Weekly Information about Bright Comets (2025 Sept. 13: South)

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Updated on September 17, 2025
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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/2025 R2 ( SWAN )

Bright new comet. Now it is 6.2 mag (Sept. 16, Mike Olason). It will turn to fade out rapidly after the peak. In the Northern Hemisphere, it is not observable now, but it will appear in October. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  13 10.79   -9 33.7   0.918   0.504    29    6.8  19:13 ( 86, 12)  
Sept.20  13 42.47  -12  3.2   0.740   0.534    31    6.6  19:19 ( 84, 13)  

* C/2025 A6 ( Lemmon )

It brightened very rapidly. It is expected to brighten up to 4 mag from October to November. Now it is 8.5 mag (Sept. 16, Virgilio Gonano). It brightens up to 4 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in November. In the Southern Hemisphere, it is not observable now, but it will appear in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 23.41   34 11.0   1.651   1.294    51    9.2   4:38 (228, -2)  
Sept.20   8 43.92   36  2.0   1.417   1.179    55    8.5   4:28 (227, -3)  

* C/2025 K1 ( ATLAS )

It is expected to brighten up to 7.5 mag in October. Now it is 11.4 mag (Sept. 6, Virgilio Gonano). It brightens up to 7.5 mag, but it will turn to fade out rapidly after that. It will be unobservable soon in the Northern Hemisphere, or in October in the Southern Hemisphere. But it will be observable again in October in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  14 11.58  -10 48.0   1.004   0.758    44   10.5  19:13 ( 93, 24)  
Sept.20  13 47.25  -13  2.4   1.128   0.611    32    9.8  19:19 ( 83, 14)  

* 414P/STEREO

It brightened very rapidly. Now it is 14.7 mag (Sept. 1, Masayoshi Yoshimi). It brightens up to 12.5 mag, but it will turn to fade out rapidly after that. It will be fainter than 18 mag in November. In the Northern Hemisphere, it will be unobservable in October. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   9 19.38   18 27.5   1.044   0.595    33   13.4   4:38 (248, -1)  
Sept.20  10  0.12   10 24.2   1.134   0.541    28   12.4   4:28 (258, -1)  

* C/2024 E1 ( Wierzchos )

It is expected to brighten up to 5 mag in January. Now it is 13.5 mag (Sept. 14, Juan Jose Gonzalez). It will brighten rapidly after this. It will be unobservable in October in the Southern Hemisphere, or in December in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  15 58.90   31 26.6   2.532   2.382    69   12.8  19:13 (145, 13)  
Sept.20  16  2.89   28 13.3   2.497   2.285    66   12.6  19:19 (138, 12)  

* 3I/2025 N1 ( ATLAS )

Third interstellar object in history following 1I/'Oumuamua and 2I/Borisov. The eccentricity is extremely big as 6. It approaches to Sun down to 1.38 a.u. in late October. It is not observable around the perihelion passage. But it is expected to be observable at 12 mag before and after that time. Now it is 13.9 mag (Sept. 10, Taras Prystavski). Brightening gradually. It will be unobservable in October. But it will be observable again in November.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  15  2.13  -13  4.0   2.546   2.166    56   13.4  19:13 ( 99, 36)  
Sept.20  14 47.34  -12 13.9   2.531   1.976    46   13.0  19:19 ( 93, 25)  

* 240P/NEAT

Now it is brighter than originally expected. Now it is 13.4 mag (Sept. 7, Ken-ichi Kadota). Brightening slowly. It stays observable in good condition. It is expected to brighten up to 12 mag and to be observable in good condition from autumn to winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   4  5.60   -1  2.8   1.711   2.256   109   13.2   4:38 (180, 56)  
Sept.20   4 10.27   -0 46.0   1.625   2.239   114   13.1   4:15 (180, 56)  

* C/2022 N2 ( PanSTARRS )

Now it is 13.5 mag (Sept. 1, Osamu Miyazaki). It stays 14 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   3 33.04   25 38.4   3.340   3.844   112   13.5   4:06 (180, 29)  
Sept.20   3 34.97   25 55.9   3.261   3.851   119   13.4   3:40 (180, 29)  

