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It brightened up to -3 mag due to the forward scattering on Oct. 9 in the SOHO coronagraph images (Q.-c. Zhang, Charles S. Morris). It became a great comet of 0 mag on the ground. Now it is 8.9 mag (Nov. 28, Virgilio Gonano). Fading rapidly. In the Northern Hemisphere, it will be unobservable in January. But it will be observable again in January. In the Southern Hemisphere, it is not observable now, but it will appear in March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 19 6.36 4 26.9 1.929 1.455 47 8.6 18:18 ( 74, 29)
Dec. 7 19 15.39 4 44.1 2.129 1.574 43 9.1 18:18 ( 77, 26)
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Brightening rapidly. It is expected to brighten up to 10 mag until Decemebr. Now it is 11.9 mag (Nov. 23, Katsumi Yoshimoto). It will turn to fade out rapidly after the peak. It will be fainter than 18 mag in March. 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)
Nov. 30 12 14.55 38 7.4 0.636 1.113 83 9.9 5:19 (254, 62)
Dec. 7 13 42.01 56 33.7 0.547 1.118 88 9.6 5:24 (222, 52)
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It approaches to Sun down to 0.09 a.u. on Jan. 13. 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 10.0 mag (Nov. 28, Michael Mattiazzo). It brightens up to -1 mag, but it will turn to fade out rapidly after that. In the Northern Hemisphere, it will never be observable after this. In the Southern Hemisphere, it will be unobservable in December.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 15 51.48 -40 56.0 2.170 1.293 20 11.8 5:19 (306,-22)
Dec. 7 16 8.64 -39 42.3 2.023 1.145 19 11.1 5:24 (306,-18)
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It returned for the first time in 68 years. It brightened up to 6.2 mag in early summer (July 1, Virgilio Gonano). Now it is 10.1 mag (Nov. 10, Mike Olason). Fading gradually. Now it is not observable. It will appear in January.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 16 37.67 -11 17.8 3.387 2.425 10 11.5 18:18 ( 83,-10)
Dec. 7 16 49.20 -12 25.2 3.462 2.499 10 11.7 5:24 (277,-11)
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Bright new Kreutz sungrazer comet. Large outburst occured on Oct. 18 and it brightened up to 8.2 mag (Oct. 20, Martin Masek). It approached to Sun down to 0.008 a.u. on Oct. 28. It was expected to brighten up to 2 mag, or -4.5 mag at best. However, it completely disappered at the perihelion. It is appearing in the morning sky, but probably nothing remains.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 11 4.69 -36 0.1 0.959 1.111 69 12.3 5:19 (345, 17)
Dec. 7 10 25.11 -39 27.5 0.959 1.266 81 12.7 5:22 ( 0, 15)
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Now it is 12.9 mag (Nov. 28, Osamu Miyazaki). Fading slowly. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it is not observable now.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 4 54.19 68 17.1 2.986 3.731 133 12.6 0:22 (180, 57)
Dec. 7 4 11.65 68 23.3 2.993 3.743 133 12.6 23:03 (180, 57)
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Now it is 13.4 mag (Oct. 31, Thomas Lehmann). It stays 14 mag for a while. It will be unobservable in January in the Northern Hemisphere, or in December in the Southern Hemisphere. But it will be observable again in March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 19 14.42 -20 52.9 3.051 2.373 39 13.2 18:18 ( 52, 14)
Dec. 7 19 26.81 -18 58.3 3.110 2.379 35 13.2 18:18 ( 56, 12)
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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 14.6 mag (Oct. 22, Hidetaka Sato). Fading slowly. In the Northern Hemisphere, it is not observable now, but it will appear in February. 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)
Nov. 30 15 46.18 -47 45.1 4.172 3.326 27 13.3 5:19 (313,-24)
Dec. 7 15 57.19 -47 50.2 4.243 3.402 27 13.4 5:24 (315,-21)
