down to 0.09 a.u. in early January. It will be obesrvable in excellent condition in the Northern Hemisphere. If it is as bright as in 2003, it will be 17.5 mag at best. But if it shows cometary activity, it may brighten up to 13.5 mag. In the Southern Hemisphere, it will not be observable at the high light.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  22 24.60  -24 11.8   0.392   1.182   109   17.4  19:39 (  0, 31)  
Nov.  9  22 22.04  -23  3.2   0.368   1.129   102   17.1  19:09 (  0, 32)  

* C/2016 N6 ( PanSTARRS )

Fading now. Now it is 16.1 mag (Sept. 23, iTelescope Observatory, Siding Spring). In the Southern Hemisphere, it stays observable for a long time until it fades out. In the Northern Hemisphere, it will not be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   6 24.32  -49 46.5   5.071   5.289    97   17.2   3:41 (  0,  5)  
Nov.  9   6 16.64  -51 14.7   5.095   5.341    99   17.2   3:06 (  0,  4)  

* 384P/2019 O1 ( Kowalski )

First return of a new periodic comet which brightened up to 18 mag in 2014. Now it is 17.2 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato). It stays 17 mag until November. It is observable in good condition in the Northern Hemisphere. It locates extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   7 37.06   43 31.3   0.343   1.150   108   17.2   4:54 (180, 82)  
Nov.  9   7 54.26   43 44.7   0.359   1.174   112   17.3   4:44 (180, 81)  

* 387P/2019 R1 ( Boattini )

It brightened up to 16 mag in September. Now it is fading. Now it is 17.1 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato). It will be fainter than 18 mag in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   9 56.53    7 50.5   1.456   1.464    70   17.3   4:55 (302, 48)  
Nov.  9  10 10.29    5 43.9   1.451   1.509    73   17.5   5:01 (310, 50)  

* C/2018 U1 ( Lemmon )

Now it is 17.4 mag (Oct. 4, Toshihiko Ikemura, Hirohisa Sato). It will stay at 14 mag for a long time from 2021 to 2022. In the Northern Hemisphere, it stays observable in good condition while brightening gradually, although it becomes low in December and January. In the Southern Hemisphere, it is not observable until March.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  18 24.35   36 26.8   7.546   7.364    75   17.4  18:31 (105, 55)  
Nov.  9  18 26.16   35 27.5   7.569   7.329    72   17.4  18:25 (105, 51)  

* C/2019 L3 ( ATLAS )

Now it is 17.6 mag (Sept. 26, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 12 mag in winter in 2022.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  22  1.77   44 40.7   7.029   7.531   117   17.5  19:16 (180, 80)  
Nov.  9  22  1.38   44  6.7   7.037   7.486   113   17.5  18:49 (180, 81)  

* 173P/Mueller 5

Now it is 17.9 mag (Oct. 8, ATLAS-MLO, Mauna Loa). It is observable at 17-18 mag for a long time from late 2019 to early 2021. It will fade out before it passes the perihelion.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   3 17.93    0 55.5   4.251   5.201   161   17.6   0:36 (  0, 56)  
Nov.  9   3 14.29    0 45.3   4.230   5.187   163   17.5   0:05 (  0, 56)  

* 65P/Gunn

Now it is 18.8 mag (Sept. 27, M. Jaeger, E. Prosperi, S. Prosperi). It is fainter than this ephemeris recently.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   2 30.86    9 47.6   3.218   4.207   175   17.6  23:45 (  0, 65)  
Nov.  9   2 26.10    9 34.2   3.241   4.221   170   17.6  23:12 (  0, 65)  

* C/2019 K4 ( Ye )

Now it is 17.7 mag (Oct. 31, Toshihiko Ikemura, Hirohisa Sato). It will be fainter than 18 mag soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2  23  1.83  -19  5.7   2.116   2.744   119   17.7  20:16 (  0, 36)  
Nov.  9  22 57.81  -21 14.6   2.278   2.788   110   17.9  19:45 (  0, 34)  

* C/2018 Y1 ( Iwamoto )

It approached to Earth down to 0.3 a.u. in mid February, and brightened up to 5.5 mag (Feb. 13, Juan Jose Gonzalez). Now it is fading. It has already faded down to 18.4 mag (Nov. 1, Toshihiko Ikemura, Hirohisa Sato).

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   1 55.20   39  4.0   2.771   3.691   154   17.7  23:08 (180, 86)  
Nov.  9   1 39.53   37 22.2   2.849   3.762   153   17.9  22:25 (180, 88)  

* C/2018 L2 ( ATLAS )

It brightened up to 11 mag in late 2018. Now it is 17.9 mag (Oct. 5, Toshihiko Ikemura, Hirohisa Sato). It will be fainter than 18 mag in November. It is observable in excellent condition in the Northern Hemisphere. It locates extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   3 14.57   45 30.7   3.360   4.230   147   17.8   0:33 (180, 79)  
Nov.  9   3  6.48   44 20.3   3.393   4.294   152   17.9  23:53 (180, 81)  

* 76P/West-Kohoutek-Ikemura

Now it is 17.8 mag (Nov. 2, Toshihiko Ikemura, Hirohisa Sato). It was exptected to brighten up to 16.5 mag from October to December. But actually, it is fainter than originally expected. It seems to brighten up to 18 mag at best. 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)  
Nov.  2   8 35.70   21 31.1   1.209   1.606    93   17.9   4:55 (313, 71)  
Nov.  9   8 52.75   23 38.9   1.156   1.611    96   17.9   5:01 (319, 75)  

* 200P/Larsen

Now it is very faint as 19.7 mag (Oct. 25, Toshihiko Ikemura, Hirohisa Sato). It brightened up to 15.5 mag in 1997, and 17 mag in 2008, however, it is much fainter in this apparition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Nov.  2   1 11.68   16  8.0   2.381   3.339   161   20.1  22:26 (  0, 71)  
Nov.  9   1  8.87   15 21.4   2.423   3.345   154   20.2  21:56 (  0, 70)  

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