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Now it is bright as 8.1 mag (Oct. 31, Marco Goiato). It will approach to Earth down to 0.08 a.u. in December, and it is expected to brighten up to 3 mag. In the Northern Hemisphere, it locates low until November, but it stays observable in excellent condition after December. In the Southern Hemisphere, it is observable in good condition until mid December when it brightens up to 3 mag. But it becomes unobservable after that.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 2 0.30 -33 4.8 0.263 1.183 131 7.8 23:10 (180, 88)
Nov. 10 2 2.73 -32 40.4 0.225 1.145 128 7.0 22:45 (180, 87)
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Now it is bright as 10.0 mag (Oct. 22, 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. In the Southern Hemispehre, it is observable in good condition until autumn, but it will be low in winter.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 7 14.89 19 9.9 0.921 1.592 112 9.4 3:23 (198, 34)
Nov. 10 7 30.18 21 12.2 0.878 1.589 116 9.2 3:14 (197, 32)
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It brightened up to 6.8 mag in September (Sept. 17, Seiichi Yoshida). Now it is fading faster than this ephemeris. It has already faded down to 12.2 mag (Nov. 1, Paul Camilleri). 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)
Nov. 3 7 25.68 -29 14.2 0.674 1.261 96 9.5 3:23 (255, 73)
Nov. 10 7 24.85 -32 41.5 0.722 1.318 99 9.9 3:14 (262, 78)
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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 10.3 mag (Oct. 30, 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)
Nov. 3 14 53.15 -68 47.0 2.861 2.415 54 10.5 20:05 ( 20, 23)
Nov. 10 15 2.27 -70 39.2 2.901 2.448 53 10.6 20:14 ( 16, 22)
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Now it is very bright as 9.9 mag (Oct. 30, Chris Wyatt). 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)
Nov. 3 0 50.28 36 54.2 0.447 1.393 148 10.6 22:01 (180, 18)
Nov. 10 1 0.42 36 46.8 0.455 1.395 147 10.7 21:43 (180, 18)
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Now it is very bright as 10.8 mag (Oct. 12, Paul Camilleri). It stays at 10-11 mag until winter. 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)
Nov. 3 16 24.52 2 15.9 2.504 1.755 32 11.1 20:05 ( 88, -7)
Nov. 10 16 39.58 3 48.3 2.491 1.737 32 11.0 20:14 ( 86,-13)
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Now it is 11.8 mag (Oct. 20, 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)
Nov. 3 8 53.41 1 36.6 2.808 2.897 85 12.2 3:23 (235, 37)
Nov. 10 8 48.38 -0 48.2 2.712 2.926 92 12.2 3:14 (231, 43)
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Now it is 11.0 mag (Oct. 20, Juan Jose Gonzalez). It will be fading slowly after this. In the Northern Hemisphere, it stays low until October. But it will be observable in good condition after that. 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)
Nov. 3 13 41.79 43 18.4 3.585 3.194 59 12.3 3:23 (239,-39)
Nov. 10 13 56.50 42 37.1 3.592 3.236 61 12.4 3:14 (240,-38)
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Now it is bright as 12.3 mag (Nov. 1, Paul Camilleri).
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 22 44.81 -0 55.7 5.185 5.770 121 13.3 20:05 (176, 56)
Nov. 10 22 44.63 -1 0.2 5.284 5.769 114 13.3 20:14 (160, 54)
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Now it is 13.5 mag (Nov. 1, Paul Camilleri). 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)
Nov. 3 21 32.12 -9 3.8 1.928 2.346 102 13.5 20:05 (139, 58)
Nov. 10 21 38.40 -8 58.5 1.986 2.319 96 13.5 20:14 (129, 53)
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It must have brightened up to 13 mag in October. But it is not observable at all.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 15 33.73 -11 42.3 2.087 1.162 15 13.5 20:05 ( 69, -9)
Nov. 10 16 2.05 -12 0.5 2.118 1.197 15 14.2 20:14 ( 67,-10)
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Now it is 13.8 mag (Nov. 1, Paul Camilleri). 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)
Nov. 3 1 56.46 -46 11.8 4.123 4.677 118 13.8 23:05 ( 0, 79)
Nov. 10 1 46.71 -45 23.4 4.118 4.632 115 13.7 22:28 ( 0, 80)
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Now it is 13.5 mag (Nov. 1, Paul Camilleri). 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)
Nov. 3 22 45.73 -25 5.4 1.524 2.107 112 14.2 20:05 (169, 80)
Nov. 10 22 52.57 -23 53.4 1.609 2.125 107 14.5 20:14 (141, 76)
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Now it is 14.0 mag (Oct. 7, Seiichi Yoshida). It stays 13-14 mag until summer in 2019. It is not observable now in the Southern Hemisphere. It will be unobservable in November also in the Northeren Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 16 32.95 1 29.9 4.105 3.332 34 14.3 20:05 ( 88, -5)
