Visual Comets in the Future (Northern Hemisphere)

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Updated on March 30, 2021

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
2021 Apr	C/2020 R4 (ATLAS)	8	39	C/2020 R4 (ATLAS)	8	88	C/2020 R4 (ATLAS)	8	81
C/2020 T2 (Palomar)	11	52	C/2020 T2 (Palomar)	11	89	C/2020 T2 (Palomar)	11	54
C/2021 D1 (SWAN)	11	19	7P/Pons- Winnecke	13	16	C/2019 L3 (ATLAS)	12	4
C/2019 L3 (ATLAS)	12	26	C/2017 K2 (PanSTARRS)	13	43	7P/Pons- Winnecke	13	60
C/2017 K2 (PanSTARRS)	13	7	C/2020 J1 (SONEAR)	13	20	C/2017 K2 (PanSTARRS)	13	82
C/2021 A4 (NEOWISE)	13	17		246P/NEAT	13	26
29P/Schwassmann- Wachmann 1	13	20		C/2020 J1 (SONEAR)	13	19
2021 May	C/2020 R4 (ATLAS)	9	86	C/2020 R4 (ATLAS)	9	88	C/2020 R4 (ATLAS)	9	36
C/2020 T2 (Palomar)	11	83	C/2020 T2 (Palomar)	11	87	C/2020 T2 (Palomar)	11	36
C/2019 L3 (ATLAS)	12	13	7P/Pons- Winnecke	11	15	7P/Pons- Winnecke	11	54
C/2017 K2 (PanSTARRS)	12	38	C/2017 K2 (PanSTARRS)	12	82	C/2019 L3 (ATLAS)	12	6
C/2021 D1 (SWAN)	13	18	246P/NEAT	13	14	C/2017 K2 (PanSTARRS)	12	83
C/2020 J1 (SONEAR)	13	28	C/2020 J1 (SONEAR)	13	31	4P/Faye	13	16
		15P/Finlay	13	13
		246P/NEAT	13	27
		C/2020 J1 (SONEAR)	13	15
2021 Jun	C/2020 T2 (Palomar)	11	77	C/2020 T2 (Palomar)	11	47	15P/Finlay	11	18
C/2019 L3 (ATLAS)	12	2	7P/Pons- Winnecke	11	6	C/2020 T2 (Palomar)	11	10
C/2017 K2 (PanSTARRS)	12	67	C/2017 K2 (PanSTARRS)	12	82	7P/Pons- Winnecke	11	36
C/2020 R4 (ATLAS)	13	52	C/2020 R4 (ATLAS)	13	15	4P/Faye	12	28
246P/NEAT	13	6	246P/NEAT	13	24	C/2019 L3 (ATLAS)	12	12
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
		29P/Schwassmann- Wachmann 1	13	9
2021 Jul	C/2020 T2 (Palomar)	11	53	C/2020 T2 (Palomar)	11	19	15P/Finlay	9	27
C/2017 K2 (PanSTARRS)	12	86	4P/Faye	11	1	8P/Tuttle	10	4
246P/NEAT	13	16	C/2017 K2 (PanSTARRS)	12	84	4P/Faye	11	43
	246P/NEAT	13	22	7P/Pons- Winnecke	11	19
	67P/Churyumov- Gerasimenko	13	15	C/2019 L3 (ATLAS)	12	24
		C/2017 K2 (PanSTARRS)	12	40
		10P/Tempel 2	13	30
		246P/NEAT	13	13
		29P/Schwassmann- Wachmann 1	13	33
		67P/Churyumov- Gerasimenko	13	53
2021 Aug	C/2020 T2 (Palomar)	11	33	4P/Faye	10	8	8P/Tuttle	9	2
C/2017 K2 (PanSTARRS)	12	85	C/2019 L3 (ATLAS)	11	4	15P/Finlay	9	36
6P/d'Arrest	12	50	C/2017 K2 (PanSTARRS)	12	48	4P/Faye	10	57
