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Now it is very bright as 3.6 mag (Dec. 16, Marco Goiato). Visible with naked eyes. It is approaching to Earth down to 0.08 a.u., and it looks so large as 3 times of Moon. In the Northern Hemisphere, it stays observable in excellent condition. In the Southern Hemisphere, it will be unobservable soon.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 4 59.09 40 49.9 0.084 1.063 158 3.3 23:03 (180, 83)
Dec. 29 6 27.98 54 37.8 0.109 1.078 148 3.8 23:52 (180, 71)
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Now it is very bright as 9.0 mag (Dec. 14, Juan Jose Gonzalez). It is observable in excellent condition in the Northern Hemisphere. It stays low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 2 33.03 31 18.3 0.648 1.507 133 9.0 20:31 ( 0, 86)
Dec. 29 2 50.18 30 18.1 0.706 1.540 130 9.4 20:20 ( 0, 85)
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Now it is bright as 9.5 mag (Dec. 14, Marco Goiato). It stays 9-10 mag until January. In the Northern Hemisphere, it stays observable in good condition for a long time until it fades out. It locates low in the Southern Hemispehre.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 8 31.50 37 3.9 0.768 1.670 144 9.5 2:31 (180, 88)
Dec. 29 8 34.55 39 43.5 0.779 1.699 149 9.7 2:07 (180, 85)
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Now it is 10.1 mag (Dec. 4, Thomas Lehmann). It stays at 11 mag until February. In the Northern Hemisphere, it stays observable for a long time until it fades out. But it stays extremely low. It will never be observable again in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 18 25.57 15 24.4 2.374 1.731 39 10.8 18:23 (103, 9)
Dec. 29 18 46.06 17 44.4 2.362 1.746 41 10.9 18:27 (106, 8)
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It brightened up to 7.7 mag in June (June 19, Juan Jose Gonzalez). Now it is fading. But it is still bright as 10.6 mag (Dec. 7, Chris Wyatt). In the Southern Hemisphere, it stays observable in good condition for a long time until the comet will fade out. In the Northern Hemisphere, it is not observable for a long time until autumn in 2019 when the comet fades out down to 16 mag.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 17 37.39 -84 9.7 3.022 2.683 60 11.3 5:33 (353,-35)
Dec. 29 19 35.53 -85 54.7 3.032 2.727 62 11.4 18:27 ( 5,-34)
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Bright new comet discovered at 12 mag. It will approach to Earth down to 0.17 a.u. in February. Then it will brighten up to 7 mag and will be observable in excellent condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 14 17.57 -24 36.2 1.659 1.278 50 12.7 5:33 (321, 19)
Dec. 29 14 16.31 -24 12.5 1.438 1.232 57 12.2 5:36 (327, 23)
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Now it is 11.5 mag (Dec. 14, Juan Jose Gonzalez). It stays 12 mag for a long time until spring.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 7 43.60 -15 36.2 2.367 3.125 133 12.3 1:44 ( 0, 39)
Dec. 29 7 27.87 -17 34.0 2.373 3.163 136 12.4 1:01 ( 0, 37)
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Now it is 13.1 mag (Dec. 4, Thomas Lehmann). It will be fading slowly after this. It is observable in good condition in the Northern Hemisphere. In the Southern Hemisphere, it is not observable until summer in 2019.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 15 10.32 40 30.9 3.622 3.500 75 12.8 5:33 (246, 48)
Dec. 29 15 20.07 40 33.3 3.624 3.546 77 12.9 5:36 (247, 52)
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Now it is 13.3 mag (Dec. 5, Sandor Szabo). It stays at 12-13 mag for a long time until autumn in 2019.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 22 35.57 -5 58.7 2.336 2.176 68 13.0 18:23 ( 38, 42)
Dec. 29 22 47.53 -5 6.4 2.390 2.156 64 12.9 18:27 ( 44, 40)
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New bright comet discovered by three amateur comet hunters. It brightened rapidly from 10 mag up to 8 mag just after the discovery. But after that, the brightness evolution became slow. Now it is 9.5 mag (Dec. 9, Alan Hale). In the Northern Hemisphere, it will never be observable again after this. In the Southern Hemisphere, it will appear in the morning sky in February. But it may be fainter than 18 mag at that time.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 19 20.82 -18 14.6 1.450 0.621 19 13.0 18:23 ( 67, 0)
Dec. 29 19 32.86 -21 1.8 1.665 0.756 14 14.3 18:27 ( 68, -5)
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Now it is 14.0 mag (Nov. 26, Chris Wyatt). It will brighten up to 10-11 mag in autumn in 2019. It stays observable in good condition for a while in the Southern Hemisphere. In the Northern Hemisphere, it stays extremely low for a long time.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 1 7.47 -36 44.7 4.275 4.366 88 13.6 19:04 ( 0, 18)
Dec. 29 1 4.77 -34 55.4 4.322 4.322 83 13.5 18:34 ( 0, 20)
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Now it is bright as 12.9 mag (Dec. 5, Sandor Szabo).