* C/2023 R1 ( PanSTARRS )

It is expected to brighten up to 13 mag in early summer in 2026. Now it is 14.8 mag (Sept. 11, G. Nobre). It stays 14 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 54.17   16  8.8   3.396   4.051   124   14.2  20:23 (180, 39)  
Sept.20  19 44.78   14 21.7   3.456   4.022   117   14.2  19:47 (180, 41)  

* C/2021 G2 ( ATLAS )

Now it is 14.6 mag (Sept. 7, Ken-ichi Kadota). It stays 15 mag for a while. It will be unobservable in October in the Southern Hemisphere, or in November in the Northern Hemisphere. But it will be observable again in December in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  15 26.15   -0 49.6   6.143   5.719    60   14.3  19:13 (116, 33)  
Sept.20  15 30.46   -0 54.9   6.254   5.745    55   14.3  19:19 (110, 28)  

* 29P/Schwassmann-Wachmann 1

Now it is not observable. It will appear in October.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  10 45.78    3 46.5   7.285   6.294     9   14.3   4:38 (273,-10)  
Sept.20  10 50.46    3 13.5   7.261   6.295    14   14.3   4:28 (271, -7)  

* 210P/Christensen

It is expected to brighten up to 8 mag from late autumn to early winter. Now it is 17.4 mag (Sept. 1, Andrew Pearce). Brightening rapidly. It will be unobservable in October in the Northern Hemisphere, or in November in the Southern Hemisphere. But it will be observable again in November in the Northern Hemisphere, or in December in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 25.21  -41  5.1   0.623   1.391   115   15.1  19:54 (  0, 84)  
Sept.20  19  1.82  -41 43.3   0.604   1.294   104   14.6  19:19 ( 23, 83)  

* C/2022 QE78 ( ATLAS )

Now it is 14.6 mag (May 10, Alfons Diepvens). It stays 15 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 40.49   18 44.4   6.176   5.476    42   14.8   4:38 (242,  6)  
Sept.20   8 46.31   18 47.8   6.097   5.476    48   14.8   4:28 (241,  8)  

* C/2022 E2 ( ATLAS )

It was observed at 12-13 mag for a long time in 2024. Now it is 14.8 mag (Aug. 31, Thomas Lehmann). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will be observable soon.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   0  2.98   55 58.7   4.278   4.854   119   15.0   0:37 (180, -1)  
Sept.20  23 47.79   55  2.8   4.263   4.892   123   15.0  23:48 (180,  0)  

* C/2024 J3 ( ATLAS )

It will brighten up to 13 mag in 2026. Now it is 14.7 mag (Aug. 28, Andrew Pearce). It stays 15 mag for a while. It will be getting lower gradually after this, and it will be unobservable in January in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  18 32.62  -12 23.0   4.968   5.360   107   15.0  19:13 (174, 67)  
Sept.20  18 31.50  -11 56.9   5.042   5.321   100   15.0  19:19 (154, 65)  

* C/2014 UN271 ( Bernardinelli-Bernstein )

Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.0 mag (Aug. 31, Andrew Pearce). It stays 15 mag for a while. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition. In the Northern Hemisphere, it is not observable until 2030.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   5 38.89  -70 21.1  14.672  14.748    92   15.0   4:38 (348, 53)  
Sept.20   5 40.80  -70 51.3  14.660  14.726    91   15.0   4:28 (350, 53)  

* 43P/Wolf-Harrington

Now it is 16.5 mag (Apr. 7, Alfons Diepvens). It stays 15 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 57.75   11  0.8   3.191   2.460    36   15.1   4:38 (251,  7)  
Sept.20   9 10.13    9 50.2   3.145   2.467    40   15.0   4:28 (251,  9)  