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It is expected to brighten up to 13.5 mag, and it will be observable in good condition in winter. Now it is 14.8 mag (Nov. 25, Ken-ichi Kadota). It will fade out rapidly after this. 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)
Nov. 30 5 29.77 5 5.7 0.756 1.708 157 13.7 0:56 ( 0, 60)
Dec. 7 4 59.73 13 45.9 0.737 1.717 171 13.7 23:50 ( 0, 70)
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Major outburst occured between Nov. 1 and 2. Another outburst occured in late November. Now it is 11.6 mag (Nov. 28, Juan Jose Gonzalez). It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 10 11.98 9 18.1 6.061 6.247 96 13.9 5:19 (350, 64)
Dec. 7 10 12.70 9 7.3 5.949 6.248 103 13.8 5:09 ( 0, 64)
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Now it is 14.9 mag (Nov. 3, Hiroshi Abe). It stays 14 mag for a while. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 6 42.80 3 21.5 5.054 5.861 141 14.3 2:07 ( 0, 58)
Dec. 7 6 40.62 3 36.4 4.983 5.843 148 14.2 1:38 ( 0, 59)
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It became much brighter than expected. Now it is 13.1 mag (Nov. 1, Thomas Lehmann). It will fade out rapidly after this. In the Northern Hemisphere, it will be getting higher gradually. In the Southern Hemisphere, it is not observable now, but it will appear in February.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 15 57.31 29 9.2 2.226 1.782 51 14.3 5:19 (245, 16)
Dec. 7 16 14.62 26 52.7 2.282 1.821 50 14.5 5:24 (249, 18)
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Now it is 14.1 mag (Aug. 29, Chris Wyatt). It stays 14 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in winter. 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)
Nov. 30 14 31.81 -19 19.0 5.885 5.022 26 14.4 5:19 (298, 5)
Dec. 7 14 38.60 -19 17.9 5.838 5.029 31 14.3 5:24 (302, 9)
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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 14.6 mag (Nov. 19, Ken-ichi Kadota). It stays 15 mag for a while. It will be getting lower gradually after this, and it will be unobservable in February in the Southern Hemisphere, or in March in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 22 43.20 -4 40.8 4.218 4.375 92 14.5 18:18 ( 5, 50)
Dec. 7 22 46.69 -4 19.3 4.295 4.346 86 14.5 18:18 ( 14, 50)
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Now it is 12.5 mag (Nov. 20, Mike Olason). It will fade out rapidly after this. It will be fainter than 18 mag in March. It will be unobservable in January in the Southern Hemisphere, or in February in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 19 27.37 -22 4.2 2.284 1.690 42 14.7 18:18 ( 49, 15)
Dec. 7 19 48.32 -20 49.3 2.341 1.710 40 14.9 18:18 ( 51, 15)
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First return of a new periodic comet which brightened up to 16 mag in 2012. Now it is 14.7 mag (Nov. 13, ATLAS-HKO, Haleakala). It will fade out rapidly after this. It will be fainter than 18 mag in February. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be unobservable in December.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 3 37.58 47 48.1 0.931 1.861 152 14.8 22:58 (180, 77)
Dec. 7 3 20.73 50 24.9 0.976 1.879 146 15.0 22:14 (180, 74)
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Now it is 16.0 mag (Nov. 23, 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 is not observable now.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 8 33.30 72 42.8 1.952 2.576 118 15.1 3:59 (180, 52)
Dec. 7 8 40.94 73 42.7 1.929 2.576 120 15.0 3:39 (180, 51)
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Now it is 15.8 mag (Nov. 4, Thomas Lehmann). It stays 15 mag for a while. In the Northern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 9 15.64 20 28.9 2.128 2.670 112 15.2 4:40 ( 0, 75)
Dec. 7 9 18.33 20 6.1 2.039 2.662 119 15.1 4:15 ( 0, 75)
