Visual Comets in the Future (Northern Hemisphere)

Home page	Updated on November 29, 2020
Southern Hemisphere

Please see the "Weekly Information about Bright Comets" and "Comet Catalog in order of Day of Perihelion" for more information.

Month	Evening			Midnight			Morning
	Comet	Mag	h	Comet	Mag	h	Comet	Mag	h
2020 Dec	C/2020 M3 (ATLAS)	8	43	C/2020 M3 (ATLAS)	8	89	C/2020 S3 (Erasmus)	5	3
	88P/Howell	10	26	156P/Russell- LINEAR	10	23	C/2020 M3 (ATLAS)	8	31
	156P/Russell- LINEAR	10	80	398P/2020 P2 (Boattini)	12	55	C/2019 N1 (ATLAS)	12	11
	141P/Machholz 2	11	34	29P/Schwassmann- Wachmann 1	13	59
	398P/2020 P2 (Boattini)	12	28	11P/Tempel- Swift- LINEAR	13	34
	29P/Schwassmann- Wachmann 1	13	81
	11P/Tempel- Swift- LINEAR	13	66
2021 Jan	C/2020 M3 (ATLAS)	10	77	C/2020 M3 (ATLAS)	10	79	C/2020 M3 (ATLAS)	10	14
	141P/Machholz 2	11	49	398P/2020 P2 (Boattini)	12	47	C/2019 N1 (ATLAS)	12	6
	88P/Howell	11	25	29P/Schwassmann- Wachmann 1	13	31
	398P/2020 P2 (Boattini)	12	72
	29P/Schwassmann- Wachmann 1	13	79
2021 Feb	C/2020 M3 (ATLAS)	12	77	C/2020 M3 (ATLAS)	12	53	C/2020 M3 (ATLAS)	12	4
	88P/Howell	12	19	398P/2020 P2 (Boattini)	13	47	C/2017 K2 (PanSTARRS)	13	56
	141P/Machholz 2	12	53	141P/Machholz 2	13	5
	398P/2020 P2 (Boattini)	13	78	29P/Schwassmann- Wachmann 1	13	8
	29P/Schwassmann- Wachmann 1	13	68	C/2017 K2 (PanSTARRS)	13	1
	C/2020 N1 (PanSTARRS)	13	60	C/2020 N1 (PanSTARRS)	13	1
2021 Mar	C/2020 N1 (PanSTARRS)	13	52	C/2017 K2 (PanSTARRS)	13	22	C/2020 R4 (ATLAS)	13	34
	29P/Schwassmann- Wachmann 1	13	45				C/2017 K2 (PanSTARRS)	13	71
	88P/Howell	13	9				246P/NEAT	13	24
2021 Apr	C/2020 R4 (ATLAS)	12	51	C/2020 R4 (ATLAS)	12	88	C/2020 R4 (ATLAS)	12	84
	C/2017 K2 (PanSTARRS)	13	9	7P/Pons- Winnecke	12	16	7P/Pons- Winnecke	12	60
	C/2019 L3 (ATLAS)	13	14	C/2017 K2 (PanSTARRS)	13	45	C/2017 K2 (PanSTARRS)	13	83
	29P/Schwassmann- Wachmann 1	13	18	C/2020 J1 (SONEAR)	13	20	246P/NEAT	13	27
							C/2020 J1 (SONEAR)	13	20
							C/2019 L3 (ATLAS)	13	4
2021 May	C/2017 K2 (PanSTARRS)	12	37	7P/Pons- Winnecke	11	15	7P/Pons- Winnecke	11	53
	C/2020 R4 (ATLAS)	13	86	C/2017 K2 (PanSTARRS)	12	82	C/2017 K2 (PanSTARRS)	12	83
	C/2020 J1 (SONEAR)	13	27	C/2020 R4 (ATLAS)	13	88	4P/Faye	13	16