* 217P/LINEAR

It brightened up to 12.1 mag in early summer (June 10, Taras Prystavski). Now it is 14.8 mag (Aug. 23, Hiroshi Abe). Fading gradually. It will be fainter than 18 mag in January. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere. But it will become high in autumn.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   7 54.45   14 51.6   2.246   1.820    52   15.7   4:38 (238, 16)  
Sept.20   8  7.60   14 28.1   2.240   1.877    56   15.9   4:28 (237, 17)  

* C/2023 C2 ( ATLAS )

It brightened up to 12.7 mag in 2024 summer (Aug. 7, 2024, Thomas Lehmann). Now it is 15.5 mag (Sept. 1, Yoshiaki Yamaguchi). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  22 50.92   58 37.6   3.394   3.955   117   15.7  23:19 (180, -4)  
Sept.20  22 42.65   58 32.4   3.427   4.009   118   15.8  22:44 (180, -4)  

* 65P/Gunn

Now it is 15.7 mag (Aug. 25, Thomas Lehmann). Fading slowly. It will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  18 24.70  -31 52.6   2.535   2.959   105   15.7  19:13 (129, 85)  
Sept.20  18 29.94  -31 41.2   2.630   2.965    99   15.8  19:19 (106, 80)  

* C/2024 T5 ( ATLAS )

Now it is 15.6 mag (Sept. 7, ATLAS-MLO, Mauna Loa). It stays 15 mag for a while. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition. It is expected to brighten up to 12 mag in winter between 2026 and 2027.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   3 24.14  -43 14.1   5.822   6.301   114   15.8   3:56 (  0, 82)  
Sept.20   3 23.29  -43 52.1   5.749   6.259   116   15.8   3:28 (  0, 81)  

* 47P/Ashbrook-Jackson

Now it is 15.5 mag (Sept. 3, Michael Jager). Fading slowly. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  22 57.24  -11 31.0   1.823   2.820   169   15.8  23:26 (180, 66)  
Sept.20  22 51.97  -11 23.1   1.841   2.816   162   15.8  22:54 (180, 66)  

* 88P/Howell

Now it is 17.7 mag (July 24, Thomas Lehmann). It will brighten rapidly after this. Now it is not observable. It will appear in January in the Southern Hemisphere, or in December in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  12 31.11   -1  6.9   3.229   2.290    17   16.1  19:13 ( 87, -1)  
Sept.20  12 43.20   -2 31.2   3.204   2.244    14   15.9  19:19 ( 83, -5)  

* C/2025 L1 ( ATLAS )

It is expected to brighten up to 13.5 mag and to be observable in good condition in 2026 spring. Now it is 16.8 mag (Aug. 12, ATLAS South Africa). Brightening slowly. In the Northern Hemisphere, it is not observable now, but it will appear in January. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  11 38.99  -68 41.1   2.387   2.297    72   16.0  19:13 ( 23, 27)  
Sept.20  12 16.43  -66 23.5   2.417   2.240    67   15.9  19:19 ( 26, 26)  

* 60P/Tsuchinshan 2

The condition is bad. It is hardly observable in this apparition. Fading gradually. It will be fainter than 18 mag in December. Now it is not observable. It will appear in October in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  10 44.27    5 44.1   2.711   1.728     9   15.9   4:38 (271,-11)  
Sept.20  11  1.73    3 51.9   2.720   1.750    12   16.0   4:28 (272,-10)  

* 78P/Gehrels 2

It will brighten up to 12 mag in 2026 summer. Now it is 16.3 mag (Sept. 1, Ken-ichi Kadota). Brightening slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 51.15  -12 45.5   2.219   2.934   126   16.4  20:21 (180, 68)  
Sept.20  19 50.71  -13  5.4   2.267   2.902   119   16.3  19:53 (180, 68)  

* C/2024 A1 ( ATLAS )

Now it is 16.7 mag (Sept. 1, Ken-ichi Kadota). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in January.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 27.21   27 50.7   4.554   3.956    48   16.5   4:38 (234,  2)  
Sept.20   8 32.45   28 51.6   4.471   3.969    54   16.4   4:28 (231,  3)  