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It brightened up to 9.6 mag from February to March (Feb. 25, Thomas Lehmann). Now it is 14.7 mag (Nov. 3, Thomas Lehmann). Fading slowly. In the Northern Hemisphere, it will be getting lower gradually. But it will be getting higher again after March. In the Southern Hemisphere, it is not observable now.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 20 39.70 34 0.3 3.923 3.914 82 15.1 18:18 ( 98, 62)
Dec. 7 20 48.48 33 11.9 4.057 3.984 78 15.2 18:18 ( 98, 58)
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Brightening rapidly. Now it is 14.9 mag (Nov. 19, Ken-ichi Kadota). Brightening slowly. It locates somewhat low in the Northern Hemisphere. In the Southern Hemisphere, it is not observable now. It will brighten up to 14 mag from winter to spring. But it is not observable at the high light.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 17 25.66 35 23.0 2.616 2.268 58 15.4 18:18 (117, 25)
Dec. 7 17 48.67 34 50.3 2.562 2.218 58 15.2 18:18 (117, 24)
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Very large comet. It is expected to brighten up to 13 mag in 2031. Now it is 15.3 mag (Nov. 10, 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. In the Northern Hemisphere, it is not observable until 2030.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 3 54.09 -70 48.9 15.711 15.697 87 15.4 23:13 ( 0,-16)
Dec. 7 3 50.12 -70 48.7 15.713 15.673 85 15.4 22:42 ( 0,-16)
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Now it is 15.7 mag (Nov. 13, ATLAS Chile). Fading slowly. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 6 38.00 10 3.1 2.663 3.524 145 15.6 2:03 ( 0, 65)
Dec. 7 6 35.06 9 45.5 2.632 3.537 152 15.5 1:32 ( 0, 65)
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Now it is 18.2 mag (Oct. 13, F. Kugel, J. Nicolas). It will brighten rapidly after this. In the Northern Hemisphere, it will be unobservable in December. In the Southern Hemisphere, it is not observable now. It will brighten up to 10 mag in 2025 spring. But the condition of this apparition is bad. It is not observable when the comet is bright.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 17 33.84 -2 24.8 2.651 1.812 25 15.9 18:18 ( 82, 7)
Dec. 7 17 51.01 -2 44.5 2.600 1.747 24 15.5 18:18 ( 84, 4)
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It brightened up to 8 mag from 2022 summer to 2023 spring. Now it is 15.6 mag (Nov. 11, ATLAS-HKO, Haleakala). It stays 16 mag for a while. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 6 4.78 20 5.6 6.472 7.388 156 15.6 1:30 ( 0, 75)
Dec. 7 6 0.38 20 21.2 6.488 7.442 164 15.6 0:58 ( 0, 75)
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Now it is 16.4 mag (Nov. 11, Ken-ichi Kadota). It stays 15 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)
Nov. 30 8 5.79 -26 40.8 3.823 4.231 107 15.7 3:30 ( 0, 28)
Dec. 7 8 0.63 -26 20.6 3.716 4.208 113 15.6 2:57 ( 0, 29)
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Now it is 16.0 mag (Nov. 20, Katsumi Yoshimoto). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 1 43.77 16 4.1 2.151 2.988 141 15.7 21:05 ( 0, 71)
Dec. 7 1 42.11 15 27.1 2.191 2.962 134 15.7 20:36 ( 0, 71)
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Now it is 15.3 mag (Nov. 6, Toshihiko Ikemura, Hirohisa Sato). It will fade out rapidly after this. It will be fainter than 18 mag in February. 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)
Nov. 30 1 50.37 6 51.5 1.743 2.577 139 15.7 21:12 ( 0, 62)
Dec. 7 1 49.07 7 9.5 1.840 2.611 132 15.9 20:43 ( 0, 62)
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It will be observable at 15 mag for a long time in 2025 in the Northern Hemisphere. Now it is 16.5 mag (Nov. 12, ATLAS-HKO, Haleakala). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition. 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)
Nov. 30 12 8.09 29 54.1 4.716 4.653 80 15.9 5:19 (271, 62)
Dec. 7 12 12.42 31 17.0 4.587 4.632 86 15.8 5:24 (273, 68)
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Fading gradually. It will be fainter than 18 mag in February. In the Northern Hemisphere, it will be unobservable in January. But it will be observable again in January. 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)