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 22 54.40 -0 22.7 5.943 5.768 75 13.6 18:23 ( 36, 49)
Dec. 29 22 57.60 -0 6.0 6.050 5.768 68 13.6 18:27 ( 45, 45)
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Now it is 13.7 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It is observable at 14 mag in excellent condition until March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 4.77 1 56.0 1.089 1.626 103 14.0 5:04 ( 0, 57)
Dec. 29 11 15.74 0 16.7 1.044 1.632 107 13.9 4:47 ( 0, 55)
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It brightened up to 6.8 mag in September (Sept. 17, Seiichi Yoshida). Now it is fading rapidly. It has already faded down to 13.8 mag (Dec. 15, R. Ramlow). It is observable in excellent condition in the Southern Hemisphere. It locates low after this in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 6 37.37 -39 1.5 1.005 1.695 116 14.0 0:37 ( 0, 16)
Dec. 29 6 27.88 -37 52.8 1.060 1.760 118 14.4 0:00 ( 0, 17)
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Now it is 14.0 mag (Nov. 14, Kunihiro Shima). It stays 13-14 mag until summer in 2019. It is not observable now.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 17 3.50 -8 39.5 4.170 3.262 19 14.2 5:33 (281, 1)
Dec. 29 17 7.97 -9 53.6 4.133 3.257 23 14.2 5:36 (286, 6)
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Now it is 14.4 mag (Dec. 12, Toshihiko Ikemura, Hirohisa Sato). It will be fading slowly after this. It is observable in excellent condition until spring in the Northern Hemispehre. In the Southern Hemisphere, it will be hardly observable after this.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 45.28 38 17.4 4.205 4.588 106 14.4 5:33 (215, 86)
Dec. 29 11 38.80 39 12.1 4.133 4.623 114 14.4 5:10 (180, 86)
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Now it is 14.3 mag (Nov. 30, Seiichi Yoshida). It stays at 14 mag until winter. It is observable in excellent condition in the Northern Hemisphere. In the Southern Hemisphere, it is not observable until summer in 2019.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 13 6.50 78 1.7 1.474 2.027 109 14.4 5:33 (187, 46)
Dec. 29 13 22.60 78 34.4 1.488 2.048 110 14.4 5:36 (185, 46)
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Now it is 14.8 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It will brighten up to 13-14 mag in winter, and it will be observable in excellent condition. It locates low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 14.34 27 28.6 1.612 2.156 109 14.5 5:13 ( 0, 82)
Dec. 29 11 22.41 27 43.4 1.540 2.148 114 14.4 4:54 ( 0, 83)
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It brightened very rapidly up to 13.8 mag in August in 2017 (Aug. 22, Kunihiro Shima). Although it was faint as 16-17 mag in November, it brightened up to 14.7 mag in December (Dec. 12, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable in excellent condition after this. It stays extremely low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 19.16 32 47.0 2.190 2.696 110 14.9 5:18 ( 0, 88)
Dec. 29 11 23.03 33 50.7 2.145 2.725 116 15.1 4:55 ( 0, 89)
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Now it is 14.5 mag (Aug. 16, P. Camilleri, H. Williams). It stays 15 mag from 2018 to 2019, and it will be observable for a long time in the Southern Hemisphere. In the Northern Hemisphere, it will never be observable again.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 19 13.56 -66 38.1 4.576 3.939 44 15.0 18:23 ( 26,-27)
Dec. 29 19 37.96 -65 48.7 4.582 3.933 43 15.0 18:27 ( 27,-27)
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Now it is bright as 15.1 mag (Nov. 21, Artyom Novichonok). It stays 14 mag for a long time in 2019. In the Southern Hemisphere, it is observable in excellent condition. In the Northern Hemisphere, it is observable in low sky until early January, but it will be unobservable after that.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 30.08 -37 22.8 3.514 3.505 81 15.3 5:29 ( 0, 18)