* 302P/Lemmon-PanSTARRS

It brightened very rapidly, and it became brighter than expected. Now it is 16.0 mag (Sept. 1, Andrew Pearce). Fading slowly. It will be fainter than 18 mag in January. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   0 46.76   -3  4.7   2.435   3.395   159   16.4   1:20 (180, 58)  
Sept.20   0 43.04   -3 38.4   2.419   3.402   166   16.5   0:49 (180, 58)  

* C/2022 R6 ( PanSTARRS )

Now it is 16.2 mag (May 13, ATLAS South Africa). It stays 16 mag for a while. It will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 31.95  -10 27.8   7.238   6.567    45   16.5   4:38 (265, 25)  
Sept.20   8 36.14  -10 37.6   7.178   6.568    49   16.5   4:28 (263, 28)  

* C/2023 H5 ( Lemmon )

Now it is 16.0 mag (Sept. 12, Alfons Diepvens). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  12 58.68   63  4.4   4.743   4.357    61   16.5  19:13 (149,-29)  
Sept.20  13 15.14   63  6.3   4.712   4.365    63   16.5  19:19 (148,-31)  

* 261P/Larson

Now it is 17.4 mag (Aug. 26, Ken-ichi Kadota). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 43.52  -17 12.0   1.439   2.174   124   16.8  20:14 (180, 72)  
Sept.20  19 46.18  -16 54.6   1.488   2.155   118   16.7  19:49 (180, 72)  

* 48P/Johnson

Now it is 16.2 mag (Aug. 30, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag in November. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   4  0.18    5 15.4   1.949   2.485   110   16.8   4:33 (180, 50)  
Sept.20   4  2.13    4 55.6   1.900   2.513   116   16.9   4:07 (180, 50)  

* C/2024 J2 ( Wierzchos )

It brightened rapidly up to 14.6 mag in winter (Jan. 31, Thomas Lehmann). Now it is 16.8 mag (Sept. 4, ATLAS-HKO, Haleakala). Fading gradually. It will be fainter than 18 mag in November. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   3 20.44  -32 26.8   2.193   2.809   117   16.8   3:53 (180, 87)  
Sept.20   3 17.61  -35 59.5   2.225   2.869   120   17.0   3:23 (  0, 89)  

* C/2020 V2 ( ZTF )

It was observed at 9-10 mag for a long time in 2023. It is fading very slowly. Now it is 16.4 mag (Aug. 29, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19  8.17  -72 27.5   8.025   8.283   101   16.8  19:40 (  0, 53)  
Sept.20  19  2.05  -71 49.6   8.155   8.334    96   16.9  19:19 (  2, 53)  

* C/2019 E3 ( ATLAS )

Very far object. Now it is 16.6 mag (July 17, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in November. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   1  0.88  -57 39.6  10.328  10.908   122   16.9   1:34 (  0, 67)  
Sept.20   0 55.49  -57 44.6  10.356  10.920   121   17.0   1:01 (  0, 67)  

* C/2023 H1 ( PanSTARRS )

Now it is 16.9 mag (Aug. 29, ATLAS South Africa). Fading slowly. It will be fainter than 18 mag in December. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 45.42  -15 34.4   4.369   5.016   125   17.0  20:16 (180, 70)  
Sept.20  19 45.67  -15 20.8   4.485   5.042   118   17.0  19:48 (180, 70)  

* C/2024 G6 ( ATLAS )

Now it is 17.1 mag (Aug. 21, Yasukazu Ikari). It stays 17 mag for a while. It will be unobservable in November. But it will be observable again in January in the Southern Hemisphere, or in December in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  15 48.95  -11 46.5   6.835   6.522    67   17.0  19:13 (110, 44)  
Sept.20  15 49.84  -11 28.6   6.938   6.514    61   17.0  19:19 (104, 38)  

* C/2023 A3 ( Tsuchinshan-ATLAS )