Nov. 30 17 4.21 -2 57.7 2.897 2.008 20 15.8 18:18 ( 86, 0)
Dec. 7 17 20.18 -2 49.8 2.989 2.097 20 16.1 18:18 ( 88, -2)
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It was observed at 9-10 mag for a long time in 2023. Now it is 15.8 mag (Nov. 14, 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 February.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 20 54.38 -64 5.0 6.540 6.120 60 15.9 18:18 ( 13,-12)
Dec. 7 20 56.57 -63 26.6 6.660 6.175 56 16.0 18:18 ( 16,-13)
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Now it is 16.4 mag (Nov. 12, ATLAS Chile). It stays 16 mag for a while. It locates somewhat low in the Northern Hemisphere. But it will become high in autumn. In the Southern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 7 7.20 -30 37.1 6.337 6.810 114 16.0 2:31 ( 0, 24)
Dec. 7 7 5.26 -30 44.8 6.277 6.798 118 16.0 2:02 ( 0, 24)
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Now it is 16.5 mag (Nov. 2, Martin Masek). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition. In the Southern Hemisphere, it will be getting higher gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 13 10.39 -1 30.0 2.508 2.042 51 16.0 5:19 (298, 32)
Dec. 7 13 23.80 -2 31.1 2.473 2.071 54 16.1 5:24 (303, 34)
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Now it is 15.8 mag (Nov. 6, ATLAS Chile). It stays 17 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)
Nov. 30 7 14.21 -49 57.5 6.094 6.327 99 16.0 2:38 ( 0, 5)
Dec. 7 7 5.13 -50 34.3 6.103 6.371 101 16.1 2:02 ( 0, 4)
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Now it is 16.8 mag (Oct. 31, Thomas Lehmann). Fading gradually. It will be fainter than 18 mag in March. It stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 23 34.11 6 23.5 0.765 1.427 108 16.1 18:57 ( 0, 62)
Dec. 7 23 56.15 6 27.4 0.804 1.439 106 16.1 18:52 ( 0, 62)
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Parent asteroid of Geminids meteor shower. Now it is 16.3 mag (Nov. 21, Katsumi Yoshimoto). Brightening gradually. It will be unobservable in March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 3 29.35 36 53.4 0.935 1.894 160 16.2 22:49 (180, 88)
Dec. 7 3 2.54 34 34.5 0.907 1.839 152 16.2 21:54 ( 0, 89)
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First return of a new periodic comet which brightened up to 15 mag in 2010. It is expected to brighten up to 15 mag from winter to spring, and it will be observable in excellent condition in the Northern Hemisphere. Now it is 17.2 mag (Nov. 22, Katsumi Yoshimoto). Brightening slowly. 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)
Nov. 30 2 22.68 7 55.1 1.072 1.977 147 16.4 21:44 ( 0, 63)
Dec. 7 2 17.64 9 4.9 1.074 1.935 139 16.2 21:11 ( 0, 64)
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Now it is 16.8 mag (May 18, ATLAS South Africa). It stays 16 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)
Nov. 30 12 13.10 -25 53.2 4.023 3.585 57 16.3 5:19 (327, 21)
Dec. 7 12 21.54 -26 59.8 3.941 3.577 61 16.2 5:24 (333, 22)
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It brightened up to 8.3 mag in 2021-2022 winter (Jan. 6, 2022, Toshiyuki Takahashi). Now it is 15.1 mag (Aug. 2, Thomas Lehmann). 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)
Nov. 30 12 28.33 -53 1.5 9.707 9.168 54 16.5 5:19 (338, -4)
Dec. 7 12 31.39 -53 41.5 9.699 9.212 57 16.5 5:24 (342, -3)
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Now it is 16.5 mag (June 6, Giuseppe Pappa). It stays 16 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in December. In the Southern Hemisphere, it will be getting higher gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 13 43.64 -41 41.1 5.941 5.214 39 16.5 5:19 (321, -3)
Dec. 7 13 44.18 -42 12.5 5.871 5.209 44 16.5 5:24 (326, 1)
