Visual Comets in the Future (Northern Hemisphere)

Home page	Updated on August 10, 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 Aug	C/2020 F3 (NEOWISE)	5	30	C/2020 K8 (Catalina- ATLAS)	12	14	C/2020 K8 (Catalina- ATLAS)	11	56
	88P/Howell	9	21	29P/Schwassmann- Wachmann 1	13	35	58P/Jackson- Neujmin	12	36
	C/2019 U6 (Lemmon)	9	44				29P/Schwassmann- Wachmann 1	13	82
	C/2017 T2 (PanSTARRS)	10	37
	2P/Encke	10	12
	C/2019 N1 (ATLAS)	13	30
2020 Sep	88P/Howell	8	15	29P/Schwassmann- Wachmann 1	13	60	C/2020 K8 (Catalina- ATLAS)	10	8
	C/2020 F3 (NEOWISE)	10	19				29P/Schwassmann- Wachmann 1	13	83
	C/2017 T2 (PanSTARRS)	11	20
	C/2019 U6 (Lemmon)	12	45
	C/2019 N1 (ATLAS)	13	11
	29P/Schwassmann- Wachmann 1	13	4
2020 Oct	88P/Howell	8	19	29P/Schwassmann- Wachmann 1	13	83	C/2020 P1 (NEOWISE)	9	5
	C/2017 T2 (PanSTARRS)	11	8	C/2020 M3 (ATLAS)	13	28	29P/Schwassmann- Wachmann 1	13	83
	C/2020 F3 (NEOWISE)	12	7				C/2020 M3 (ATLAS)	13	41
	29P/Schwassmann- Wachmann 1	13	21
2020 Nov	88P/Howell	9	24	P/2009 Q4 (Boattini)	12	42	C/2020 P1 (NEOWISE)	11	11
	141P/Machholz 2	13	29	29P/Schwassmann- Wachmann 1	13	82	C/2019 N1 (ATLAS)	12	10
	29P/Schwassmann- Wachmann 1	13	81	C/2020 M3 (ATLAS)	13	78	P/2009 Q4 (Boattini)	12	14
	C/2020 M3 (ATLAS)	13	6				29P/Schwassmann- Wachmann 1	13	25
							C/2020 M3 (ATLAS)	13	55
2020 Dec	88P/Howell	10	26	P/2009 Q4 (Boattini)	12	53	C/2019 N1 (ATLAS)	12	11
	141P/Machholz 2	11	34	29P/Schwassmann- Wachmann 1	13	58	C/2020 M3 (ATLAS)	13	30
	P/2009 Q4 (Boattini)	12	27	C/2020 M3 (ATLAS)	13	81
	29P/Schwassmann- Wachmann 1	13	81
	C/2020 M3 (ATLAS)	13	11
2021 Jan	141P/Machholz 2	11	50	P/2009 Q4 (Boattini)	12	47	C/2019 N1 (ATLAS)	12	7
	88P/Howell	11	26	29P/Schwassmann- Wachmann 1	13	32	C/2017 T2 (PanSTARRS)	13	11
	P/2009 Q4 (Boattini)	12	72
	29P/Schwassmann- Wachmann 1	13	79
2021 Feb	88P/Howell	12	19	141P/Machholz 2	13	5	C/2017 K2 (PanSTARRS)	13	56
	141P/Machholz 2	13	53	29P/Schwassmann- Wachmann 1	13	8	C/2017 T2 (PanSTARRS)	13	13
	29P/Schwassmann- Wachmann 1	13	68	P/2009 Q4 (Boattini)	13	46
	P/2009 Q4 (Boattini)	13	75	C/2017 K2 (PanSTARRS)	13	1
	C/2020 N1 (PanSTARRS)	13	60	C/2020 N1 (PanSTARRS)	13	2
2021 Mar	C/2020 N1 (PanSTARRS)	13	52	C/2017 K2 (PanSTARRS)	13	21	C/2017 K2 (PanSTARRS)	13	70
	29P/Schwassmann- Wachmann 1	13	44				246P/NEAT	13	24
	88P/Howell	13	8
2021 Apr	C/2017 K2 (PanSTARRS)	13	7	7P/Pons- Winnecke	13	16	7P/Pons- Winnecke	13	60
	29P/Schwassmann- Wachmann 1	13	20	C/2017 K2 (PanSTARRS)	13	43	C/2017 K2 (PanSTARRS)	13	82
				C/2020 J1 (SONEAR)	13	20	246P/NEAT	13	26
							C/2020 J1 (SONEAR)	13	19