It brightened up to -3 mag due to the forward scattering in the SOHO coronagraph images (Oct. 9, 2024, Q.-c. Zhang, Charles S. Morris). It became a great comet of 0 mag on the ground. Now it is 17.0 mag (Sept. 7, Ken-ichi Kadota). Fading gradually. It will be fainter than 18 mag in October. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  17 54.78   19 14.3   4.900   5.105    96   17.1  19:13 (166, 35)  
Sept.20  17 54.07   18 14.7   5.064   5.177    90   17.2  19:19 (156, 33)  

* C/2023 X2 ( Lemmon )

Now it is 17.4 mag (Aug. 19, Ken-ichi Kadota). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   7 16.73   71 24.0   5.275   5.153    77   17.2   4:38 (195,-22)  
Sept.20   7 31.74   72 49.0   5.197   5.145    81   17.1   4:28 (194,-23)  

* C/2024 R4 ( PanSTARRS )

Brightening rapidly. It is expected to brighten up to 13 mag from 2027 to 2028. Now it is 16.8 mag (Sept. 1, Ken-ichi Kadota). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting lower gradually after this, and it will be unobservable in December.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  21 58.15   24  3.0   6.587   7.435   145   17.2  22:27 (180, 31)  
Sept.20  21 53.31   23 53.1   6.574   7.395   142   17.1  21:55 (180, 31)  

* C/2023 T3 ( Fuls )

Now it is 17.0 mag (Aug. 7, ATLAS Chile). It stays 18 mag for a while. It will be unobservable in October in the Northern Hemisphere, or in November in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  14 33.05  -20 49.9   4.643   4.110    52   17.2  19:13 ( 87, 34)  
Sept.20  14 41.33  -20 55.7   4.751   4.141    47   17.3  19:19 ( 84, 29)  

* C/2023 U1 ( Fuls )

It continues brightening even after the perihelion passage. Now it is 17.1 mag (Sept. 3, ATLAS South Africa). It stays 18 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   2 24.72  -66 41.8   5.168   5.591   109   17.2   2:57 (  0, 58)  
Sept.20   2  7.18  -67 40.9   5.201   5.615   109   17.2   2:13 (  0, 57)  

* 493P/2024 Q2 ( LONEOS )

Now it is 17.5 mag (Sept. 6, ATLAS-MLO, Mauna Loa). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   5  1.22   45 17.7   3.742   3.894    91   17.3   4:38 (190,  9)  
Sept.20   5  6.22   46 12.4   3.643   3.886    96   17.2   4:28 (188,  8)  

* 195P/Hill

Now it is 17.2 mag (Mar. 6, ATLAS South Africa). It stays 17 mag for a while. In the Northern Hemisphere, it will be unobservable soon. But it will be observable again in September. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   9  0.84  -13 57.3   5.172   4.444    39   17.3   4:38 (273, 21)  
Sept.20   9  7.52  -14 58.1   5.127   4.445    43   17.3   4:28 (272, 24)  

* C/2019 U5 ( PanSTARRS )

Now it is 17.1 mag (Sept. 2, Andrew Pearce). It stays 18 mag for a while. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   6  1.06  -41 37.9   8.170   8.156    85   17.3   4:38 (295, 67)  
Sept.20   5 59.82  -42 23.1   8.160   8.200    88   17.3   4:28 (299, 70)  

* 145P/Shoemaker-Levy 5

Now it is 17.3 mag (Sept. 2, Francois Kugel). It stays 17 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  22 33.90  -24 43.5   1.313   2.270   155   17.4  23:03 (180, 80)  
Sept.20  22 28.10  -24 27.6   1.313   2.238   149   17.3  22:30 (180, 79)  

* C/2017 K2 ( PanSTARRS )

It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 16.9 mag (Sept. 5, Alfons Diepvens). It stays 17 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   6 19.55   27 55.0   9.719   9.523    75   17.3   4:38 (211, 20)  
Sept.20   6 20.04   28  6.7   9.651   9.573    82   17.3   4:28 (208, 21)  