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Now it is 16.1 mag (Nov. 1, Thomas Lehmann). Fading slowly. It will be fainter than 18 mag in March. 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)
Nov. 30 9 18.24 -40 19.6 3.692 3.787 87 16.6 4:42 ( 0, 15)
Dec. 7 9 7.23 -41 26.4 3.647 3.834 93 16.6 4:04 ( 0, 13)
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Now it is 16.6 mag (Nov. 14, ATLAS-MLO, Mauna Loa). It stays 16 mag for a while. It will be unobservable in February in the Northern Hemisphere, or in December in the Southern Hemisphere. But it will be observable again in March in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 22 13.79 21 2.0 5.440 5.617 95 16.7 18:18 ( 36, 73)
Dec. 7 22 12.03 20 13.7 5.514 5.573 88 16.7 18:18 ( 52, 68)
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Now it is 16.6 mag (Nov. 8, 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)
Nov. 30 2 46.08 9 56.6 2.991 3.899 153 16.7 22:07 ( 0, 65)
Dec. 7 2 43.43 9 30.8 3.044 3.899 145 16.7 21:37 ( 0, 65)
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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 16.7 mag (Nov. 12, ATLAS South Africa). It stays 17 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)
Nov. 30 6 32.30 -41 36.1 5.598 6.010 110 16.8 1:57 ( 0, 13)
Dec. 7 6 26.06 -41 28.9 5.612 6.058 112 16.8 1:23 ( 0, 13)
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It brightened up to 13.5 mag in last winter (Dec. 5, 2023, Chris Wyatt). Now it is 16.6 mag (Nov. 10, J. Nicolas, F. Kugel). It stays 17 mag for a while. It will be getting higher gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 13 26.09 -2 19.4 3.343 2.773 47 16.8 5:19 (296, 28)
Dec. 7 13 35.17 -3 13.4 3.306 2.810 52 16.9 5:24 (301, 32)
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Very far object. Now it is 16.8 mag (Nov. 6, 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)
Nov. 30 1 1.35 -66 54.6 10.573 10.512 83 16.8 20:22 ( 0,-12)
Dec. 7 0 56.45 -66 11.3 10.635 10.519 80 16.9 19:50 ( 0,-11)
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It brightened up to 12.0 mag in June (June 13, Ken-ichi Kadota). Now it is 17.3 mag (Oct. 31, Hirohisa Sato). Fading gradually. It will be fainter than 18 mag in February. 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)
Nov. 30 9 45.51 31 51.8 1.860 2.375 109 17.0 5:10 ( 0, 87)
Dec. 7 9 46.19 31 59.3 1.828 2.425 115 17.0 4:43 ( 0, 87)
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Now it is 17.3 mag (Nov. 12, ATLAS Chile). 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)
Nov. 30 4 0.87 -16 41.0 3.156 3.973 141 17.1 23:21 ( 0, 38)
Dec. 7 3 57.12 -16 54.2 3.185 3.972 138 17.1 22:50 ( 0, 38)
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First return of a new periodic comet which brightened up to 15 mag in 2010. Now it is 18.7 mag (Nov. 4, Toshihiko Ikemura, Hirohisa Sato). Fading gradually. It will be fainter than 18 mag in February. 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)
Nov. 30 9 41.93 29 20.2 1.722 2.250 109 17.3 5:06 ( 0, 84)
Dec. 7 9 45.21 29 33.0 1.688 2.292 115 17.3 4:42 ( 0, 84)
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Peculiar asteroid moving along a cometary orbit. 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)
Nov. 30 3 38.40 -14 13.6 1.895 2.743 142 17.3 22:59 ( 0, 41)
Dec. 7 3 33.21 -15 0.9 1.885 2.694 137 17.3 22:26 ( 0, 40)
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Now it is 16.8 mag (Nov. 2, Toshihiko Ikemura, Hirohisa Sato). Fading gradually. It will be fainter than 18 mag in January. 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)
Nov. 30 0 45.52 -2 35.0 1.357 2.050 121 17.3 20:07 ( 0, 53)
Dec. 7 0 50.63 -1 49.4 1.431 2.059 115 17.5 19:45 ( 0, 53)
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It will brighten up to 14 mag in 2025 spring. Now it is 17.3 mag (Nov. 21, Ken-ichi Kadota). Brightening gradually. In the Southern Hemisphere, it will be getting lower gradually.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 23 40.69 -27 8.7 1.631 1.990 95 17.3 19:03 ( 0, 28)
