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It returned for the first time in 68 years. Now it is 6.7 mag (July 8, Virgilio Gonano). It will fade out rapidly after this. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it is not observable now, but it will appear in August. It is brighter than this ephemeris recently.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 9 0.92 42 9.4 1.918 1.179 31 7.3 18:31 (136, -8)
July 13 9 39.39 41 9.4 1.901 1.192 33 7.4 18:34 (137, -6)
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It returns for the first time in 70 years. It brightened up to 3.7 mag in early April (Apr. 6, Jose Guilherme Aguiar). Now it is 7.8 mag (July 5, Marco Goiato). Fading rapidly. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition. It is brighter than this ephemeris recently.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 8 18.39 -38 10.7 1.691 1.536 63 8.7 18:31 ( 62, 30)
July 13 8 52.00 -40 45.1 1.764 1.629 65 9.1 18:34 ( 59, 31)
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It will approach to Sun down to 0.4 a.u. in late September, and it is expected to brighten up to 2 mag. The brightness evolution slowed down since May. Now it is 9.7 mag (July 8, Virgilio Gonano). It will brighten rapidly after this. It will be unobservable soon in the Northern Hemisphere, or in August in the Southern Hemisphere. But it will be observable again in September in the Southern Hemisphere, or in October in the Northern Hemisphere. At the high light, in the Northern Hemisphere, it will be observable in good condition after the perihelion passage. In the Southern Hemisphere, it will be observable in the low sky before and after the perihelion passage.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 11 11.53 2 32.6 1.996 1.796 63 9.4 18:31 (132, 40)
July 13 11 6.01 2 8.3 2.024 1.682 56 9.2 18:34 (123, 35)
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The condition is bad in this apparition. It brightens up to 10 mag in early summer, however, it is not observable at all. It will fade out rapidly after this. It will be fainter than 18 mag in October. It will never be observable after this.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 8 1.49 25 22.9 2.194 1.232 14 11.4 18:31 (115, -8)
July 13 8 29.47 24 27.8 2.243 1.280 13 11.9 18:34 (114, -8)
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It brightened very rapidly. Now it is 10.8 mag (July 8, Virgilio Gonano). It will fade out rapidly after this. It will be fainter than 18 mag in November. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it is not observable now, but it will appear in August.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 9 15.26 58 46.2 1.799 1.267 43 11.5 18:31 (151,-17)
July 13 10 12.24 56 38.6 1.813 1.321 45 11.8 18:34 (152,-13)
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Now it is 14.1 mag (July 9, Mike Olason). It will fade out rapidly after this. 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)
July 6 4 16.58 32 19.6 2.254 1.574 37 11.6 5:38 (224, 5)
July 13 4 40.45 33 41.6 2.245 1.589 38 11.8 5:36 (223, 4)
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It brightens up to 11 mag in August. It brightens up to 11.5 mag, but it will turn to fade out rapidly after that. Now it is not observable. It will appear in September in the Northern Hemisphere. 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)
July 6 7 18.47 6 31.0 2.054 1.119 16 12.6 18:31 ( 94, -6)
July 13 7 48.26 6 31.2 1.993 1.053 15 12.2 18:34 ( 94, -6)
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Now it is 12.8 mag (May 31, Hiroshi Abe). It stays 12 mag for a while. Now it is not observable. It will appear soon in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 7 9.03 37 13.1 4.695 3.720 14 12.7 18:31 (120,-24)
July 13 7 12.57 37 49.6 4.674 3.710 16 12.7 5:36 (239,-23)
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It brightened up to 9.6 mag from February to March (Feb. 25, Thomas Lehmann). Now it is 12.4 mag (July 8, Osamu Miyazaki). Fading gradually. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now, but it will appear in September.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 20 6.56 62 45.1 2.097 2.387 93 12.9 1:10 (180, -8)