246P/NEAT	13	17	67P/Churyumov- Gerasimenko	12	26	C/2019 L3 (ATLAS)	11	40
	6P/d'Arrest	12	16	7P/Pons- Winnecke	11	8
	7P/Pons- Winnecke	12	3	C/2017 K2 (PanSTARRS)	12	10
	29P/Schwassmann- Wachmann 1	13	13	67P/Churyumov- Gerasimenko	12	67
	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/2020 T2 (Palomar)	12	21	C/2019 L3 (ATLAS)	11	14	15P/Finlay	11	49
C/2021 A1 (Leonard)	13	2	C/2017 K2 (PanSTARRS)	11	21	C/2019 L3 (ATLAS)	11	59
	7P/Pons- Winnecke	13	5	C/2021 A1 (Leonard)	13	17
	29P/Schwassmann- Wachmann 1	13	34	29P/Schwassmann- Wachmann 1	13	87
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)	10	30	C/2019 L3 (ATLAS)	10	84
C/2020 T2 (Palomar)	12	13	104P/Kowal 2	13	18	C/2021 A1 (Leonard)	11	38
104P/Kowal 2	13	47	29P/Schwassmann- Wachmann 1	13	61	C/2019 T4 (ATLAS)	13	9
29P/Schwassmann- Wachmann 1	13	1	15P/Finlay	13	1	15P/Finlay	13	56
132P/Helin- Roman- Alu 2	13	52	132P/Helin- Roman- Alu 2	13	54	29P/Schwassmann- Wachmann 1	13	87
		132P/Helin- Roman- Alu 2	13	12
2021 Nov	6P/d'Arrest	9	27	67P/Churyumov- Gerasimenko	8	37	C/2021 A1 (Leonard)	7	50
19P/Borrelly	10	17	4P/Faye	10	48	67P/Churyumov- Gerasimenko	8	82
C/2017 K2 (PanSTARRS)	11	34	C/2019 L3 (ATLAS)	10	53	4P/Faye	10	66
104P/Kowal 2	11	45	104P/Kowal 2	12	7	C/2019 L3 (ATLAS)	10	87
29P/Schwassmann- Wachmann 1	13	21	29P/Schwassmann- Wachmann 1	13	87	C/2019 T4 (ATLAS)	12	22
C/2020 T2 (Palomar)	13	5	132P/Helin- Roman- Alu 2	13	39	29P/Schwassmann- Wachmann 1	13	87
132P/Helin- Roman- Alu 2	13	52
2021 Dec	C/2021 A1 (Leonard)	4	5	67P/Churyumov- Gerasimenko	8	58	C/2021 A1 (Leonard)	4	45
19P/Borrelly	9	35	C/2019 L3 (ATLAS)	10	90	67P/Churyumov- Gerasimenko	8	83
C/2019 L3 (ATLAS)	10	16	4P/Faye	10	62	C/2019 L3 (ATLAS)	10	89
6P/d'Arrest	10	33	29P/Schwassmann- Wachmann 1	13	87	4P/Faye	10	63
104P/Kowal 2	10	47		C/2017 K2 (PanSTARRS)	11	11
C/2017 K2 (PanSTARRS)	11	15		C/2019 T4 (ATLAS)	12	26
4P/Faye	11	10		22P/Kopff	12	5
29P/Schwassmann- Wachmann 1	13	86		29P/Schwassmann- Wachmann 1	13	23
		9P/Tempel 1	13	22
2022 Jan	C/2021 A1 (Leonard)	6	3	67P/Churyumov- Gerasimenko	9	84	67P/Churyumov- Gerasimenko	9	84
19P/Borrelly	8	46	C/2019 L3 (ATLAS)	10	88	C/2019 L3 (ATLAS)	10	27
67P/Churyumov- Gerasimenko	9	26	4P/Faye	11	64	C/2017 K2 (PanSTARRS)	10	28