Dec. 7 23 45.98 -25 45.4 1.660 1.944 90 17.4 18:40 ( 0, 29)
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Now it is 17.8 mag (Nov. 6, Toshihiko Ikemura, Hirohisa Sato). 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)
Nov. 30 7 41.74 41 1.5 6.303 7.028 134 17.4 3:07 (180, 84)
Dec. 7 7 40.19 41 15.6 6.251 7.042 140 17.4 2:37 (180, 84)
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Now it is 17.4 mag (Nov. 7, ATLAS-HKO, Haleakala). It stays 18 mag for a while. In the Northern Hemisphere, it will be getting lower gradually. But it will be getting higher again after January. In the Southern Hemisphere, it is not observable now, but it will appear in March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 19 10.91 17 54.0 5.152 4.684 56 17.5 18:18 ( 86, 38)
Dec. 7 19 13.32 16 58.0 5.251 4.709 52 17.5 18:18 ( 89, 32)
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Now it is 17.9 mag (Nov. 11, ATLAS-HKO, Haleakala). Fading gradually. It will be fainter than 18 mag in December. 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)
Nov. 30 4 30.71 40 43.1 2.154 3.103 160 17.6 23:50 (180, 84)
Dec. 7 4 7.65 41 24.6 2.223 3.161 158 17.7 23:00 (180, 83)
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It brightened up to 14.4 mag in summer (Aug. 17, Hiroshi Abe). Now it is 17.7 mag (Nov. 23, Ken-ichi Kadota). It will fade out rapidly after this. It will be fainter than 18 mag in December. 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)
Nov. 30 6 1.09 43 41.5 0.999 1.919 150 17.7 1:27 (180, 81)
Dec. 7 5 49.75 45 29.6 1.031 1.967 154 18.0 0:48 (180, 80)
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Now it is 17.4 mag (Nov. 4, ATLAS-MLO, Mauna Loa). 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)
Nov. 30 6 59.25 -5 12.4 3.844 4.580 133 17.8 2:24 ( 0, 50)
Dec. 7 6 56.25 -6 2.0 3.785 4.573 138 17.8 1:53 ( 0, 49)
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Now it is 17.8 mag (Oct. 20, Ken-ichi Kadota). Fading slowly. 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.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 10 10.69 31 35.0 2.154 2.577 103 17.8 5:19 (316, 85)
Dec. 7 10 13.47 31 41.0 2.105 2.613 110 17.8 5:10 ( 0, 87)
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Now it is 18.0 mag (Nov. 10, ATLAS Chile). 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)
Nov. 30 5 17.05 -59 10.5 4.745 4.987 98 17.8 0:42 ( 0, -4)
Dec. 7 5 0.13 -59 56.5 4.767 4.991 97 17.9 23:51 ( 0, -5)
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Now it is 17.9 mag (May 17, J. L. Virlichie, P. Traverse, H. Roy). It stays 18 mag for a while. In the Northern Hemisphere, it is not observable now, but it will appear in December. In the Southern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 12 56.72 -47 18.0 6.140 5.540 48 17.9 5:19 (331, -2)
Dec. 7 12 58.80 -47 29.6 6.066 5.527 52 17.8 5:24 (336, 1)
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Now it is 17.8 mag (Nov. 1, Purple Mountain Observatory, XuYi Station). Fading slowly. It will be fainter than 18 mag in December. In the Northern Hemisphere, it stays observable in good condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 30 3 2.10 15 48.2 3.629 4.567 159 17.8 22:23 ( 0, 71)
Dec. 7 2 58.25 15 40.5 3.688 4.579 151 17.9 21:52 ( 0, 71)
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Now it is 18.0 mag (Aug. 18, Taras Prystavski). 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)
Nov. 30 7 45.73 37 44.8 8.078 8.792 134 18.0 3:11 (180, 87)
Dec. 7 7 40.98 37 45.0 8.005 8.797 141 17.9 2:38 (180, 87)
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Now it is 17.4 mag (Oct. 1, Martin Masek). Fading gradually. It will be fainter than 18 mag in December. 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)
Nov. 30 7 5.13 35 6.4 1.298 2.166 142 17.9 2:30 (180, 90)
Dec. 7 7 2.77 35 33.6 1.281 2.187 149 17.9 2:00 (180, 89)
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