July 13 19 56.89 62 48.5 2.151 2.461 95 13.1 0:33 (180, -8)
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Now it is 13.5 mag (June 11, Thomas Lehmann). It stays 13 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in August. In the Southern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 15 24.40 -68 43.1 2.093 2.789 123 13.1 20:27 ( 0, 56)
July 13 15 27.53 -66 19.9 2.078 2.750 121 13.0 20:02 ( 0, 59)
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First return of a new periodic comet which was discovered in 2011, half a year after the perihelion passage. It brightened very rapidly up to 10.7 mag in spring (Apr. 28, Marco Goiato). Now it is 15.6 mag (June 19, Ken-ichi Kadota). Fading rapidly. It will be fainter than 18 mag in September. 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)
July 6 13 22.15 -29 13.7 0.856 1.491 105 13.5 18:31 (167, 84)
July 13 13 51.11 -29 13.7 0.927 1.542 104 14.0 18:34 (163, 84)
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Now it is 13.8 mag (June 19, Ken-ichi Kadota). It stays 14 mag for a while. It will be unobservable in August in the Northern Hemisphere, or in October in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 12 12.10 -21 38.7 4.944 5.008 87 14.0 18:31 (123, 68)
July 13 12 16.83 -21 2.8 5.040 5.003 82 14.0 18:34 (115, 63)
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It was observed at 9-10 mag for a long time in 2023. Now it is 14.5 mag (June 27, ATLAS Chile). Fading slowly. 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)
July 6 0 34.69 -58 2.1 4.466 4.946 112 14.2 5:38 ( 0, 67)
July 13 0 29.89 -60 0.6 4.469 5.002 116 14.2 5:06 ( 0, 65)
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Now it is 16.0 mag (June 11, Jean-Francois Soulier). In the Northern Hemisphere, it is not observable now, but it will appear in September. In the Southern Hemisphere, it will be unobservable soon. But it will be observable again in September.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 8 47.54 17 43.4 7.117 6.214 25 14.2 18:31 (116, 5)
July 13 8 52.53 17 19.6 7.162 6.216 19 14.2 18:34 (111, 0)
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Now it is 14.4 mag (July 6, Hiroshi Abe). Fading slowly. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 1 42.37 4 2.1 1.874 1.953 78 14.7 5:38 (206, 48)
July 13 1 53.42 4 56.4 1.827 1.975 82 14.7 5:36 (200, 48)
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It will brighten up to 14 mag from summer to autumn. Now it is 15.8 mag (June 8, A. Pearce). It stays 14 mag for a while. 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)
July 6 12 53.41 -17 53.7 1.481 1.869 95 14.8 18:31 (153, 71)
July 13 13 3.49 -18 19.6 1.515 1.838 90 14.7 18:34 (139, 69)
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Now it is 16.7 mag (June 7, Taras Prystavski). It will fade out rapidly after this. 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)
July 6 4 5.00 15 44.9 2.155 1.556 42 14.8 5:38 (234, 19)
July 13 4 22.90 17 46.9 2.153 1.587 43 14.8 5:36 (231, 19)
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It will brighten up to 14.5 mag in summer. Now it is 15.3 mag (July 5, ATLAS-HKO, Haleakala). Fading gradually. 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)
July 6 2 36.67 -7 16.2 1.428 1.463 71 14.9 5:38 (232, 51)
July 13 2 56.59 -4 54.7 1.390 1.445 71 14.8 5:36 (228, 50)
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Now it is 16.0 mag (July 2, ATLAS Chile). It stays 15 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in October. In the Southern Hemisphere, it will be getting lower gradually. But it will be getting higher again after August.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 9 43.74 -22 32.4 3.322 2.950 60 15.0 18:31 ( 88, 40)
July 13 9 43.99 -22 24.5 3.444 2.980 55 15.1 18:34 ( 84, 33)
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Now it is 16.5 mag (June 20, Thomas Lehmann). 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. The brightness evolution is slower than originally expected.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 5 21.98 -50 48.5 2.816 2.765 76 15.0 5:38 (311, 37)