Dec. 29 11 28.56 -39 58.1 3.399 3.476 86 15.2 5:00 ( 0, 15)
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Now it is 15.2 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It stays 15 mag until March. It is observable in excellent condition in the Northern Hemisphere. It is not observable at all in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 10 50.15 64 51.8 2.699 3.283 118 15.3 4:50 (180, 60)
Dec. 29 10 27.73 68 43.3 2.644 3.280 122 15.3 4:01 (180, 56)
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Now it is 15.0 mag (Dec. 5, Sandor Szabo). It is expected to brighten up to 7-8 mag in 2020. In 2018, it will be observable at 15-16 mag in good condition from autum to winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 3 11.68 -4 54.9 5.060 5.745 130 15.6 21:08 ( 0, 50)
Dec. 29 3 8.11 -4 27.3 5.083 5.685 123 15.6 20:37 ( 0, 51)
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Although it was faint as 18 mag until Dec. 10, it suddenly brightened in outburst up to 15.4 mag on Dec. 12 (Dec. 12, A. Heinze). It stays observable in good condition for a while.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 1 43.67 3 37.5 1.992 2.572 115 15.7 19:41 ( 0, 59)
Dec. 29 1 46.93 4 28.8 2.087 2.585 109 15.9 19:16 ( 0, 60)
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Now it is 14.6 mag (Dec. 5, Sandor Szabo). It will be fading after this. It stays observable in excellent condition for a while 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)
Dec. 22 23 46.94 -15 9.9 2.177 2.249 81 16.0 18:23 ( 12, 39)
Dec. 29 23 57.36 -13 34.9 2.278 2.273 77 16.3 18:27 ( 19, 40)
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It approached to Earth down to 0.3 a.u., and brightened up to 8.3 mag in July (July 22, Juan Jose Gonzalez). Now it is fading. It has faded down to 13.2 mag in September (Sept. 24, Thomas Lehmann). Appearing in the morning sky in the Northern Hemisphere. It will appear in the morning sky in January also in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 15 28.53 -2 37.4 3.018 2.379 41 16.2 5:33 (292, 24)
Dec. 29 15 28.78 -1 49.5 2.985 2.453 48 16.3 5:36 (297, 30)
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Now it is 17.4 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It was predicted to be observable at 16.5 mag in good condition from autumn to winter. But recently, it is a bit fainter than predicted actually. It locates somewhat low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 8 34.23 24 9.5 1.602 2.471 144 16.4 2:34 ( 0, 79)
Dec. 29 8 30.65 23 58.9 1.573 2.487 152 16.4 2:03 ( 0, 79)
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Now it is 16.7 mag (Nov. 29, Toshihiko Ikemura, Hirohisa Sato). It is observable at 16.5 mag in good condition in winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 4 27.84 2 54.8 0.864 1.784 149 16.5 22:24 ( 0, 58)
Dec. 29 4 23.69 5 48.2 0.881 1.778 144 16.5 21:52 ( 0, 61)
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It brightened up to 14.7 mag in early 2018 (Jan. 25, Catalina Sky Survey). Now it is fading slowly. Now it is 16.4 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable in good condition for a long time until the comet fades out. It is never observable again in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 6 59.55 71 49.2 5.378 6.067 130 16.6 1:02 (180, 53)
Dec. 29 6 37.33 72 32.4 5.404 6.091 130 16.6 0:12 (180, 53)
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Now it is 16.1 mag (Dec. 12, Toshihiko Ikemura, Hirohisa Sato). It stays 16-17 mag for a long time until 2020. It is observable in good condition in the Northern Hemisphere. It is not observable at all in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 55.01 70 46.7 8.031 8.455 112 16.7 5:33 (183, 54)
Dec. 29 11 57.49 71 17.2 7.996 8.453 114 16.6 5:29 (180, 54)