Nov. 10 16 36.85 -0 10.3 4.146 3.318 29 14.3 20:14 ( 82,-11)
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It brightened up to 8.7 mag in July (July 18, Marco Goiato). Then it faded down to 12.3 mag in August (Aug. 29, Chris Wyatt). Now it is not observable. It will appear in the morning sky in late December.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 14 44.45 -25 25.5 2.943 1.978 10 14.3 20:05 ( 50, -9)
Nov. 10 14 56.51 -24 51.4 3.047 2.070 7 14.6 3:14 (312,-12)
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Now it is 14.1 mag (Oct. 7, 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)
Nov. 3 8 47.04 71 35.5 1.471 1.949 102 14.4 3:23 (192,-20)
Nov. 10 9 28.67 73 25.3 1.458 1.953 104 14.4 3:14 (193,-22)
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Now it is 14.3 mag (Aug. 17, Ken-ichi Kadota). It will be observable at 13-14 mag for a long time from 2017 to 2018. 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)
Nov. 3 12 1.10 34 39.0 4.752 4.359 61 14.4 3:23 (240,-17)
Nov. 10 12 1.18 34 49.2 4.684 4.390 66 14.4 3:14 (237,-14)
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Now it is 15.4 mag (Oct. 7, iTelescope Observatory, Siding Spring). It locates low. But it brightens up to 14.5 mag from October to November.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 17 33.87 -26 5.9 1.183 0.833 43 14.5 20:05 ( 73, 23)
Nov. 10 18 15.23 -26 54.1 1.130 0.842 46 14.5 20:14 ( 73, 24)
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It brightened rapidly in outburst up to 6.9 mag (July 19, Maik Meyer). Then it faded down to 9.3 mag (Aug. 2, Katsumi Yoshimoto). It approached to Sun down to 0.2 a.u. in August, and it was expected to brighten up to 3 mag. However, it must have been already disintegrated. In the Northern Hemisphere, it is appearing in the morning sky. But it will be too faint to observe.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 13 6.08 21 22.0 2.456 1.840 41 14.6 3:23 (259,-23)
Nov. 10 13 15.79 22 46.4 2.491 1.957 47 14.9 3:14 (257,-22)
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Now it is 15.6 mag (Oct. 13, D. Buczynski). Brightening very rapidly. It will brighten up to 14 mag from January to February, and it is expected to be observable in excellent condition.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 9 20.72 14 27.8 1.480 1.666 82 15.2 3:23 (231, 23)
Nov. 10 9 37.74 12 45.5 1.415 1.652 84 15.0 3:14 (232, 25)
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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)
Nov. 3 16 7.89 -68 29.5 4.474 4.001 55 15.0 20:05 ( 24, 28)
Nov. 10 16 33.79 -68 38.7 4.494 3.989 53 15.0 20:14 ( 23, 28)
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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). Now it is not observable. It will appear in the morning sky again in December in the Northern Hemisphere, or in January in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 15 16.07 -5 51.5 2.822 1.876 14 15.0 20:05 ( 70,-16)
Nov. 10 15 18.37 -5 33.8 2.901 1.945 12 15.2 20:14 ( 65,-23)
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Now it is 16.5 mag (Oct. 4, I. Dulevich, S. Plaksa). 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)
Nov. 3 9 53.30 28 20.4 2.202 2.250 79 15.6 3:23 (227, 8)
Nov. 10 10 6.74 28 1.7 2.111 2.234 83 15.4 3:14 (227, 9)
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Now it is 15.8 mag (Oct. 13, S. Shurpakov). It will brighten up to 15 mag in winter. 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)
Nov. 3 11 16.70 44 8.8 3.483 3.345 73 16.0 3:23 (227,-15)
Nov. 10 11 18.49 46 8.4 3.352 3.332 80 15.9 3:14 (223,-14)
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Now it is 16.0 mag (Oct. 11, C. Bell). 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)
Nov. 3 3 43.34 -5 57.7 5.265 6.162 152 16.0 0:56 (180, 61)
Nov. 10 3 38.90 -6 2.0 5.191 6.103 154 15.9 0:25 (180, 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 16.1 mag (Oct. 10, I. Dulevich, S. Plaksa). 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)
Nov. 3 8 21.12 62 8.2 5.581 5.905 104 16.5 3:23 (195,-11)
Nov. 10 8 16.86 63 40.8 5.517 5.928 109 16.5 3:14 (192,-11)
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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 16.0 mag (Sept. 30, J. Drummond). 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)
Nov. 3 1 6.63 -53 40.7 5.416 5.816 109 16.6 22:16 ( 0, 71)
Nov. 10 1 1.84 -53 2.3 5.533 5.876 105 16.6 21:43 ( 0, 72)
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Now it is 17.0 mag (Oct. 12, C. Bell). It is observable at 16.5 mag in good condition from autumn to winter. It locates somewhat low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 8 18.01 26 27.5 2.013 2.387 99 16.7 3:23 (211, 22)