	C/2019 L3 (ATLAS)	13	12	246P/NEAT	13	13	C/2020 R4 (ATLAS)	13	29
				C/2020 J1 (SONEAR)	13	31	15P/Finlay	13	13
							246P/NEAT	13	27
							C/2020 J1 (SONEAR)	13	15
							C/2019 L3 (ATLAS)	13	6
2021 Jun	C/2017 K2 (PanSTARRS)	12	66	7P/Pons- Winnecke	11	6	15P/Finlay	11	18
	246P/NEAT	13	5	C/2017 K2 (PanSTARRS)	12	82	7P/Pons- Winnecke	11	36
	C/2019 L3 (ATLAS)	13	2	246P/NEAT	13	24	4P/Faye	12	28
	C/2020 J1 (SONEAR)	13	37	C/2020 J1 (SONEAR)	13	26	C/2017 K2 (PanSTARRS)	12	68
							10P/Tempel 2	12	11
							8P/Tuttle	12	7
							246P/NEAT	13	26
							C/2019 L3 (ATLAS)	13	12
							29P/Schwassmann- Wachmann 1	13	9
2021 Jul	C/2017 K2 (PanSTARRS)	12	86	4P/Faye	11	1	15P/Finlay	9	26
	246P/NEAT	13	16	C/2017 K2 (PanSTARRS)	12	84	8P/Tuttle	10	4
				246P/NEAT	13	22	7P/Pons- Winnecke	11	19
				67P/Churyumov- Gerasimenko	13	14	4P/Faye	11	43
							C/2017 K2 (PanSTARRS)	12	41
							10P/Tempel 2	13	30
							C/2019 L3 (ATLAS)	13	24
							246P/NEAT	13	14
							29P/Schwassmann- Wachmann 1	13	32
							67P/Churyumov- Gerasimenko	13	53
2021 Aug	C/2017 K2 (PanSTARRS)	12	86	4P/Faye	10	9	8P/Tuttle	9	2
	6P/d'Arrest	12	51	C/2017 K2 (PanSTARRS)	12	49	15P/Finlay	9	37
	246P/NEAT	13	20	67P/Churyumov- Gerasimenko	12	27	4P/Faye	10	58
				6P/d'Arrest	12	17	7P/Pons- Winnecke	11	8
				7P/Pons- Winnecke	12	4	67P/Churyumov- Gerasimenko	12	67
				C/2019 L3 (ATLAS)	13	5	C/2017 K2 (PanSTARRS)	12	11
				29P/Schwassmann- Wachmann 1	13	14	C/2019 L3 (ATLAS)	13	41
				246P/NEAT	13	20	29P/Schwassmann- Wachmann 1	13	62
							10P/Tempel 2	13	36
2021 Sep	6P/d'Arrest	10	36	4P/Faye	10	16	4P/Faye	10	68
	C/2017 K2 (PanSTARRS)	11	68	67P/Churyumov- Gerasimenko	10	32	67P/Churyumov- Gerasimenko	10	76
				C/2017 K2 (PanSTARRS)	11	20	15P/Finlay	11	50
				C/2019 L3 (ATLAS)	12	14	C/2019 L3 (ATLAS)	12	61
				7P/Pons- Winnecke	13	5	29P/Schwassmann- Wachmann 1	13	87
				29P/Schwassmann- Wachmann 1	13	36
2021 Oct	6P/d'Arrest	9	25	67P/Churyumov- Gerasimenko	9	32	67P/Churyumov- Gerasimenko	9	81
	C/2017 K2 (PanSTARRS)	11	52	4P/Faye	10	29	4P/Faye	10	69
	19P/Borrelly	11	3	C/2019 L3 (ATLAS)	12	30	C/2019 L3 (ATLAS)	12	83
	104P/Kowal 2	13	47	104P/Kowal 2	13	19	15P/Finlay	13	57
	132P/Helin- Roman- Alu 2	13	52	29P/Schwassmann- Wachmann 1	13	61	29P/Schwassmann- Wachmann 1	13	87