July 13 5 45.76 -53 12.3 2.782 2.763 78 15.0 5:36 (314, 38)
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Now it is 14.7 mag (May 31, Hiroshi Abe). Fading slowly. It will be unobservable soon. 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)
July 6 8 53.34 24 47.8 3.007 2.136 25 15.0 18:31 (122, 2)
July 13 9 10.01 23 38.0 3.054 2.157 23 15.1 18:34 (119, 0)
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It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 14.5 mag (Apr. 27, Hiroshi Abe). It stays 15 mag for a while. Now it is not observable. It will be observable soon.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 6 0.57 15 45.0 7.183 6.211 15 15.2 5:38 (252, -2)
July 13 6 4.28 15 59.5 7.207 6.269 21 15.2 5:36 (249, 2)
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Alan Hale reported its cometary appearance. Now it is 14.7 mag (June 12, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in October. It will be unobservable soon in the Northern Hemisphere, or in September in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 9 41.21 12 33.1 2.315 1.659 39 15.2 18:31 (120, 18)
July 13 10 0.45 10 53.4 2.364 1.678 37 15.4 18:34 (117, 17)
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It is expected to brighten up to 13 mag in 2025 autumn, and it will be observable in good condition. Now it is 15.9 mag (July 1, ATLAS-HKO, Haleakala). It stays 15 mag for a while. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 23 4.25 -4 8.5 4.519 5.084 118 15.3 4:08 (180, 59)
July 13 23 4.47 -3 59.6 4.393 5.046 125 15.2 3:41 (180, 59)
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Now it is 15.9 mag (Mar. 26, ATLAS Chile). It stays 15 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in August. In the Southern Hemisphere, it will be getting higher gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 5 48.24 2 53.8 7.207 6.313 26 15.5 5:38 (261, 8)
July 13 5 53.58 3 4.2 7.149 6.289 29 15.5 5:36 (258, 12)
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It brightened very rapidly in outburst in late May. Now it is 15.3 mag (June 12, Ken-ichi Kadota). Fading slowly. 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)
July 6 15 23.72 -24 9.0 2.420 3.175 130 15.5 20:25 (180, 79)
July 13 15 24.45 -23 43.3 2.498 3.179 123 15.6 19:58 (180, 79)
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It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 16.4 mag (June 30, ATLAS Chile). It stays 16 mag for a while. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be getting lower gradually. But it will be getting higher again after September.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 10 52.20 -46 44.3 8.229 8.234 86 15.5 18:31 ( 56, 58)
July 13 10 56.05 -46 31.0 8.347 8.279 82 15.6 18:34 ( 57, 54)
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It was observed at three apparitions in 2003, 2012 and 2016. It has not been observed yet in this apparition. It will fade out rapidly after this. It will be fainter than 18 mag soon. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be unobservable soon.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 5 24.19 19 46.5 1.384 0.595 22 15.6 5:38 (244, 2)
July 13 6 8.48 19 14.9 1.483 0.620 19 16.2 5:36 (247, -1)
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Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.3 mag (June 19, Thomas Lehmann). It stays 16 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)
July 6 4 1.16 -62 52.7 16.120 16.199 92 15.6 5:38 (328, 48)
July 13 4 4.66 -63 14.3 16.071 16.175 94 15.6 5:36 (330, 50)
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Now it is 14.9 mag (June 5, Thomas Lehmann). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear 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)
July 6 7 35.99 -32 5.2 5.928 5.416 55 15.7 18:31 ( 63, 19)
July 13 7 38.68 -32 19.0 5.990 5.458 54 15.7 18:34 ( 60, 14)
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Now it is 16.3 mag (Mar. 29, Ken-ichi Kadota). It stays 16 mag for a while. Now it is not observable. It will appear in September in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 7 6.66 21 32.5 2.869 1.853 1 15.8 18:31 (105,-16)