C/2019 L3 (ATLAS)	10	47	C/2019 T4 (ATLAS)	12	7	22P/Kopff	11	8
104P/Kowal 2	10	54	29P/Schwassmann- Wachmann 1	13	60	4P/Faye	11	6
4P/Faye	11	65		C/2019 T4 (ATLAS)	12	25
6P/d'Arrest	12	34		9P/Tempel 1	12	22
29P/Schwassmann- Wachmann 1	13	86
2022 Feb	19P/Borrelly	8	48	C/2019 L3 (ATLAS)	10	63	C/2017 K2 (PanSTARRS)	10	42
C/2019 L3 (ATLAS)	10	82	67P/Churyumov- Gerasimenko	10	84	67P/Churyumov- Gerasimenko	10	19
67P/Churyumov- Gerasimenko	10	82	104P/Kowal 2	10	11	22P/Kopff	11	8
104P/Kowal 2	10	63	C/2019 T4 (ATLAS)	11	28	C/2019 T4 (ATLAS)	11	27
4P/Faye	13	67	4P/Faye	13	49	9P/Tempel 1	12	21
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	A/2019 U5	13	77
	A/2019 U5	13	18
2022 Mar	19P/Borrelly	9	46	C/2017 K2 (PanSTARRS)	9	1	C/2017 K2 (PanSTARRS)	9	54
C/2019 L3 (ATLAS)	10	76	C/2019 L3 (ATLAS)	10	35	22P/Kopff	10	8
C/2019 T4 (ATLAS)	11	13	C/2019 T4 (ATLAS)	11	33	C/2019 T4 (ATLAS)	11	9
104P/Kowal 2	12	65	104P/Kowal 2	12	15	9P/Tempel 1	11	18
67P/Churyumov- Gerasimenko	12	81	67P/Churyumov- Gerasimenko	12	60	A/2019 U5	13	86
A/2019 U5	13	3	A/2019 U5	13	45	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)	11	60	C/2019 L3 (ATLAS)	11	10	22P/Kopff	10	10
C/2019 T4 (ATLAS)	11	40	19P/Borrelly	11	3	9P/Tempel 1	11	15
A/2019 U5	13	36	C/2019 T4 (ATLAS)	11	37	C/2021 A1 (Leonard)	12	11
116P/Wild 4	13	74	A/2019 U5	13	82	A/2019 U5	13	84
C/2020 V2 (ZTF)	13	64	116P/Wild 4	13	44	117P/Helin- Roman- Alu 1	13	26
29P/Schwassmann- Wachmann 1	13	41	C/2020 V2 (ZTF)	13	64	C/2020 V2 (ZTF)	13	33
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	C/2019 T4 (ATLAS)	11	26	22P/Kopff	11	17
C/2019 T4 (ATLAS)	11	43	19P/Borrelly	12	3	9P/Tempel 1	12	20
C/2019 L3 (ATLAS)	11	33	A/2019 U5	12	83	A/2019 U5	12	57
19P/Borrelly	12	37	117P/Helin- Roman- Alu 1	13	15	C/2021 A1 (Leonard)	13	16
A/2019 U5	12	74	C/2021 A1 (Leonard)	13	10	117P/Helin- Roman- Alu 1	13	26
73P/Schwassmann- Wachmann 3	13	55	73P/Schwassmann- Wachmann 3	13	15	C/2020 V2 (ZTF)	13	19
C/2020 V2 (ZTF)	13	64	C/2020 V2 (ZTF)	13	43
116P/Wild 4	13	64	116P/Wild 4	13	22
2022 Jun	C/2017 K2 (PanSTARRS)	6	47	C/2017 K2 (PanSTARRS)	6	65	C/2017 K2 (PanSTARRS)	6	59
C/2019 T4 (ATLAS)	11	40	C/2019 T4 (ATLAS)	11	10	22P/Kopff	11	31
C/2019 L3 (ATLAS)	11	6	A/2019 U5	12	64	169P/NEAT	12	11