Nov. 10 8 24.65 26 0.4 1.941 2.395 104 16.6 3:14 (208, 23)
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Now it is 16.4 mag (Sept. 29, Catalina Sky Survey). It is observable in good condition in the Southern Hemisphere. It locates somewhat low in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 22 47.13 -18 53.2 2.880 3.423 115 16.7 20:05 (174, 74)
Nov. 10 22 48.28 -18 20.2 2.988 3.439 108 16.8 20:14 (147, 71)
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Now it is 17.0 mag (Oct. 12, D. Buczynski). 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)
Nov. 3 11 14.13 68 0.9 8.412 8.473 90 16.8 3:23 (204,-27)
Nov. 10 11 21.94 68 17.2 8.347 8.470 93 16.7 3:14 (203,-26)
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Now it is 16.2 mag (Sept. 13, ATLAS-MLO, Mauna Loa). It stays 16 mag for a while. In the Northern Hemisphere, it stays observable in good condition after this until it fades out. 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)
Nov. 3 1 25.64 54 3.0 1.572 2.409 138 16.8 22:34 (180, 1)
Nov. 10 1 14.24 53 13.6 1.637 2.467 138 16.9 21:56 (180, 2)
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It stays 15 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)
Nov. 3 11 16.24 -21 46.7 4.341 3.730 46 16.9 3:23 (281, 23)
Nov. 10 11 19.88 -23 43.3 4.230 3.697 51 16.8 3:14 (281, 27)
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Asteroid, but it brightened rapidly. Now it is 16.4 mag (Oct. 9, P. Camilleri, J. Oey).
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 22 27.19 -45 18.9 6.539 6.756 98 17.0 20:05 ( 25, 79)
Nov. 10 22 22.10 -44 50.8 6.635 6.741 91 17.0 20:14 ( 49, 74)
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First return of a new periodic comet which brightened up to 16.5 mag in 2005. Now it is 16.3 mag (Oct. 15, S. Shurpakov). It will be observable at 17 mag in good condition in autumn. It locates low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 1 50.29 31 12.6 1.157 2.120 161 17.1 23:00 (180, 24)
Nov. 10 1 48.82 29 38.9 1.180 2.136 159 17.2 22:31 (180, 25)
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Now it is 17.5 mag (Oct. 10, D. Buczynski). 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)
Nov. 3 10 21.96 20 9.1 2.338 2.215 70 17.1 3:23 (238, 9)
Nov. 10 10 32.69 20 2.4 2.294 2.254 75 17.1 3:14 (237, 10)
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It brightened very rapidly. Now it is 16.7 mag (Oct. 12, Purple Mountain Observatory, XuYi Station). It seems to stay bright for a while.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 23 54.06 -12 50.2 0.942 1.768 132 17.2 21:04 (180, 68)
Nov. 10 23 56.91 -11 6.4 0.995 1.776 126 17.4 20:39 (180, 66)
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Now it is 17.9 mag (Oct. 10, Catalina Sky Survey). It will brighten rapidly. It was expected to be observable at 15.5 mag in good condition in winter. But actually, it is fainter than expected.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 5 1.12 -7 42.0 1.040 1.888 136 17.5 2:14 (180, 63)
Nov. 10 4 59.46 -7 21.4 0.987 1.867 141 17.2 1:45 (180, 62)
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First return of a new periodic comet which brightened up to 17.5 mag in 2010. Now it is 18.1 mag (Oct. 13, J.-F. Soulier). It was expected to brighten up to 16.5 mag from November to December. But actually, it is a bit fainter than expected. It is observable in excellent condition in the Northern Hemisphere. It locates low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 6 10.06 29 40.7 1.194 1.965 127 17.3 3:23 (180, 25)
Nov. 10 6 13.35 30 48.1 1.151 1.971 133 17.3 2:59 (180, 24)
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Now it is 17.4 mag (June 6, Slooh.com Canary Islands Observatory). 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)
Nov. 3 11 28.47 5 56.6 10.445 9.835 49 17.3 3:23 (259, 5)
Nov. 10 11 31.13 5 50.1 10.360 9.844 56 17.3 3:14 (257, 8)
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Now it is 17.0 mag (Oct. 12, ATLAS-MLO, Mauna Loa). Fading now. It stays observable in good condition for a long time after this in the Southern Hemisphere. It stays low in the Northern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 22 51.29 -39 45.4 4.660 5.012 105 17.3 20:05 ( 9, 85)
Nov. 10 22 45.77 -39 52.4 4.805 5.041 98 17.4 20:14 ( 59, 80)
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Now it is 18.1 mag (Oct. 13, W. Hasubick). 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)
Nov. 3 5 29.14 7 43.2 7.268 8.010 135 17.4 2:42 (180, 47)
Nov. 10 5 24.46 7 15.8 7.201 8.016 143 17.4 2:10 (180, 48)
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It brightened up to 12 mag from spring to summer. Now it is fading. It has already faded down to 17.1 mag (Oct. 8, Toshihiko Ikemura, Hirohisa Sato).