* 24P/Schaumasse

It will brighten up to 8 mag in winter, and will be observable in good condition. Now it is 19.7 mag (Aug. 26, Alan Hale). It will brighten rapidly after this. In the Northern Hemisphere, it stays observable in good condition. It locates somewhat low in the Southern Hemisphere. But it will become high in winter.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   5 43.81   18  1.0   1.688   1.872    84   17.8   4:38 (208, 32)  
Sept.20   6  0.99   18 27.5   1.568   1.813    86   17.4   4:28 (207, 32)  

* 21P/Giacobini-Zinner

It brightened up to 11 mag in the SWAN images in early spring (Jan. 27, Vladimir Bezugly). Fading slowly. It will be fainter than 18 mag in October. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will be getting higher gradually.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 51.99   -6 45.9   3.009   2.320    39   17.4   4:38 (265, 19)  
Sept.20   9  2.18   -7 55.9   3.022   2.381    42   17.6   4:28 (265, 21)  

* 164P/Christensen

Now it is 17.3 mag (Sept. 15, Catalina Sky Survey). Brightening slowly. In the Northern Hemisphere, it will be getting higher gradually. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   8 47.64   22 21.3   2.597   1.968    42   17.6   4:38 (241,  2)  
Sept.20   9  3.44   22  0.4   2.577   2.002    45   17.5   4:28 (241,  3)  

* C/2025 R1 ( ATLAS )

Now it is 17.0 mag (Sept. 9, B. Kumar). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   4 40.12   70 10.5   1.900   2.150    89   17.7   4:38 (183,-15)  
Sept.20   4 22.61   76 22.3   1.800   2.118    93   17.5   4:28 (180,-21)  

* C/2021 S3 ( PanSTARRS )

It brightened up to 9.6 mag from February to March in 2024 (Feb. 25, 2024, Thomas Lehmann). Now it is 17.9 mag (Aug. 23, ATLAS-HKO, Haleakala). Fading slowly. It will be fainter than 18 mag in November. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  23 11.02   43 42.7   5.834   6.554   132   17.5  23:40 (180, 11)  
Sept.20  23  6.72   43  8.1   5.868   6.613   134   17.6  23:08 (180, 12)  

* C/2025 J1 ( Borisov )

Now it is 17.7 mag (Aug. 30, J. Linder). Brightening slowly. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  10 52.88   70 17.7   4.625   4.324    66   17.7   4:38 (204,-37)  
Sept.20  10 58.53   69 56.8   4.543   4.290    69   17.6   4:28 (205,-36)  

* 486P/2024 H1 ( Leonard )

Now it is 17.3 mag (Aug. 31, Michael Jager). Fading gradually. It will be fainter than 18 mag in October. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   0 35.78    6  9.1   1.582   2.549   159   17.6   1:09 (180, 49)  
Sept.20   0 31.27    5 35.4   1.578   2.568   167   17.7   0:37 (180, 49)  

* C/2025 L2 ( MAPS )

Now it is 17.8 mag (Sept. 9, A. Sankovich). It stays 18 mag for a while. In the Northern Hemisphere, it will be unobservable soon. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  20 52.32  -51 48.0   2.339   3.005   122   17.6  21:22 (  0, 73)  
Sept.20  20 42.32  -53 23.9   2.412   2.982   115   17.7  20:45 (  0, 72)  

* C/2024 N3 ( Sarneczky )

Now it is 17.5 mag (Aug. 25, Erik Bryssinck). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  16 29.51   50 45.0   5.259   5.153    78   17.6  19:13 (159, -1)  
Sept.20  16 32.61   48 45.6   5.304   5.165    76   17.7  19:19 (154, -1)  

* C/2024 G4 ( PanSTARRS )

Now it is 17.8 mag (Aug. 23, Alfons Diepvens). It stays 18 mag for a while. It will be getting lower gradually after this, and it will be unobservable in November in the Southern Hemisphere, or in December in the Northern Hemisphere. But it will be observable again in January in the Northern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  16 53.58    8 38.9   5.157   5.115    81   17.7  19:13 (144, 39)  
Sept.20  16 57.46    7 47.4   5.229   5.100    77   17.7  19:19 (136, 36)  