				15P/Finlay	13	2	132P/Helin- Roman- Alu 2	13	9
				132P/Helin- Roman- Alu 2	13	54
2021 Nov	6P/d'Arrest	9	27	67P/Churyumov- Gerasimenko	8	36	67P/Churyumov- Gerasimenko	8	82
	19P/Borrelly	10	16	4P/Faye	10	47	4P/Faye	10	66
	C/2017 K2 (PanSTARRS)	11	35	C/2019 L3 (ATLAS)	12	52	C/2019 L3 (ATLAS)	12	87
	104P/Kowal 2	11	45	104P/Kowal 2	12	7	29P/Schwassmann- Wachmann 1	13	87
	29P/Schwassmann- Wachmann 1	13	20	29P/Schwassmann- Wachmann 1	13	87
	132P/Helin- Roman- Alu 2	13	52	132P/Helin- Roman- Alu 2	13	40
2021 Dec	19P/Borrelly	9	34	67P/Churyumov- Gerasimenko	8	57	67P/Churyumov- Gerasimenko	8	83
	6P/d'Arrest	10	33	4P/Faye	10	63	4P/Faye	10	63
	104P/Kowal 2	10	47	C/2019 L3 (ATLAS)	11	90	C/2017 K2 (PanSTARRS)	11	10
	C/2017 K2 (PanSTARRS)	11	15	29P/Schwassmann- Wachmann 1	13	87	C/2019 L3 (ATLAS)	11	89
	4P/Faye	11	9				22P/Kopff	12	5
	C/2019 L3 (ATLAS)	11	15				29P/Schwassmann- Wachmann 1	13	24
	29P/Schwassmann- Wachmann 1	13	86				9P/Tempel 1	13	22
							C/2019 T4 (ATLAS)	13	26
2022 Jan	19P/Borrelly	8	47	67P/Churyumov- Gerasimenko	9	84	67P/Churyumov- Gerasimenko	9	84
	67P/Churyumov- Gerasimenko	9	28	4P/Faye	11	64	C/2017 K2 (PanSTARRS)	10	29
	104P/Kowal 2	10	55	C/2019 L3 (ATLAS)	11	88	22P/Kopff	11	8
	4P/Faye	11	65	29P/Schwassmann- Wachmann 1	13	61	4P/Faye	11	7
	C/2019 L3 (ATLAS)	11	49	C/2019 T4 (ATLAS)	13	9	C/2019 L3 (ATLAS)	11	28
	6P/d'Arrest	12	34				9P/Tempel 1	12	22
	29P/Schwassmann- Wachmann 1	13	86				C/2019 T4 (ATLAS)	13	25
2022 Feb	19P/Borrelly	8	48	67P/Churyumov- Gerasimenko	10	84	C/2017 K2 (PanSTARRS)	10	42
	67P/Churyumov- Gerasimenko	10	82	104P/Kowal 2	10	10	67P/Churyumov- Gerasimenko	10	17
	104P/Kowal 2	10	63	C/2019 L3 (ATLAS)	11	61	22P/Kopff	11	8
	C/2019 L3 (ATLAS)	11	81	C/2019 T4 (ATLAS)	13	28	9P/Tempel 1	12	21
	4P/Faye	13	67	4P/Faye	13	48	C/2019 T4 (ATLAS)	13	27
	29P/Schwassmann- Wachmann 1	13	85	29P/Schwassmann- Wachmann 1	13	33	116P/Wild 4	13	18
	116P/Wild 4	13	37	116P/Wild 4	13	74	A/2019 U5	13	77
				A/2019 U5	13	17
2022 Mar	19P/Borrelly	9	47	C/2017 K2 (PanSTARRS)	9	1	C/2017 K2 (PanSTARRS)	9	54
	104P/Kowal 2	12	65	104P/Kowal 2	12	15	22P/Kopff	10	8
	C/2019 L3 (ATLAS)	12	76	C/2019 L3 (ATLAS)	12	36	9P/Tempel 1	11	18