45P/Honda- Mrkos- Pajdusakova	12	8	73P/Schwassmann- Wachmann 3	13	8	A/2019 U5	12	30
73P/Schwassmann- Wachmann 3	12	44	117P/Helin- Roman- Alu 1	13	25	9P/Tempel 1	12	29
A/2019 U5	12	85	C/2020 V2 (ZTF)	13	25	117P/Helin- Roman- Alu 1	13	25
117P/Helin- Roman- Alu 1	13	8	19P/Borrelly	13	1	C/2020 V2 (ZTF)	13	8
C/2020 V2 (ZTF)	13	48	9P/Tempel 1	13	2	C/2021 A1 (Leonard)	13	14
19P/Borrelly	13	29	116P/Wild 4	13	3
116P/Wild 4	13	41	C/2021 A1 (Leonard)	13	17
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
C/2019 T4 (ATLAS)	11	25	A/2019 U5	12	33	22P/Kopff	12	53
C/2020 R7 (ATLAS)	12	1	C/2020 V2 (ZTF)	13	10	A/2019 U5	12	1
A/2019 U5	12	66	117P/Helin- Roman- Alu 1	13	23	C/2020 V2 (ZTF)	13	2
C/2020 V2 (ZTF)	13	30	9P/Tempel 1	13	15	117P/Helin- Roman- Alu 1	13	13
117P/Helin- Roman- Alu 1	13	23		9P/Tempel 1	13	32
2022 Aug	C/2017 K2 (PanSTARRS)	6	41	C/2017 K2 (PanSTARRS)	6	13	C/2020 V2 (ZTF)	12	13
73P/Schwassmann- Wachmann 3	11	12	A/2019 U5	12	2	22P/Kopff	12	59
C/2020 R7 (ATLAS)	12	12	22P/Kopff	12	36	81P/Wild 2	13	4
C/2019 T4 (ATLAS)	12	11	117P/Helin- Roman- Alu 1	13	15	29P/Schwassmann- Wachmann 1	13	38
A/2019 U5	12	40
C/2020 V2 (ZTF)	12	17
117P/Helin- Roman- Alu 1	13	23
2022 Sep	C/2017 K2 (PanSTARRS)	6	20	C/2020 V2 (ZTF)	12	2	C/2020 V2 (ZTF)	12	30
73P/Schwassmann- Wachmann 3	11	9	118P/Shoemaker- Levy 4	13	2	81P/Wild 2	12	15
C/2020 V2 (ZTF)	12	10	22P/Kopff	13	57	C/2019 L3 (ATLAS)	12	11
C/2019 T4 (ATLAS)	12	3	29P/Schwassmann- Wachmann 1	13	11	118P/Shoemaker- Levy 4	13	56
A/2019 U5	12	21		22P/Kopff	13	58
C/2020 R7 (ATLAS)	12	13		C/2020 Y2 (ATLAS)	13	4
117P/Helin- Roman- Alu 1	13	23		29P/Schwassmann- Wachmann 1	13	65
22P/Kopff	13	3
2022 Oct	C/2017 K2 (PanSTARRS)	6	3	C/2020 V2 (ZTF)	11	13	C/2020 V2 (ZTF)	11	46
C/2020 V2 (ZTF)	11	8	118P/Shoemaker- Levy 4	12	13	81P/Wild 2	11	23
73P/Schwassmann- Wachmann 3	12	18	29P/Schwassmann- Wachmann 1	13	33	A/2019 U5	12	2
A/2019 U5	12	5		118P/Shoemaker- Levy 4	12	64
C/2020 R7 (ATLAS)	12	13		C/2019 L3 (ATLAS)	12	27
		29P/Schwassmann- Wachmann 1	13	84
		C/2020 Y2 (ATLAS)	13	5
2022 Nov	C/2020 V2 (ZTF)	10	17	C/2020 V2 (ZTF)	10	30	C/2020 V2 (ZTF)	10	53
C/2020 R7 (ATLAS)	13	7	118P/Shoemaker- Levy 4	11	28	81P/Wild 2	11	29