2021 May	C/2017 K2 (PanSTARRS)	12	38	7P/Pons- Winnecke	11	15	7P/Pons- Winnecke	11	54
	C/2020 J1 (SONEAR)	13	28	C/2017 K2 (PanSTARRS)	12	82	C/2017 K2 (PanSTARRS)	12	83
	C/2019 L3 (ATLAS)	13	13	246P/NEAT	13	14	4P/Faye	13	16
				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	67	7P/Pons- Winnecke	11	6	15P/Finlay	11	18
	246P/NEAT	13	6	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	25	C/2017 K2 (PanSTARRS)	12	67
							10P/Tempel 2	12	12
							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	27
	246P/NEAT	13	16	C/2017 K2 (PanSTARRS)	12	84	8P/Tuttle	10	4
				246P/NEAT	13	22	4P/Faye	11	43
				67P/Churyumov- Gerasimenko	13	15	7P/Pons- Winnecke	11	19
							C/2017 K2 (PanSTARRS)	12	40
							10P/Tempel 2	13	30
							C/2019 L3 (ATLAS)	13	24
							246P/NEAT	13	13
							29P/Schwassmann- Wachmann 1	13	33
							67P/Churyumov- Gerasimenko	13	53
2021 Aug	C/2017 K2 (PanSTARRS)	12	85	4P/Faye	10	8	8P/Tuttle	9	2
	6P/d'Arrest	12	50	C/2017 K2 (PanSTARRS)	12	48	15P/Finlay	9	36
	246P/NEAT	13	17	67P/Churyumov- Gerasimenko	12	26	4P/Faye	10	57
				6P/d'Arrest	12	16	7P/Pons- Winnecke	11	8
				7P/Pons- Winnecke	12	3	C/2017 K2 (PanSTARRS)	12	10
				C/2019 L3 (ATLAS)	13	4	67P/Churyumov- Gerasimenko	12	67
				29P/Schwassmann- Wachmann 1	13	13	C/2019 L3 (ATLAS)	13	40
				246P/NEAT	13	20	29P/Schwassmann- Wachmann 1	13	60
							10P/Tempel 2	13	35
2021 Sep	6P/d'Arrest	10	37	4P/Faye	10	16	4P/Faye	10	67
	C/2017 K2 (PanSTARRS)	11	69	67P/Churyumov- Gerasimenko	10	32	67P/Churyumov- Gerasimenko	10	76
				C/2017 K2 (PanSTARRS)	11	21	15P/Finlay	11	49
				C/2019 L3 (ATLAS)	12	14	C/2019 L3 (ATLAS)	12	59
				7P/Pons- Winnecke	13	5	29P/Schwassmann- Wachmann 1	13	87
				29P/Schwassmann- Wachmann 1	13	34
2021 Oct	6P/d'Arrest	9	26	67P/Churyumov- Gerasimenko	9	32	67P/Churyumov- Gerasimenko	9	81
	C/2017 K2 (PanSTARRS)	11	53	4P/Faye	10	29	4P/Faye	10	69
	19P/Borrelly	11	3	C/2019 L3 (ATLAS)	12	30	C/2019 L3 (ATLAS)	12	84
	104P/Kowal 2	13	47	104P/Kowal 2	13	18	15P/Finlay	13	56
	29P/Schwassmann- Wachmann 1	13	1	29P/Schwassmann- Wachmann 1	13	61	29P/Schwassmann- Wachmann 1	13	87
	132P/Helin- Roman- Alu 2	13	52	15P/Finlay	13	1	132P/Helin- Roman- Alu 2	13	12
				132P/Helin- Roman- Alu 2	13	54
2021 Nov	6P/d'Arrest	9	27	67P/Churyumov- Gerasimenko	8	37	67P/Churyumov- Gerasimenko	8	82
	19P/Borrelly	10	17	4P/Faye	10	48	4P/Faye	10	66
	C/2017 K2 (PanSTARRS)	11	34	C/2019 L3 (ATLAS)	12	53	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	21	29P/Schwassmann- Wachmann 1	13	87
	132P/Helin- Roman- Alu 2	13	52	132P/Helin- Roman- Alu 2	13	39
2021 Dec	19P/Borrelly	9	35	67P/Churyumov- Gerasimenko	8	58	67P/Churyumov- Gerasimenko	8	83