	67P/Churyumov- Gerasimenko	12	82	67P/Churyumov- Gerasimenko	12	60	67P/Churyumov- Gerasimenko	12	1
	C/2019 T4 (ATLAS)	12	12	C/2019 T4 (ATLAS)	12	33	C/2019 T4 (ATLAS)	13	9
	A/2019 U5	13	2	A/2019 U5	13	44	A/2019 U5	13	86
	116P/Wild 4	13	74	116P/Wild 4	13	74	116P/Wild 4	13	10
	29P/Schwassmann- Wachmann 1	13	68	29P/Schwassmann- Wachmann 1	13	13
2022 Apr	19P/Borrelly	10	42	C/2017 K2 (PanSTARRS)	8	25	C/2017 K2 (PanSTARRS)	8	64
	C/2019 L3 (ATLAS)	12	61	19P/Borrelly	11	3	22P/Kopff	10	10
	C/2019 T4 (ATLAS)	12	40	C/2019 L3 (ATLAS)	12	11	9P/Tempel 1	11	15
	A/2019 U5	13	35	C/2019 T4 (ATLAS)	12	37	A/2019 U5	13	84
	116P/Wild 4	13	74	A/2019 U5	13	82	117P/Helin- Roman- Alu 1	13	26
	29P/Schwassmann- Wachmann 1	13	42	116P/Wild 4	13	45
	67P/Churyumov- Gerasimenko	13	78	67P/Churyumov- Gerasimenko	13	39
2022 May	C/2017 K2 (PanSTARRS)	7	18	C/2017 K2 (PanSTARRS)	7	65	C/2017 K2 (PanSTARRS)	7	66
	45P/Honda- Mrkos- Pajdusakova	10	7	19P/Borrelly	12	3	22P/Kopff	11	18
	19P/Borrelly	12	37	A/2019 U5	12	83	9P/Tempel 1	12	20
	A/2019 U5	12	83	C/2019 T4 (ATLAS)	13	26	A/2019 U5	12	57
	C/2019 L3 (ATLAS)	12	34	117P/Helin- Roman- Alu 1	13	16	117P/Helin- Roman- Alu 1	13	26
	C/2019 T4 (ATLAS)	13	43	73P/Schwassmann- Wachmann 3	13	16
	73P/Schwassmann- Wachmann 3	13	56	116P/Wild 4	13	23
	116P/Wild 4	13	65
2022 Jun	C/2017 K2 (PanSTARRS)	6	48	C/2017 K2 (PanSTARRS)	6	64	C/2017 K2 (PanSTARRS)	6	57
	73P/Schwassmann- Wachmann 3	12	43	A/2019 U5	12	62	22P/Kopff	11	32
	45P/Honda- Mrkos- Pajdusakova	12	8	73P/Schwassmann- Wachmann 3	12	6	169P/NEAT	12	12
	A/2019 U5	12	84	C/2019 T4 (ATLAS)	13	8	A/2019 U5	12	28
	C/2019 T4 (ATLAS)	13	39	117P/Helin- Roman- Alu 1	13	25	9P/Tempel 1	12	29
	117P/Helin- Roman- Alu 1	13	9	9P/Tempel 1	13	3	117P/Helin- Roman- Alu 1	13	25
	C/2019 L3 (ATLAS)	13	4	19P/Borrelly	13	1
	19P/Borrelly	13	29	116P/Wild 4	13	2
	116P/Wild 4	13	39
2022 Jul	C/2017 K2 (PanSTARRS)	6	54	C/2017 K2 (PanSTARRS)	6	56	C/2017 K2 (PanSTARRS)	6	20
	73P/Schwassmann- Wachmann 3	11	23	22P/Kopff	12	14	169P/NEAT	12	2
	C/2020 R7 (ATLAS)	12	1	A/2019 U5	12	31	22P/Kopff	12	52
	A/2019 U5	12	65	117P/Helin- Roman- Alu 1	13	23	117P/Helin- Roman- Alu 1	13	11
	117P/Helin- Roman- Alu 1	13	23	9P/Tempel 1	13	14	9P/Tempel 1	13	32
	C/2019 T4 (ATLAS)	13	24