73P/Schwassmann- Wachmann 3	13	20	29P/Schwassmann- Wachmann 1	13	58	118P/Shoemaker- Levy 4	11	64
C/2020 K1 (PanSTARRS)	13	16	C/2020 Y2 (ATLAS)	13	4	A/2019 U5	11	27
		C/2019 T4 (ATLAS)	12	13
		C/2019 L3 (ATLAS)	12	31
		29P/Schwassmann- Wachmann 1	13	84
		C/2020 Y2 (ATLAS)	13	1
2022 Dec	C/2020 V2 (ZTF)	9	43	C/2020 V2 (ZTF)	9	40	C/2020 V2 (ZTF)	9	50
29P/Schwassmann- Wachmann 1	13	22	118P/Shoemaker- Levy 4	11	50	118P/Shoemaker- Levy 4	11	64
	C/2019 L3 (ATLAS)	13	9	A/2019 U5	11	51
	29P/Schwassmann- Wachmann 1	13	84	81P/Wild 2	11	33
	C/2020 Y2 (ATLAS)	13	4	C/2019 T4 (ATLAS)	12	36
		C/2019 L3 (ATLAS)	13	30
		29P/Schwassmann- Wachmann 1	13	84
2023 Jan	C/2020 V2 (ZTF)	9	60	C/2020 V2 (ZTF)	9	38	C/2020 V2 (ZTF)	9	25
118P/Shoemaker- Levy 4	11	20	A/2019 U5	11	12	A/2019 U5	11	57
29P/Schwassmann- Wachmann 1	13	84	118P/Shoemaker- Levy 4	11	69	118P/Shoemaker- Levy 4	11	33
	C/2019 L3 (ATLAS)	13	21	81P/Wild 2	11	33
	29P/Schwassmann- Wachmann 1	13	84	C/2019 T4 (ATLAS)	12	52
		C/2019 L3 (ATLAS)	13	24
		29P/Schwassmann- Wachmann 1	13	18
		C/2020 R7 (ATLAS)	13	21
2023 Feb	C/2020 V2 (ZTF)	9	59	C/2020 V2 (ZTF)	9	19	96P/Machholz 1	8	12
118P/Shoemaker- Levy 4	12	73	A/2019 U5	10	38	C/2020 V2 (ZTF)	9	2
29P/Schwassmann- Wachmann 1	13	84	118P/Shoemaker- Levy 4	12	73	A/2019 U5	10	56
C/2019 L3 (ATLAS)	13	3	C/2019 T4 (ATLAS)	12	12	81P/Wild 2	11	33
	C/2019 L3 (ATLAS)	13	20	118P/Shoemaker- Levy 4	12	11
	29P/Schwassmann- Wachmann 1	13	59	C/2019 T4 (ATLAS)	12	61
		237P/LINEAR	13	23
		C/2020 R7 (ATLAS)	13	39
2023 Mar	C/2020 V2 (ZTF)	9	42	A/2019 U5	10	54	A/2019 U5	10	55
A/2019 U5	10	28	C/2019 T4 (ATLAS)	12	41	81P/Wild 2	12	35
C/2019 L3 (ATLAS)	13	21	364P/PanSTARRS	13	43	237P/LINEAR	12	28
29P/Schwassmann- Wachmann 1	13	83	C/2020 R7 (ATLAS)	13	12	C/2020 K1 (PanSTARRS)	12	1
118P/Shoemaker- Levy 4	13	74	C/2019 L3 (ATLAS)	13	20	C/2019 T4 (ATLAS)	12	68
	29P/Schwassmann- Wachmann 1	13	36	96P/Machholz 1	12	16
	118P/Shoemaker- Levy 4	13	57	364P/PanSTARRS	13	87
		C/2020 R7 (ATLAS)	13	62
2023 Apr	C/2020 V2 (ZTF)	10	14	A/2019 U5	10	53	A/2019 U5	10	8
A/2019 U5	10	53	237P/LINEAR	11	2	237P/LINEAR	11	35
C/2019 T4 (ATLAS)	13	25	364P/PanSTARRS	11	28	364P/PanSTARRS	11	80
C/2020 R7 (ATLAS)	13	4	81P/Wild 2	12	18	81P/Wild 2	12	37