	6P/d'Arrest	10	33	4P/Faye	10	62	4P/Faye	10	63
	104P/Kowal 2	10	47	C/2019 L3 (ATLAS)	11	90	C/2017 K2 (PanSTARRS)	11	11
	C/2017 K2 (PanSTARRS)	11	15	29P/Schwassmann- Wachmann 1	13	87	C/2019 L3 (ATLAS)	11	89
	4P/Faye	11	10				22P/Kopff	12	5
	C/2019 L3 (ATLAS)	11	16				29P/Schwassmann- Wachmann 1	13	23
	29P/Schwassmann- Wachmann 1	13	86				9P/Tempel 1	13	22
							C/2019 T4 (ATLAS)	13	26
2022 Jan	19P/Borrelly	8	46	67P/Churyumov- Gerasimenko	9	84	67P/Churyumov- Gerasimenko	9	84
	67P/Churyumov- Gerasimenko	9	26	C/2019 L3 (ATLAS)	11	88	C/2017 K2 (PanSTARRS)	10	28
	104P/Kowal 2	10	54	4P/Faye	11	64	22P/Kopff	11	8
	C/2019 L3 (ATLAS)	11	47	29P/Schwassmann- Wachmann 1	13	60	C/2019 L3 (ATLAS)	11	27
	4P/Faye	11	65	C/2019 T4 (ATLAS)	13	7	4P/Faye	11	6
	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	11	67P/Churyumov- Gerasimenko	10	19
	104P/Kowal 2	10	63	C/2019 L3 (ATLAS)	11	63	22P/Kopff	11	8
	C/2019 L3 (ATLAS)	11	82	4P/Faye	13	49	9P/Tempel 1	12	21
	4P/Faye	13	67	C/2019 T4 (ATLAS)	13	28	C/2019 T4 (ATLAS)	13	27
	29P/Schwassmann- Wachmann 1	13	85	29P/Schwassmann- Wachmann 1	13	35	116P/Wild 4	13	20
	116P/Wild 4	13	38	116P/Wild 4	13	74
2022 Mar	19P/Borrelly	9	46	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	35	9P/Tempel 1	11	18
	67P/Churyumov- Gerasimenko	12	81	67P/Churyumov- Gerasimenko	12	60	C/2019 T4 (ATLAS)	13	9
	C/2019 T4 (ATLAS)	12	13	C/2019 T4 (ATLAS)	12	33	116P/Wild 4	13	9
	116P/Wild 4	13	74	116P/Wild 4	13	74
	29P/Schwassmann- Wachmann 1	13	68	29P/Schwassmann- Wachmann 1	13	13
2022 Apr	19P/Borrelly	10	42	C/2017 K2 (PanSTARRS)	8	26	C/2017 K2 (PanSTARRS)	8	64
	C/2019 L3 (ATLAS)	12	60	19P/Borrelly	11	3	22P/Kopff	10	10
	C/2019 T4 (ATLAS)	12	40	C/2019 L3 (ATLAS)	12	10	9P/Tempel 1	11	15
	116P/Wild 4	13	74	C/2019 T4 (ATLAS)	12	37	117P/Helin- Roman- Alu 1	13	26
	29P/Schwassmann- Wachmann 1	13	41	116P/Wild 4	13	44
	67P/Churyumov- Gerasimenko	13	78	67P/Churyumov- Gerasimenko	13	38
2022 May	C/2017 K2 (PanSTARRS)	7	16	C/2017 K2 (PanSTARRS)	7	52	C/2017 K2 (PanSTARRS)	7	66
	45P/Honda- Mrkos- Pajdusakova	10	6	19P/Borrelly	12	3	22P/Kopff	11	17
	19P/Borrelly	12	37	C/2019 T4 (ATLAS)	13	26	9P/Tempel 1	12	20
	C/2019 L3 (ATLAS)	12	33	117P/Helin- Roman- Alu 1	13	15	117P/Helin- Roman- Alu 1	13	26
	C/2019 T4 (ATLAS)	13	43	73P/Schwassmann- Wachmann 3	13	15
	73P/Schwassmann- Wachmann 3	13	55	116P/Wild 4	13	22
	116P/Wild 4	13	64
2022 Jun	C/2017 K2 (PanSTARRS)	6	47	C/2017 K2 (PanSTARRS)	6	65	C/2017 K2 (PanSTARRS)	6	59
	45P/Honda- Mrkos- Pajdusakova	12	7	73P/Schwassmann- Wachmann 3	13	8	22P/Kopff	11	31
	73P/Schwassmann- Wachmann 3	12	44	C/2019 T4 (ATLAS)	13	10	169P/NEAT	12	11