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Now it is 17.3 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17 mag in good condition in winter. It locates low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 16.35 21 52.5 2.008 2.492 107 17.0 5:15 ( 0, 77)
Dec. 29 11 19.43 22 41.1 1.964 2.532 114 17.0 4:51 ( 0, 78)
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It brightened up to 7 mag from May to June in 2017. Now it is fading. It has already faded down to 15.9 mag (Dec. 8, Thomas Lehmann). In the Southern Hemisphere, it stays observable for a long time after this. It will never be observable again in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 0 50.37 -47 32.5 6.309 6.232 81 17.2 18:47 ( 0, 8)
Dec. 29 0 51.13 -46 29.9 6.442 6.290 76 17.2 18:27 ( 1, 9)
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Now it is 17.2 mag (Dec. 12, Toshihiko Ikemura, Hirohisa Sato). Fading slowly. It stays observable at 17 mag in good condition until summer in 2019.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 42.10 5 49.1 9.748 9.903 96 17.2 5:33 (356, 61)
Dec. 29 11 42.95 5 56.2 9.642 9.913 103 17.2 5:14 ( 0, 61)
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Now it is 16.0 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It was observed at 18 mag in last winter. It will be observable in good condition at 16-17 mag also in this winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 7 17.96 2 17.4 2.111 3.012 151 17.2 1:18 ( 0, 57)
Dec. 29 7 13.55 2 9.7 2.103 3.030 156 17.2 0:46 ( 0, 57)
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Now it is 17.9 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17 mag in good condition in winter in the Northern Hemisphere. It locates very low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 10 46.20 33 33.2 0.774 1.505 117 17.3 4:45 ( 0, 88)
Dec. 29 10 59.93 34 18.3 0.758 1.519 120 17.2 4:31 ( 0, 89)
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First return of a new periodic comet which brightened up to 17.5 mag in 2010. Now it is 17.0 mag (Nov. 29, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this, and will be fainter than 18 mag in late January. 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)
Dec. 22 5 57.33 36 45.7 1.082 2.052 166 17.3 23:53 (180, 88)
Dec. 29 5 51.99 37 14.8 1.109 2.072 163 17.4 23:20 (180, 88)
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Now it is 16.3 mag (Dec. 8, Ken-ichi Kadota). It will be getting higher gradually after this. But it will be fading, and will be fainter than 18 mag in January.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 22 32.14 -14 58.4 1.108 1.120 64 17.4 18:23 ( 33, 34)
Dec. 29 23 6.49 -11 18.4 1.164 1.187 66 18.0 18:27 ( 34, 37)
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Now it is 17.2 mag (Nov. 29, Toshihiko Ikemura, Hirohisa Sato). It was observed at 17 mag in last winter. It will be observable in good condition at 17.5 mag also in this winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 4 52.16 4 57.8 7.153 8.058 155 17.4 22:48 ( 0, 60)
Dec. 29 4 46.93 4 41.8 7.208 8.066 148 17.4 22:15 ( 0, 60)
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Now it is 17.2 mag (Nov. 30, Toshihiko Ikemura, Hirohisa Sato). It will be fading gradually after this, and it will be fainter than 18 mag in winter. In the Northern Hemisphere, it stays observable in good condition for a long time. In the Southern Hemisphere, it will never be observable again.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 23 5.14 66 38.7 7.656 7.988 106 17.4 18:23 (166, 56)
Dec. 29 23 11.71 65 47.3 7.729 8.016 103 17.5 18:27 (161, 55)
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First return of a new periodic comet discovered in 2014. It has not been recovered yet. Now it is not detected, fainter than 20.0 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). The condition of this apparition is excelllent. It will brighten rapidly, and will be observable at 15.5 mag in excellent condition in March.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 11 7.09 3 40.6 1.461 1.941 103 17.7 5:06 ( 0, 59)