29P/Schwassmann- Wachmann 1	13	61	C/2019 T4 (ATLAS)	13	73	C/2019 T4 (ATLAS)	13	70
	C/2020 R7 (ATLAS)	13	48	C/2020 R7 (ATLAS)	13	77
	29P/Schwassmann- Wachmann 1	13	12	71P/Clark	13	1
2023 May	A/2019 U5	10	52	A/2019 U5	10	25	237P/LINEAR	10	46
81P/Wild 2	12	10	237P/LINEAR	10	24	81P/Wild 2	12	37
C/2019 T4 (ATLAS)	13	60	81P/Wild 2	12	37	C/2019 T4 (ATLAS)	13	51
C/2020 R7 (ATLAS)	13	47	C/2019 T4 (ATLAS)	13	76	C/2020 R7 (ATLAS)	13	81
	C/2020 R7 (ATLAS)	13	86	71P/Clark	13	5
		185P/Petriew	13	14
2023 Jun	237P/LINEAR	10	19	237P/LINEAR	10	53	C/2020 V2 (ZTF)	9	13
A/2019 U5	11	30	81P/Wild 2	13	37	237P/LINEAR	10	51
81P/Wild 2	13	32	C/2019 T4 (ATLAS)	13	77	185P/Petriew	11	13
C/2019 T4 (ATLAS)	13	77	C/2020 R7 (ATLAS)	13	86	81P/Wild 2	13	28
C/2020 R7 (ATLAS)	13	51		364P/PanSTARRS	13	3
		C/2019 T4 (ATLAS)	13	32
		126P/IRAS	13	24
		C/2020 R7 (ATLAS)	13	52
2023 Jul	237P/LINEAR	10	42	237P/LINEAR	10	56	C/2020 V2 (ZTF)	9	36
A/2019 U5	11	3	103P/Hartley 2	12	44	237P/LINEAR	10	46
103P/Hartley 2	12	6	126P/IRAS	13	13	185P/Petriew	11	10
81P/Wild 2	13	34	81P/Wild 2	13	36	103P/Hartley 2	12	83
C/2019 T4 (ATLAS)	13	75	C/2019 T4 (ATLAS)	13	44	126P/IRAS	13	55
		81P/Wild 2	13	5
		C/2019 T4 (ATLAS)	13	7
2023 Aug	103P/Hartley 2	9	8	C/2020 V2 (ZTF)	9	15	C/2017 K2 (PanSTARRS)	9	17
237P/LINEAR	11	56	103P/Hartley 2	9	47	C/2020 V2 (ZTF)	9	47
126P/IRAS	13	5	237P/LINEAR	11	56	103P/Hartley 2	9	90
12P/Pons- Brooks	13	70	2P/Encke	11	5	237P/LINEAR	11	18
	126P/IRAS	13	42	185P/Petriew	11	11
	12P/Pons- Brooks	13	39	2P/Encke	11	49
		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	C/2020 V2 (ZTF)	9	28	2P/Encke	8	46
12P/Pons- Brooks	13	68	2P/Encke	11	2	C/2017 K2 (PanSTARRS)	9	40
126P/IRAS	13	21	237P/LINEAR	12	32	C/2020 V2 (ZTF)	9	42
	12P/Pons- Brooks	13	32	185P/Petriew	13	13
	126P/IRAS	13	55	12P/Pons- Brooks	13	3
		126P/IRAS	13	78
2023 Oct	C/2020 V2 (ZTF)	10	14	103P/Hartley 2	7	17	103P/Hartley 2	7	71
12P/Pons- Brooks	12	59	C/2017 K2 (PanSTARRS)	9	17	2P/Encke	7	18
237P/LINEAR	13	53	C/2020 V2 (ZTF)	9	23	C/2017 K2 (PanSTARRS)	9	47
	62P/Tsuchinshan 1	12	22	C/2020 V2 (ZTF)	9	4
	12P/Pons- Brooks	12	12	62P/Tsuchinshan 1	12	76
	237P/LINEAR	13	12	A/2019 U5	12	11
	29P/Schwassmann- Wachmann 1	13	9	29P/Schwassmann- Wachmann 1	13	68