	C/2019 T4 (ATLAS)	13	40	117P/Helin- Roman- Alu 1	13	25	9P/Tempel 1	12	29
	117P/Helin- Roman- Alu 1	13	8	19P/Borrelly	13	1	117P/Helin- Roman- Alu 1	13	25
	C/2019 L3 (ATLAS)	13	6	9P/Tempel 1	13	2
	19P/Borrelly	13	29	116P/Wild 4	13	3
	116P/Wild 4	13	41
2022 Jul	C/2017 K2 (PanSTARRS)	6	53	C/2017 K2 (PanSTARRS)	6	57	C/2017 K2 (PanSTARRS)	6	23
	73P/Schwassmann- Wachmann 3	11	24	22P/Kopff	12	14	169P/NEAT	12	3
	117P/Helin- Roman- Alu 1	13	23	117P/Helin- Roman- Alu 1	13	23	22P/Kopff	12	53
	C/2019 T4 (ATLAS)	13	25	9P/Tempel 1	13	15	117P/Helin- Roman- Alu 1	13	13
							9P/Tempel 1	13	32
2022 Aug	C/2017 K2 (PanSTARRS)	6	41	C/2017 K2 (PanSTARRS)	6	13	22P/Kopff	12	59
	73P/Schwassmann- Wachmann 3	11	12	22P/Kopff	12	36	81P/Wild 2	13	4
	117P/Helin- Roman- Alu 1	13	23	117P/Helin- Roman- Alu 1	13	15	29P/Schwassmann- Wachmann 1	13	38
	C/2019 T4 (ATLAS)	13	11
2022 Sep	C/2017 K2 (PanSTARRS)	6	20	118P/Shoemaker- Levy 4	13	2	81P/Wild 2	12	15
	73P/Schwassmann- Wachmann 3	11	9	22P/Kopff	13	57	118P/Shoemaker- Levy 4	13	56
	117P/Helin- Roman- Alu 1	13	23	29P/Schwassmann- Wachmann 1	13	11	22P/Kopff	13	58
	22P/Kopff	13	3				29P/Schwassmann- Wachmann 1	13	65
	C/2019 T4 (ATLAS)	13	3				C/2019 L3 (ATLAS)	13	7
2022 Oct	C/2017 K2 (PanSTARRS)	6	3	118P/Shoemaker- Levy 4	12	13	81P/Wild 2	11	23
	73P/Schwassmann- Wachmann 3	12	18	29P/Schwassmann- Wachmann 1	13	33	118P/Shoemaker- Levy 4	12	64
							29P/Schwassmann- Wachmann 1	13	84
2022 Nov	73P/Schwassmann- Wachmann 3	13	20	118P/Shoemaker- Levy 4	11	28	81P/Wild 2	11	29
	C/2020 K1 (PanSTARRS)	13	14	29P/Schwassmann- Wachmann 1	13	58	118P/Shoemaker- Levy 4	11	64
							29P/Schwassmann- Wachmann 1	13	84
2022 Dec	29P/Schwassmann- Wachmann 1	13	22	118P/Shoemaker- Levy 4	11	50	118P/Shoemaker- Levy 4	11	64
				29P/Schwassmann- Wachmann 1	13	84	81P/Wild 2	11	33
							29P/Schwassmann- Wachmann 1	13	84
2023 Jan	118P/Shoemaker- Levy 4	11	20	118P/Shoemaker- Levy 4	11	69	118P/Shoemaker- Levy 4	11	33
	29P/Schwassmann- Wachmann 1	13	84	29P/Schwassmann- Wachmann 1	13	84	81P/Wild 2	11	33
							29P/Schwassmann- Wachmann 1	13	18
2023 Feb	118P/Shoemaker- Levy 4	12	73	118P/Shoemaker- Levy 4	12	73	96P/Machholz 1	8	12
	29P/Schwassmann- Wachmann 1	13	84	29P/Schwassmann- Wachmann 1	13	59	81P/Wild 2	11	33
							118P/Shoemaker- Levy 4	12	11
							237P/LINEAR	13	23
2023 Mar	29P/Schwassmann- Wachmann 1	13	83	364P/PanSTARRS	13	43	81P/Wild 2	12	35
	118P/Shoemaker- Levy 4	13	74	29P/Schwassmann- Wachmann 1	13	36	237P/LINEAR	12	28
				118P/Shoemaker- Levy 4	13	57	C/2020 K1 (PanSTARRS)	12	1
							96P/Machholz 1	12	16
							364P/PanSTARRS	13	87