2022 Aug	C/2017 K2 (PanSTARRS)	6	42	C/2017 K2 (PanSTARRS)	6	14	22P/Kopff	12	59
	73P/Schwassmann- Wachmann 3	11	12	A/2019 U5	12	3	81P/Wild 2	13	4
	C/2020 R7 (ATLAS)	12	11	22P/Kopff	12	35	29P/Schwassmann- Wachmann 1	13	38
	A/2019 U5	12	40	117P/Helin- Roman- Alu 1	13	16
	117P/Helin- Roman- Alu 1	13	23
	C/2019 T4 (ATLAS)	13	12
2022 Sep	C/2017 K2 (PanSTARRS)	6	21	118P/Shoemaker- Levy 4	13	2	81P/Wild 2	12	14
	73P/Schwassmann- Wachmann 3	11	9	22P/Kopff	13	57	118P/Shoemaker- Levy 4	13	55
	A/2019 U5	12	22	117P/Helin- Roman- Alu 1	13	1	22P/Kopff	13	58
	C/2020 R7 (ATLAS)	12	13	29P/Schwassmann- Wachmann 1	13	11	29P/Schwassmann- Wachmann 1	13	64
	117P/Helin- Roman- Alu 1	13	23				C/2019 L3 (ATLAS)	13	6
	C/2019 T4 (ATLAS)	13	3
	22P/Kopff	13	2
2022 Oct	C/2017 K2 (PanSTARRS)	6	3	118P/Shoemaker- Levy 4	12	14	81P/Wild 2	11	24
	73P/Schwassmann- Wachmann 3	12	18	29P/Schwassmann- Wachmann 1	13	35	118P/Shoemaker- Levy 4	12	64
	A/2019 U5	12	6				A/2019 U5	12	4
	C/2020 R7 (ATLAS)	12	13				29P/Schwassmann- Wachmann 1	13	84
2022 Nov	C/2020 R7 (ATLAS)	13	6	118P/Shoemaker- Levy 4	11	29	118P/Shoemaker- Levy 4	11	64
	73P/Schwassmann- Wachmann 3	13	19	29P/Schwassmann- Wachmann 1	13	60	81P/Wild 2	11	30
	C/2020 K1 (PanSTARRS)	13	16				A/2019 U5	11	29
							29P/Schwassmann- Wachmann 1	13	84
2022 Dec	29P/Schwassmann- Wachmann 1	13	21	118P/Shoemaker- Levy 4	11	49	118P/Shoemaker- Levy 4	11	63
				29P/Schwassmann- Wachmann 1	13	84	A/2019 U5	11	51
							81P/Wild 2	11	33
							29P/Schwassmann- Wachmann 1	13	84
2023 Jan	118P/Shoemaker- Levy 4	11	18	A/2019 U5	11	11	A/2019 U5	11	57
	29P/Schwassmann- Wachmann 1	13	84	118P/Shoemaker- Levy 4	11	68	118P/Shoemaker- Levy 4	11	64
				29P/Schwassmann- Wachmann 1	13	84	81P/Wild 2	11	33
							29P/Schwassmann- Wachmann 1	13	19
							C/2020 R7 (ATLAS)	13	21
2023 Feb	118P/Shoemaker- Levy 4	12	74	A/2019 U5	10	40	96P/Machholz 1	8	13
	29P/Schwassmann- Wachmann 1	13	84	118P/Shoemaker- Levy 4	12	73	A/2019 U5	10	56
				29P/Schwassmann- Wachmann 1	13	60	81P/Wild 2	11	33
							118P/Shoemaker- Levy 4	12	11
							C/2020 K1 (PanSTARRS)	13	1
							237P/LINEAR	13	23
							C/2020 R7 (ATLAS)	13	41
2023 Mar	A/2019 U5	10	27	A/2019 U5	10	54	A/2019 U5	10	54
	29P/Schwassmann- Wachmann 1	13	83	364P/PanSTARRS	13	45	81P/Wild 2	12	35