Dec. 29 11 16.94 2 42.6 1.367 1.914 107 17.5 4:48 ( 0, 58)
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Now it is 17.8 mag (Dec. 14, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17.5 mag in excellent condition in January.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 8 13.98 7 35.9 0.762 1.662 144 17.6 2:14 ( 0, 63)
Dec. 29 8 15.01 5 25.8 0.732 1.655 149 17.5 1:47 ( 0, 60)
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Now it is 18.7 mag (Dec. 14, Toshihiko Ikemura, Hirohisa Sato). It brightened up to 16 mag in 2018 spring. It stays observable in good condition until 2019 spring when the comet will be fainter than 18 mag. It is fainter than this ephemeris recently.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 10 57.06 8 36.3 3.235 3.654 107 17.5 4:56 ( 0, 63)
Dec. 29 10 56.94 10 5.5 3.170 3.699 115 17.5 4:29 ( 0, 65)
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Now it is 17.2 mag (Nov. 29, Toshihiko Ikemura, Hirohisa Sato). It is observable at 17.5 mag until January, in good condition in the Northern Hemisphere. It locates very low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 6 14.21 42 59.1 2.871 3.811 160 17.6 0:15 (180, 82)
Dec. 29 6 8.22 43 24.8 2.887 3.823 159 17.6 23:37 (180, 82)
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It is expected to brighten up to 10 mag in autumn in 2019. Now it is 17.4 mag (Dec. 10, Toshihiko Ikemura, Hirohisa Sato). In the Northern Hemisphere, it stays observable for a long time while the comet is brightening. In the Southern Hemisphere, it it not observable until late September in 2019.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 13 27.81 50 33.4 3.420 3.640 95 17.8 5:33 (224, 64)
Dec. 29 13 36.19 52 56.9 3.284 3.573 99 17.6 5:36 (215, 66)
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It was expected to be observable at 17.5 mag in good condition in winter in the Northern Hemisphere. But actually, it is so faint as 21.0 mag (Oct. 5, K. Sarneczky, et. al). It locates low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 5 30.52 34 7.7 2.077 3.045 167 17.7 23:26 ( 0, 89)
Dec. 29 5 24.58 34 27.1 2.088 3.038 161 17.7 22:53 ( 0, 89)
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Now it is 17.7 mag (Dec. 8, Toshihiko Ikemura, Hirohisa Sato). First return of a new periodic comet which brightened up to 16 mag in 2011. It is observable at 17.5 mag in good condition in winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 2 35.79 12 49.5 1.675 2.434 130 17.7 20:32 ( 0, 68)
Dec. 29 2 36.97 12 16.9 1.731 2.420 123 17.7 20:06 ( 0, 67)
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Now it is 18.8 mag (Nov. 29, Toshihiko Ikemura, Hirohisa Sato). It is observable at 18 mag in winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 6 58.44 21 12.0 2.553 3.516 166 17.9 0:59 ( 0, 76)
Dec. 29 6 53.54 21 25.2 2.530 3.510 174 17.9 0:26 ( 0, 76)
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Now it is 17.0 mag (Nov. 27, MASTER-II Observatory, Tunka). It will be fading after this, and will be fainter than 18 mag in December. It is observable in good condition in the Northern Hemisphere. It is not observable in the Southern Hemisphere. Its cometary activity was observed on Mar. 26 (M. Mommert, D. Polishook, N. Moskovitz).
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 0 58.30 46 38.9 2.221 2.805 116 17.9 18:55 (180, 78)
Dec. 29 1 2.31 45 49.1 2.344 2.859 111 18.1 18:32 (180, 79)
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Now it is 18.1 mag (Dec. 14, Toshihiko Ikemura, Hirohisa Sato). It is observable at 18 mag in winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Dec. 22 7 25.65 4 34.3 6.725 7.606 151 18.0 1:25 ( 0, 60)
Dec. 29 7 23.49 4 21.6 6.686 7.602 157 17.9 0:56 ( 0, 59)
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