2023 Apr	29P/Schwassmann- Wachmann 1	13	61	237P/LINEAR	11	2	237P/LINEAR	11	35
				364P/PanSTARRS	11	28	364P/PanSTARRS	11	80
				81P/Wild 2	12	18	81P/Wild 2	12	37
				29P/Schwassmann- Wachmann 1	13	12	71P/Clark	13	1
2023 May	81P/Wild 2	12	10	237P/LINEAR	10	24	237P/LINEAR	10	46
				81P/Wild 2	12	37	81P/Wild 2	12	37
							71P/Clark	13	5
							185P/Petriew	13	14
2023 Jun	237P/LINEAR	10	19	237P/LINEAR	10	53	237P/LINEAR	10	51
	81P/Wild 2	13	32	81P/Wild 2	13	37	185P/Petriew	11	13
							81P/Wild 2	13	28
							364P/PanSTARRS	13	3
							126P/IRAS	13	24
2023 Jul	237P/LINEAR	10	42	237P/LINEAR	10	56	237P/LINEAR	10	46
	103P/Hartley 2	12	6	103P/Hartley 2	12	44	185P/Petriew	11	10
	81P/Wild 2	13	34	126P/IRAS	13	13	103P/Hartley 2	12	83
				81P/Wild 2	13	36	126P/IRAS	13	55
							81P/Wild 2	13	5
2023 Aug	103P/Hartley 2	9	8	103P/Hartley 2	9	47	C/2017 K2 (PanSTARRS)	9	17
	237P/LINEAR	11	56	237P/LINEAR	11	56	103P/Hartley 2	9	90
	126P/IRAS	13	5	2P/Encke	12	1	2P/Encke	10	42
	12P/Pons- Brooks	13	70	126P/IRAS	13	42	237P/LINEAR	11	18
				12P/Pons- Brooks	13	39	185P/Petriew	11	11
							126P/IRAS	13	81
							12P/Pons- Brooks	13	8
2023 Sep	103P/Hartley 2	9	3	103P/Hartley 2	7	41	103P/Hartley 2	7	82
	237P/LINEAR	12	54	237P/LINEAR	12	32	2P/Encke	8	37
	12P/Pons- Brooks	13	68	12P/Pons- Brooks	13	32	C/2017 K2 (PanSTARRS)	9	40
	126P/IRAS	13	21	126P/IRAS	13	55	185P/Petriew	13	13
							12P/Pons- Brooks	13	3
							126P/IRAS	13	78
2023 Oct	12P/Pons- Brooks	12	59	103P/Hartley 2	7	17	103P/Hartley 2	7	71
	237P/LINEAR	13	53	C/2017 K2 (PanSTARRS)	9	17	2P/Encke	7	5
				62P/Tsuchinshan 1	12	22	C/2017 K2 (PanSTARRS)	9	47
				12P/Pons- Brooks	12	12	62P/Tsuchinshan 1	12	76
				237P/LINEAR	13	12	29P/Schwassmann- Wachmann 1	13	68
				29P/Schwassmann- Wachmann 1	13	9
2023 Nov	12P/Pons- Brooks	11	48	103P/Hartley 2	7	12	103P/Hartley 2	7	58
	144P/Kushida	13	34	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	144P/Kushida	13	8
				29P/Schwassmann- Wachmann 1	13	32	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	14	103P/Hartley 2	8	30	103P/Hartley 2	8	46
	144P/Kushida	11	71	C/2017 K2 (PanSTARRS)	10	52	C/2017 K2 (PanSTARRS)	10	22
	13P/Olbers	13	39	144P/Kushida	11	72	12P/Pons- Brooks	10	7
	P/2016 J3 (STEREO)	13	29	13P/Olbers	13	36	29P/Schwassmann- Wachmann 1	13	76
				29P/Schwassmann- Wachmann 1	13	58	26P/Grigg- Skjellerup	13	9
2024 Jan	12P/Pons- Brooks	8	25	62P/Tsuchinshan 1	7	31	62P/Tsuchinshan 1	7	68
	144P/Kushida	8	71	144P/Kushida	8	38	12P/Pons- Brooks	8	10
	C/2017 K2 (PanSTARRS)	10	57	103P/Hartley 2	10	45	103P/Hartley 2	10	40
	P/2016 J3 (STEREO)	10	24	C/2017 K2 (PanSTARRS)	10	53	26P/Grigg- Skjellerup	12	11