	118P/Shoemaker- Levy 4	13	74	C/2020 R7 (ATLAS)	13	11	237P/LINEAR	12	27
				29P/Schwassmann- Wachmann 1	13	35	C/2020 K1 (PanSTARRS)	12	1
				118P/Shoemaker- Levy 4	13	56	96P/Machholz 1	13	16
							364P/PanSTARRS	13	87
							C/2020 R7 (ATLAS)	13	61
2023 Apr	A/2019 U5	10	53	A/2019 U5	10	53	A/2019 U5	10	9
	C/2020 R7 (ATLAS)	13	2	237P/LINEAR	11	1	237P/LINEAR	11	35
	29P/Schwassmann- Wachmann 1	13	62	364P/PanSTARRS	11	31	364P/PanSTARRS	11	84
				81P/Wild 2	12	17	81P/Wild 2	12	37
				C/2020 R7 (ATLAS)	13	46	C/2020 R7 (ATLAS)	13	77
				29P/Schwassmann- Wachmann 1	13	13	71P/Clark	13	1
2023 May	A/2019 U5	10	52	A/2019 U5	10	26	237P/LINEAR	10	46
	81P/Wild 2	12	9	237P/LINEAR	10	23	81P/Wild 2	12	37
	C/2020 R7 (ATLAS)	13	46	81P/Wild 2	12	37	C/2020 R7 (ATLAS)	13	81
				C/2020 R7 (ATLAS)	13	85	71P/Clark	13	6
2023 Jun	237P/LINEAR	10	18	237P/LINEAR	10	53	237P/LINEAR	10	52
	A/2019 U5	11	31	81P/Wild 2	13	37	185P/Petriew	11	13
	81P/Wild 2	13	32	C/2020 R7 (ATLAS)	13	87	364P/PanSTARRS	13	4
	C/2020 R7 (ATLAS)	13	54				81P/Wild 2	13	29
							C/2020 R7 (ATLAS)	13	53
2023 Jul	237P/LINEAR	10	43	237P/LINEAR	10	56	237P/LINEAR	10	46
	A/2019 U5	11	4	103P/Hartley 2	12	44	185P/Petriew	11	10
	103P/Hartley 2	12	7	126P/IRAS	13	15	103P/Hartley 2	12	84
	81P/Wild 2	13	34	81P/Wild 2	13	36	126P/IRAS	13	57
							81P/Wild 2	13	6
2023 Aug	103P/Hartley 2	9	8	103P/Hartley 2	9	47	C/2017 K2 (PanSTARRS)	9	16
	237P/LINEAR	11	56	237P/LINEAR	11	56	103P/Hartley 2	9	90
	126P/IRAS	13	5	2P/Encke	11	5	237P/LINEAR	11	16
	12P/Pons- Brooks	13	70	126P/IRAS	13	41	185P/Petriew	11	11
				12P/Pons- Brooks	13	40	2P/Encke	11	49
							126P/IRAS	13	81
							12P/Pons- Brooks	13	9
2023 Sep	103P/Hartley 2	9	4	103P/Hartley 2	7	42	103P/Hartley 2	7	82
	237P/LINEAR	12	54	2P/Encke	10	2	2P/Encke	8	47
	12P/Pons- Brooks	13	68	237P/LINEAR	12	33	C/2017 K2 (PanSTARRS)	9	39
	126P/IRAS	13	21	12P/Pons- Brooks	13	33	185P/Petriew	13	13
				126P/IRAS	13	55	12P/Pons- Brooks	13	3
							126P/IRAS	13	79
2023 Oct	12P/Pons- Brooks	12	60	103P/Hartley 2	7	17	103P/Hartley 2	7	72
	237P/LINEAR	13	53	C/2017 K2 (PanSTARRS)	9	16	2P/Encke	7	19
				62P/Tsuchinshan 1	12	22	C/2017 K2 (PanSTARRS)	9	47
				12P/Pons- Brooks	12	13	62P/Tsuchinshan 1	12	76