2023 Nov	C/2020 V2 (ZTF)	10	13	103P/Hartley 2	7	12	103P/Hartley 2	7	58
12P/Pons- Brooks	11	48	62P/Tsuchinshan 1	8	22	62P/Tsuchinshan 1	8	76
144P/Kushida	13	34	C/2017 K2 (PanSTARRS)	9	48	C/2017 K2 (PanSTARRS)	9	48
	C/2020 V2 (ZTF)	10	5	A/2019 U5	12	19
	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
C/2020 V2 (ZTF)	11	13	144P/Kushida	11	72	12P/Pons- Brooks	10	7
13P/Olbers	13	39	13P/Olbers	13	36	A/2019 U5	12	19
	29P/Schwassmann- Wachmann 1	13	58	29P/Schwassmann- Wachmann 1	13	76
		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
103P/Hartley 2	11	10	C/2017 K2 (PanSTARRS)	10	53	A/2019 U5	12	13
C/2020 V2 (ZTF)	12	10	13P/Olbers	12	19	26P/Grigg- Skjellerup	12	11
13P/Olbers	12	48	A/2019 U5	12	10	29P/Schwassmann- Wachmann 1	13	40
29P/Schwassmann- Wachmann 1	13	26	29P/Schwassmann- Wachmann 1	13	76
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	A/2019 U5	12	10
P/2001 Q6 (NEAT)	12	31	29P/Schwassmann- Wachmann 1	13	76
207P/NEAT	12	38
A/2019 U5	13	10
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	A/2019 U5	13	4
P/2001 Q6 (NEAT)	12	22	29P/Schwassmann- Wachmann 1	13	55
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	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
A/2019 U5	13	14
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
2025 Aug
2025 Sep	210P/Christensen	13	12		414P/2021 A3 (STEREO)	12	15
2025 Oct	210P/Christensen	11	11	24P/Schaumasse	13	18	414P/2021 A3 (STEREO)	12	3
		24P/Schaumasse	13	73
2025 Nov		24P/Schaumasse	10	18	210P/Christensen	8	11
		24P/Schaumasse	10	74
2025 Dec		24P/Schaumasse	8	14	24P/Schaumasse	8	73
	29P/Schwassmann- Wachmann 1	13	10	210P/Christensen	9	30
		88P/Howell	12	3
		29P/Schwassmann- Wachmann 1	13	52
2026 Jan		24P/Schaumasse	8	6	24P/Schaumasse	8	68
	29P/Schwassmann- Wachmann 1	13	32	88P/Howell	11	4
		210P/Christensen	13	33
		29P/Schwassmann- Wachmann 1	13	51
2026 Feb	29P/Schwassmann- Wachmann 1	13	4	24P/Schaumasse	8	17	24P/Schaumasse	8	63
	29P/Schwassmann- Wachmann 1	13	51	88P/Howell	9	4
		29P/Schwassmann- Wachmann 1	13	51
2026 Mar	29P/Schwassmann- Wachmann 1	13	35	24P/Schaumasse	10	40	88P/Howell	9	2
	29P/Schwassmann- Wachmann 1	13	53	24P/Schaumasse	10	61
		29P/Schwassmann- Wachmann 1	13	17

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