July 13 7 26.04 21 15.1 2.857 1.840 1 15.7 5:36 (256,-17)
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It brightened up to 8.9 mag from January to March (Feb. 13, Chris Wyatt). Now it is 15.1 mag (June 5, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in August. It stays extremely low in the Northern Hemisphere. In the Southern Hemisphere, it will be getting lower gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 10 54.77 3 52.1 2.560 2.223 59 16.1 18:31 (129, 37)
July 13 11 7.71 2 39.6 2.676 2.274 56 16.5 18:34 (124, 35)
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It brightened up to 11.1 mag in early 2022 (Mar. 31, 2022, F. Kugel, J.-G. Bosch, J. Nicolas). Now it is 15.4 mag (June 26, Thomas Lehmann). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in October.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 17 20.48 32 59.2 6.745 7.298 119 16.3 22:21 (180, 22)
July 13 17 18.14 32 45.3 6.821 7.339 117 16.3 21:51 (180, 22)
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Now it is 16.8 mag (July 5, ATLAS Chile). It stays 16 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)
July 6 13 43.08 -45 55.0 4.949 5.430 113 16.3 18:44 ( 0, 79)
July 13 13 37.24 -44 53.3 5.038 5.415 106 16.3 18:34 ( 22, 79)
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Now it is 16.6 mag (July 6, ATLAS Chile). 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)
July 6 23 51.12 -18 2.9 1.755 2.341 112 16.5 4:55 (180, 73)
July 13 23 54.87 -18 7.1 1.702 2.358 118 16.4 4:31 (180, 73)
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It brightened up to 12.1 mag in 2023 spring (May 20, 2023, Jose Guilherme de S. Aguiar). Now it is 15.4 mag (May 30, Thomas Lehmann). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear 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)
July 6 6 18.54 -35 59.9 5.437 4.999 59 16.6 5:38 (299, 23)
July 13 6 24.43 -35 43.4 5.484 5.046 59 16.7 5:36 (297, 26)
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Very far object. Now it is 16.7 mag (July 5, ATLAS Chile). It stays 17 mag for a while. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 3 2.59 -64 21.0 10.191 10.388 98 16.7 5:38 (334, 53)
July 13 3 3.22 -64 45.5 10.162 10.393 100 16.7 5:36 (338, 55)
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Now it is 17.0 mag (May 6, ATLAS Chile). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in August. In the Southern Hemisphere, it will be getting higher gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 6 9.22 -23 56.1 7.767 7.131 48 16.7 5:38 (287, 18)
July 13 6 14.73 -23 54.2 7.735 7.113 49 16.7 5:36 (284, 22)
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It approaches to Sun down to 0.09 a.u. on Jan. 13, 2025. According to the calculation, it will brighten up to -1 mag. But probably, it will be disintegrated. At the high light, it may be observable after the perihelion passage only in the Southern Hemisphere. Now it is 16.8 mag (July 5, ATLAS Chile). It will brighten rapidly after this. 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)
July 6 12 54.23 -69 40.0 3.076 3.564 110 17.0 18:31 ( 5, 55)
July 13 12 51.52 -67 20.8 3.046 3.474 106 16.8 18:34 ( 12, 56)
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Now it is 16.5 mag (June 23, ATLAS-HKO, Haleakala). It stays 17 mag for a while. It will be getting lower gradually after this, and it will be unobservable in September in the Northern Hemisphere, or in October in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 12 42.82 1 16.4 3.281 3.354 85 16.8 18:31 (161, 52)
July 13 12 47.18 0 28.3 3.364 3.340 79 16.9 18:34 (150, 51)
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It brightened up to 14 mag in early 2023 and 2023 autumn. Now it is 17.3 mag (July 6, ATLAS-HKO, Haleakala). Fading slowly. 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)
July 6 22 9.02 22 18.6 4.395 4.924 115 16.9 3:13 (180, 33)
July 13 22 0.56 22 38.5 4.351 4.969 122 16.9 2:37 (180, 32)