				237P/LINEAR	13	13	A/2019 U5	12	11
				29P/Schwassmann- Wachmann 1	13	9	29P/Schwassmann- Wachmann 1	13	67
2023 Nov	12P/Pons- Brooks	11	49	103P/Hartley 2	7	11	103P/Hartley 2	7	58
	144P/Kushida	13	33	62P/Tsuchinshan 1	8	22	62P/Tsuchinshan 1	8	76
				C/2017 K2 (PanSTARRS)	9	48	C/2017 K2 (PanSTARRS)	9	48
				144P/Kushida	13	73	A/2019 U5	12	19
				29P/Schwassmann- Wachmann 1	13	32	144P/Kushida	13	9
							29P/Schwassmann- Wachmann 1	13	75
2023 Dec	12P/Pons- Brooks	10	37	62P/Tsuchinshan 1	7	21	62P/Tsuchinshan 1	7	73
	C/2017 K2 (PanSTARRS)	10	16	103P/Hartley 2	8	31	103P/Hartley 2	8	46
	144P/Kushida	10	71	C/2017 K2 (PanSTARRS)	10	52	12P/Pons- Brooks	10	7
	13P/Olbers	13	40	144P/Kushida	10	72	C/2017 K2 (PanSTARRS)	10	23
	P/2016 J3 (STEREO)	13	27	13P/Olbers	13	35	A/2019 U5	12	19
				29P/Schwassmann- Wachmann 1	13	60	26P/Grigg- Skjellerup	13	9
							29P/Schwassmann- Wachmann 1	13	76
2024 Jan	12P/Pons- Brooks	8	25	62P/Tsuchinshan 1	7	30	62P/Tsuchinshan 1	7	68
	144P/Kushida	8	71	144P/Kushida	8	37	12P/Pons- Brooks	8	10
	C/2017 K2 (PanSTARRS)	10	56	103P/Hartley 2	10	44	103P/Hartley 2	10	18
	P/2016 J3 (STEREO)	10	23	C/2017 K2 (PanSTARRS)	10	54	A/2019 U5	12	13
	103P/Hartley 2	11	9	13P/Olbers	12	17	26P/Grigg- Skjellerup	12	11
	13P/Olbers	12	48	A/2019 U5	12	10	29P/Schwassmann- Wachmann 1	13	38
	29P/Schwassmann- Wachmann 1	13	25	29P/Schwassmann- Wachmann 1	13	76
	207P/NEAT	13	35
2024 Feb	12P/Pons- Brooks	6	18	62P/Tsuchinshan 1	7	52	12P/Pons- Brooks	6	9
	144P/Kushida	8	72	144P/Kushida	8	27	62P/Tsuchinshan 1	7	65
	C/2017 K2 (PanSTARRS)	11	60	C/2017 K2 (PanSTARRS)	11	31	29P/Schwassmann- Wachmann 1	13	12
	13P/Olbers	11	48	103P/Hartley 2	12	50
	103P/Hartley 2	12	33	A/2019 U5	12	10
	P/2001 Q6 (NEAT)	12	31	207P/NEAT	12	1
	207P/NEAT	12	39	29P/Schwassmann- Wachmann 1	13	76
	A/2019 U5	13	11
	29P/Schwassmann- Wachmann 1	13	76
2024 Mar	12P/Pons- Brooks	4	17	144P/Kushida	9	22	62P/Tsuchinshan 1	9	40
	144P/Kushida	9	72	62P/Tsuchinshan 1	9	65	P/2001 Q6 (NEAT)	13	4
	62P/Tsuchinshan 1	9	31	C/2017 K2 (PanSTARRS)	11	8
	13P/Olbers	10	39	207P/NEAT	12	29
	C/2017 K2 (PanSTARRS)	11	58	A/2019 U5	13	3
	P/2001 Q6 (NEAT)	12	21	29P/Schwassmann- Wachmann 1	13	54
	207P/NEAT	12	51
	A/2019 U5	13	14