* 105P/Singer Brewster

It faded down to 20.0 mag, fainter than predicted by 3-4 mag, after the perihelion passage (Mar. 12, Taras Prystavski). However, it is brightening very rapidly after that. Now it is 18.7 mag (Aug. 29, ATLAS South Africa). Fading slowly. It will be fainter than 18 mag in November. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 55.07   -9 58.9   1.910   2.651   127   17.7  20:25 (180, 65)  
Sept.20  19 57.17  -10 31.1   2.011   2.679   121   17.7  20:00 (180, 65)  

* C/2020 K1 ( PanSTARRS )

It brightened up to 12.1 mag in 2023 spring (May 20, 2023, Jose Guilherme de S. Aguiar). Now it is 17.4 mag (Mar. 25, ATLAS South Africa). It stays 18 mag for a while. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   6 41.49  -18 14.3   8.220   7.982    72   17.7   4:38 (254, 52)  
Sept.20   6 42.24  -18 31.8   8.183   8.029    77   17.7   4:28 (251, 55)  

* 491P/2024 K2 ( Spacewatch-PanSTARRS )

Now it is 17.8 mag (Aug. 27, ATLAS Chile). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 38.56  -22 53.7   3.430   4.060   122   17.8  20:09 (180, 78)  
Sept.20  19 38.95  -22 40.4   3.534   4.072   115   17.9  19:42 (180, 78)  

* C/2023 V1 ( Lemmon )

Now it is 17.7 mag (Aug. 10, Alfons Diepvens). It stays 18 mag for a while. In the Northern Hemisphere, it will be getting lower gradually. In the Southern Hemisphere, it will never be observable after this.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  15 21.94   44  6.5   5.444   5.114    65   17.9  19:13 (146, -1)  
Sept.20  15 22.44   42 32.7   5.496   5.120    63   17.9  19:19 (141, -4)  

* 188P/LINEAR-Mueller

Now it is 18.4 mag (Sept. 1, Ken-ichi Kadota). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  21 42.27  -21 35.0   2.008   2.921   149   17.9  22:12 (180, 76)  
Sept.20  21 38.45  -21 20.4   2.038   2.900   142   17.9  21:41 (180, 76)  

* C/2023 RS61 ( PanSTARRS )

Although it is around 20 mag usually, now it is bright in outburst. Now it is 17.2 mag (Sept. 15, ATLAS-MLO, Mauna Loa). It stays 18 mag for a while. In the Northern Hemisphere, it stays observable in good condition. It stays extremely low in the Southern Hemisphere.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   3 15.33   37 41.6   8.499   8.928   112   17.9   3:48 (180, 17)  
Sept.20   3 14.57   37 55.9   8.394   8.918   118   17.9   3:20 (180, 17)  

* 351P/Wiegert-PanSTARRS

Now it is brighter than expected. Now it is 17.4 mag (Aug. 31, ATLAS South Africa). Fading slowly. It will be fainter than 18 mag soon. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13  19 39.04  -14 19.4   2.588   3.256   123   17.9  20:09 (180, 69)  
Sept.20  19 40.12  -14 11.3   2.682   3.266   117   18.0  19:43 (180, 69)  

* 242P/Spahr

Now it is 17.8 mag (Mar. 17, ATLAS Chile). It stays 18 mag for a while. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   7 33.43   -7  7.3   4.584   4.147    58   17.9   4:38 (252, 35)  
Sept.20   7 39.39   -7 49.5   4.518   4.156    62   17.9   4:28 (251, 38)  

* 276P/Vorobjov

Now it is 17.9 mag (Mar. 6, Erik Bryssinck). It stays 18 mag for a while. It stays observable in good condition.

Date(TT)  R.A. (2000) Decl.   Delta     r    Elong.  m1   Best Time(A, h)  
Sept.13   6 47.35   11 12.3   4.345   4.089    68   18.0   4:38 (227, 30)  
Sept.20   6 52.54   10 41.9   4.258   4.098    74   17.9   4:28 (225, 32)  

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