	103P/Hartley 2	11	10	13P/Olbers	12	19	29P/Schwassmann- Wachmann 1	13	40
	13P/Olbers	12	48	29P/Schwassmann- Wachmann 1	13	76
	29P/Schwassmann- Wachmann 1	13	26
	207P/NEAT	13	35
2024 Feb	12P/Pons- Brooks	6	18	62P/Tsuchinshan 1	7	50	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	30	29P/Schwassmann- Wachmann 1	13	12
	13P/Olbers	11	48	103P/Hartley 2	12	49
	103P/Hartley 2	12	50	29P/Schwassmann- Wachmann 1	13	76
	P/2001 Q6 (NEAT)	12	31
	207P/NEAT	12	38
	29P/Schwassmann- Wachmann 1	13	76
2024 Mar	12P/Pons- Brooks	4	17	144P/Kushida	9	22	62P/Tsuchinshan 1	9	65
	144P/Kushida	9	72	62P/Tsuchinshan 1	9	65	P/2001 Q6 (NEAT)	13	4
	62P/Tsuchinshan 1	9	32	C/2017 K2 (PanSTARRS)	11	10
	13P/Olbers	10	40	207P/NEAT	12	30
	C/2017 K2 (PanSTARRS)	11	59	29P/Schwassmann- Wachmann 1	13	55
	P/2001 Q6 (NEAT)	12	22
	207P/NEAT	12	51
	29P/Schwassmann- Wachmann 1	13	76
2024 Apr	12P/Pons- Brooks	4	9	144P/Kushida	11	16	62P/Tsuchinshan 1	11	19
	13P/Olbers	9	23	62P/Tsuchinshan 1	11	64	P/2001 Q6 (NEAT)	13	9
	144P/Kushida	11	65	29P/Schwassmann- Wachmann 1	13	28
	62P/Tsuchinshan 1	11	62	P/2001 Q6 (NEAT)	13	2
	C/2017 K2 (PanSTARRS)	12	37
	P/2001 Q6 (NEAT)	13	21
	29P/Schwassmann- Wachmann 1	13	74
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	5
	144P/Kushida	13	50
	29P/Schwassmann- Wachmann 1	13	49
2024 Jun	13P/Olbers	7	12				154P/Brewington	11	13
2024 Jul	13P/Olbers	7	18				154P/Brewington	11	23
							C/2017 K2 (PanSTARRS)	13	6
2024 Aug	13P/Olbers	8	20				154P/Brewington	12	33
							C/2017 K2 (PanSTARRS)	13	38
2024 Sep	13P/Olbers	9	19	C/2017 K2 (PanSTARRS)	13	12	C/2017 K2 (PanSTARRS)	13	65
	37P/Forbes	13	11
2024 Oct	13P/Olbers	10	13	C/2017 K2 (PanSTARRS)	13	37	333P/LINEAR	13	33
	37P/Forbes	13	12				C/2017 K2 (PanSTARRS)	13	74
2024 Nov	13P/Olbers	12	3	333P/LINEAR	10	3	333P/LINEAR	10	62
				C/2017 K2 (PanSTARRS)	13	75	C/2017 K2 (PanSTARRS)	13	75
				29P/Schwassmann- Wachmann 1	13	9	29P/Schwassmann- Wachmann 1	13	64
2024 Dec	333P/LINEAR	9	47	333P/LINEAR	9	12	333P/LINEAR	9	61
	C/2017 K2 (PanSTARRS)	13	27	29P/Schwassmann- Wachmann 1	13	33	29P/Schwassmann- Wachmann 1	13	64
				C/2017 K2 (PanSTARRS)	13	76	C/2017 K2 (PanSTARRS)	13	35
2025 Jan	333P/LINEAR	11	47	29P/Schwassmann- Wachmann 1	13	64	29P/Schwassmann- Wachmann 1	13	64
2025 Feb	29P/Schwassmann- Wachmann 1	13	29	29P/Schwassmann- Wachmann 1	13	65	29P/Schwassmann- Wachmann 1	13	25
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	43
2025 May	29P/Schwassmann- Wachmann 1	13	60	29P/Schwassmann- Wachmann 1	13	19
2025 Jun
2025 Jul							217P/LINEAR	13	3

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