	29P/Schwassmann- Wachmann 1	13	76
2024 Apr	12P/Pons- Brooks	4	9	144P/Kushida	11	16	62P/Tsuchinshan 1	11	20
	13P/Olbers	9	23	62P/Tsuchinshan 1	11	64	P/2001 Q6 (NEAT)	13	8
	144P/Kushida	11	65	P/2001 Q6 (NEAT)	13	1
	62P/Tsuchinshan 1	11	62	29P/Schwassmann- Wachmann 1	13	29
	C/2017 K2 (PanSTARRS)	12	38
	P/2001 Q6 (NEAT)	13	20
	A/2019 U5	13	14
	29P/Schwassmann- Wachmann 1	13	75
2024 May	13P/Olbers	8	11	144P/Kushida	13	7	154P/Brewington	11	4
	C/2017 K2 (PanSTARRS)	12	11	29P/Schwassmann- Wachmann 1	13	6
	144P/Kushida	13	51
	29P/Schwassmann- Wachmann 1	13	50
2024 Jun	13P/Olbers	7	11				154P/Brewington	11	13
2024 Jul	13P/Olbers	7	19				154P/Brewington	11	24
							C/2017 K2 (PanSTARRS)	13	8
2024 Aug	13P/Olbers	8	20				154P/Brewington	12	32
							C/2017 K2 (PanSTARRS)	13	37
2024 Sep	13P/Olbers	9	19	C/2017 K2 (PanSTARRS)	13	11	C/2017 K2 (PanSTARRS)	13	64
	37P/Forbes	13	11
2024 Oct	13P/Olbers	10	13	C/2017 K2 (PanSTARRS)	13	37	333P/LINEAR	13	33
	37P/Forbes	13	13				C/2017 K2 (PanSTARRS)	13	74
2024 Nov	13P/Olbers	12	3	333P/LINEAR	10	2	333P/LINEAR	10	62
				C/2017 K2 (PanSTARRS)	13	75	C/2017 K2 (PanSTARRS)	13	75
				29P/Schwassmann- Wachmann 1	13	8	29P/Schwassmann- Wachmann 1	13	63
2024 Dec	333P/LINEAR	9	47	333P/LINEAR	9	12	333P/LINEAR	9	62
	C/2017 K2 (PanSTARRS)	13	29	C/2017 K2 (PanSTARRS)	13	76	C/2017 K2 (PanSTARRS)	13	37
				29P/Schwassmann- Wachmann 1	13	34	29P/Schwassmann- Wachmann 1	13	64
2025 Jan	333P/LINEAR	12	46	29P/Schwassmann- Wachmann 1	13	64	29P/Schwassmann- Wachmann 1	13	64
2025 Feb	29P/Schwassmann- Wachmann 1	13	28	29P/Schwassmann- Wachmann 1	13	65	29P/Schwassmann- Wachmann 1	13	26
2025 Mar	29P/Schwassmann- Wachmann 1	13	66	29P/Schwassmann- Wachmann 1	13	65	29P/Schwassmann- Wachmann 1	13	7
2025 Apr	29P/Schwassmann- Wachmann 1	13	66	29P/Schwassmann- Wachmann 1	13	41
2025 May	29P/Schwassmann- Wachmann 1	13	58	29P/Schwassmann- Wachmann 1	13	17
2025 Jun
2025 Jul							217P/LINEAR	13	2
2025 Aug
2025 Sep	210P/Christensen	13	11
2025 Oct	210P/Christensen	11	10	24P/Schaumasse	13	17	24P/Schaumasse	13	73
2025 Nov				24P/Schaumasse	10	18	210P/Christensen	8	10
							24P/Schaumasse	10	74

The h means the highest altitude in that month at lat. 35 deg in the Northern Hemisphere.