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 22 57.91 4 45.4 1.594 2.326 126 17.4 20:08 (180, 50)
Nov. 10 23 1.17 4 49.1 1.705 2.367 120 17.7 20:14 (168, 49)
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Now it is 17.0 mag (Oct. 4, A. Diepvens). 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)
Nov. 3 22 36.97 73 11.5 7.352 7.794 113 17.4 20:05 (179,-18)
Nov. 10 22 38.30 72 16.7 7.372 7.822 113 17.5 20:14 (176,-18)
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It brightened very rapidly up to 13.8 mag in August in 2017 (Aug. 22, Kunihiro Shima). Now it is 16.9 mag (Oct. 11, D. Buczynski). In the Northern Hemisphere, it stays observable in excellent condition after this. It will be observable also in the Southern Hemisphere in December, but it stays low.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 10 21.35 28 55.2 2.575 2.501 74 17.5 3:23 (231, 3)
Nov. 10 10 32.25 29 7.4 2.519 2.528 79 17.6 3:14 (230, 4)
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Now it is 17.5 mag (Oct. 6, K. Hills). It was observed at 18 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)
Nov. 3 7 25.00 6 19.6 2.445 2.903 107 17.6 3:23 (207, 45)
Nov. 10 7 27.22 5 31.7 2.376 2.917 113 17.5 3:14 (202, 47)
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Now it is 16.6 mag (Oct. 7, Toshihiko Ikemura, Hirohisa Sato). It will be fading after this. It will be fainter than 18 mag in December.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 21 48.42 -7 19.3 1.440 1.967 106 17.5 20:05 (148, 58)
Nov. 10 21 57.83 -6 56.4 1.495 1.955 101 17.6 20:14 (137, 55)
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Now it is 18.1 mag (Oct. 15, Kunihiro Shima). Although it is around the aphelion, it is observable at 17.5 mag in November, 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)
Nov. 3 3 23.89 40 36.3 1.473 2.394 151 17.7 0:38 (180, 14)
Nov. 10 3 5.33 39 38.1 1.442 2.386 157 17.6 23:46 (180, 15)
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Peculiar asteroid moving along a cometary orbit. Now it is 17.2 mag (Sept. 9, M. Jaeger, et al.). It is observable at 17.5 mag in good condition in November. It locates somewhat low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 3 40.99 25 11.3 2.162 3.116 160 17.9 0:54 (180, 30)
Nov. 10 3 37.40 24 31.3 2.131 3.108 168 17.8 0:23 (180, 30)
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Now it is 17.9 mag (Oct. 8, W. Hasubick). 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)
Nov. 3 6 38.54 37 41.4 3.126 3.738 121 17.8 3:23 (186, 17)
Nov. 10 6 38.12 38 32.6 3.056 3.747 127 17.8 3:14 (182, 16)
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Now it is 17.9 mag (Oct. 6, D. Buczynski). It will be fainter than 18 mag in December.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 5 10.20 2 5.1 7.041 7.815 138 17.8 2:23 (180, 53)
Nov. 10 5 8.35 1 51.0 7.019 7.849 144 17.9 1:54 (180, 53)
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Now it is 17.7 mag (Oct. 1, Ken-ichi Kadota). It was observed at 16 mag from summer to autumn in 2017. It will be observable at 17 mag in good condition also in 2018. It locates somewhat low in the Southern Hemisphere.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 0 36.56 27 45.3 3.015 3.909 150 17.9 21:46 (180, 27)
Nov. 10 0 34.42 27 8.4 3.102 3.955 145 18.0 21:16 (180, 28)
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Return of a new periodic comet which brightened up to 17 mag in 2001. Now it is 19.2 mag (Oct. 12, K. Hills). It was predicted to brighten up to 17.5 mag from September to November. But actually, it is fainter than predicted by 2 mag.
Date(TT) R.A. (2000) Decl. Delta r Elong. m1 Best Time(A, h)
Nov. 3 1 35.81 -11 2.2 1.285 2.204 150 19.4 22:45 (180, 66)
Nov. 10 1 31.31 -9 49.3 1.322 2.210 145 19.5 22:13 (180, 65)
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