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Now it is 17.3 mag (June 28, A. Diepvens). Brightening slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in September.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 3 14.17 37 29.6 3.559 3.017 50 17.1 5:38 (211, 8)
July 13 3 26.13 39 14.9 3.457 2.979 54 16.9 5:36 (208, 8)
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Now it is 16.4 mag (May 4, Toshiyuki Takahashi). 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)
July 6 15 1.47 -1 14.1 2.245 2.867 118 17.0 20:03 (180, 56)
July 13 15 3.35 -1 34.0 2.323 2.866 112 17.1 19:37 (180, 57)
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Now it is 17.5 mag (July 2, ATLAS-HKO, Haleakala). It stays 18 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)
July 6 1 50.71 17 39.7 1.928 1.885 72 17.4 5:38 (202, 34)
July 13 2 4.33 20 4.0 1.864 1.879 75 17.3 5:36 (198, 33)
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Now it is 16.5 mag (July 4, A. Diepvens). 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)
July 6 21 42.48 49 5.6 3.998 4.288 99 17.3 2:47 (180, 6)
July 13 21 27.84 49 11.6 3.935 4.300 104 17.3 2:04 (180, 6)
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Now it is 17.8 mag (June 29, ATLAS Chile). Fading slowly. It will be fainter than 18 mag soon. 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)
July 6 14 10.50 -16 15.4 3.176 3.677 111 17.6 19:12 (180, 71)
July 13 14 14.51 -15 54.2 3.289 3.700 105 17.7 18:49 (180, 71)
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Now it is 17.6 mag (July 6, ATLAS-HKO, Haleakala). 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)
July 6 0 16.89 30 37.0 6.514 6.548 87 17.7 5:20 (180, 24)
July 13 0 14.09 31 1.3 6.356 6.503 93 17.6 4:50 (180, 24)
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It brightened up to 14.5 mag from February to March (Mar. 11, W. Pei). Now it is 17.2 mag (June 25, ATLAS-MLO, Mauna Loa). It will fade out rapidly after this. It will be fainter than 18 mag soon. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it will be getting lower gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 11 43.51 3 33.2 2.067 1.979 70 17.7 18:31 (142, 44)
July 13 11 57.06 1 41.1 2.164 2.015 67 17.9 18:34 (135, 44)
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Now it is 17.1 mag (July 1, ATLAS Chile). It stays 18 mag for a while. It stays extremely low in the Northern Hemisphere. But it will become high in spring. In the Southern Hemisphere, it stays observable in good condition. It is expected to brighten up to 13 mag in 2026, and it will be observable in excellent condition in the Northern Hemisphere. In the Southern Hemisphere, it locates very low at the high light.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 18 56.61 -42 25.5 7.011 7.975 160 17.7 0:02 ( 0, 83)
July 13 18 51.70 -42 9.5 6.979 7.932 158 17.7 23:25 ( 0, 83)
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Now it is 16.5 mag (June 13, ATLAS-MLO, Mauna Loa). It will fade out rapidly after this. 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)
July 6 21 52.42 -4 15.8 1.055 1.912 134 17.8 2:56 (180, 59)
July 13 21 50.13 -5 5.6 1.044 1.950 142 17.9 2:27 (180, 60)
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Now it is 16.9 mag (July 1, G. Duszanowicz). Fading slowly. It will be fainter than 18 mag soon. In the Northern Hemisphere, it will be getting lower 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)
July 6 17 57.35 -15 52.0 2.224 3.212 163 17.8 22:57 (180, 71)
July 13 17 42.94 -18 16.4 2.266 3.215 154 17.8 22:15 (180, 73)
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It will approach to Sun down to 0.12 a.u. on Aug. 4. It will brighten up to 11 mag, but it is not observable at the high light. It brightens up to 10.5 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it is not observable now. In the Southern Hemisphere, it will be unobservable in August. But it will be observable again in August.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
July 6 5 52.10 14 37.3 1.803 0.896 18 20.3 5:38 (252, 0)
July 13 6 24.07 15 46.2 1.653 0.739 16 19.3 5:36 (252, -2)
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