Engelhardsberg observatory
Comets By Designation (table is sortable)
info
Nr.
comet
last observed
thumbnail
observations
1
2P/Encke
08.09.2023
11
2
4P/Faye
04.09.2021
6
3
6P/d'Arrest
01.09.2021
3
4
7P/Pons-Winnecke
15.04.2021
3
5
8P/Tuttle
08.05.2021
1
6
9P/Tempel
2016
6
7
10P/Tempel
08.09.2021
5
8
11P/Tempel-Swift-Linear
14.11.2020
1
9
12P/Pons-Brooks
28.03.2024
17
10
13P/Olbers
01.09.2024
16
11
14P/Wolf
2017
1
12
15P/Finlay
15.08.2021
6
13
16P/Brooks
2014
1
14
17P/Holmes
29.10.2021
6
15
19P/Borrelly
20.03.2022
4
16
21P/Giacobini-Zinner
18.09.2018
32
17
22P/Kopff
25.07.2022
6
18
24P/Schaumasse
22.02.2018
4
19
28P/Neujmin
15.08.2021
1
20
29P/Schwassmann-Wachmann
27.12.2024
18
21
30P/Reinmuth
26.12.2024
3
22
31P/Schwassmann-Wachmann
07.03.2019
1
23
32P/Comas-Sola
30.12.2023
10
24
33P/Daniel
25.12.2024
3
25
36P/Whipple
28.08.2019
1
26
37P/Forbes
20.08.2018
4
27
38P/Stephan-Oterma
27.02.2019
6
28
40P/Väisälä
2015
1
29
41P/Tuttle-Giacobini-Kresak
2017
10
30
43P/Wolf-Harrington
01.02.2025
5
31
44P/Reinmuth
05.09.2022
2
32
45P/Honda-Mrkos-Pajdusakova
2017
12
33
46P/Wirtanen
07.03.2019
5
34
47P/Ashbrook-Jackson
2017
4
35
48P/Johnson
15.08.2018
5
36
49P/Arend-Rigaux
01.02.2025
2
37
50P/Arend
26.12.2024
3
38
52P/Harrington/Abell
2014
3
39
53P/van Biesbroeck
2016
4
40
54P/de Vico-Swift-NEAT
31.08.2024
3
41
56P/Slaughter-Burnham
2016
4
42
57P/du Toit-Neujmin-Delporte
2015
1
43
59P/Kearns-Kwee
2017
1
44
60P/Tsuchinshan
30.03.2019
2
45
61P/Shajn-Schaldach
30.08.2022
3
46
62P/Tsuchinshan 1
21.01.2024
6
47
63P/Wild
2013
1
48
64P/Swift-Gehrels
18.09.2018
12
49
65P/Gunn
07.06.2024
5
50
66P/du Toit
13.08.2018
1
51
67P/Churyumov-Gerasimenko
02.03.2022
8
52
68P/Klemola
26.08.2019
5
53
70P/Kojima
23.03.2022
7
54
71P/Clark
2017
2
55
73P/Schwassmann-Wachmann 3
26.03.2022
5
56
74P/Smirnova-Chernykh
06.04.2018
5
57
76P/West-Kohoutek-Ikemura
04.12.2019
1
58
77P/Longmore
2016
3
59
78P/Gehrels 2
22.03.2020
7
60
81P/Wild
19.01.2023
11
61
84P/Giclas
2014
2
62
87P/Bus
24.03.2020
2
63
88P/Howell
26.05.2020
12
64
89P/Russell
2016
1
65
90P/Gehrels 1
2017
1
66
91P/Rusell
11.04.2020
1
67
93P/Lovas 1
2017
3
68
94P/Russell
09.02.2023
2
69
95P/Chiron
2016
3
70
98P/Takamizawa
2013
2
71
99P/Kowal 1
23.03.2022
3
72
100P/Hartley 1
27.03.2022
2
73
101P/Chernykh
30.11.2019
3
74
102P/Shoemaker
2013
3
75
103P/Hartley 2
05.09.2023
6
76
104P/Kowal 2
26.03.2022
6
77
105P/Singer Brewster
08.04.2018
2
78
106P/Schuster
2014
1
79
107P/Wilson-Harrington
07.08.2022
1
80
108P/Ciffreo
28.02.2022
5
81
110P/Hartley
26.03.2022
4
82
112P/Urata-Niijima
19.04.2020
3
83
114P/Wiseman-Skiff
22.03.2020
5
84
115P/Maury
20.08.2020
3
85
116P/Wild
26.03.2022
7
86
117P/Helin-Roman-Alu 1
18.03.2020
4
87
118P/Shoemaker-Levy 4
27.12.2022
4
88
119P/Parker-Hartley
27.12.2022
5
89
121P/Shoemaker-Holt 2
16.01.2024
1
90
123P/West-Hartley
07.05.2019
6
91
124P/Mrkos
15.03.2020
5
92
125P/Spacewatch
05.06.2024
2
93
126P/Iras
06.09.2023
2
94
127P/Holm-Olmstead
24.08.2022
1
95
128P/Shoemaker-Holt 1
2016
1
96
129P/Shoemaker-Levy
14.08.2018
4
97
130P/McNaught-Hughes
04.09.2024
5
98
131P/Mueller
05.09.2018
1
99
132P/Helin-Roman-Alu 2
06.09.2021
3
100
133P/Elst-Pizzaro
02.09.2019
1
101
134P/Kowal-Vavrova
2014
6
102
136P/Mueller
2016
1
103
137P/Shoemaker-Levy
14.08.2018
4
104
139P/Vaisala-Oterma
2017
2
105
141P/Machholz
07.03.2021
2
106
143P/Kowal-Mrkos
08.04.2018
1
107
144P/Kushida
28.01.2024
6
108
145P/Shoemaker-Levy
2017
1
109
146P/Shoemaker-LINEAR
16.08.2024
5
110
149P/Mueller
29.03.2019
1
111
150P/LONEOS
09.01.2024
3
112
152P/Helin-Lawrence
13.04.2021
1
113
154P/Brewington
13.08.2024
9
114
155P/Shoemaker
15.03.2020
2
115
156P/Russell-LINEAR
07.03.2021
3
116
157P/Tritton
06.09.2022
2
117
158P/Kowal-LINEAR
2013
1
118
159P/LONEOS
2017
1
119
160P/LINEAR
21.01.2020
2
120
162P/Siding Spring
2016
1
121
164P/Christensen
27.02.2019
1
122
170P/Christensen
2014
2
123
171P/Spahr
18.09.2018
1
124
172P/Yeung
2016
1
125
173P/Mueller
28.12.2019
2
126
174P/Echeclus
2016
2
127
176P/LINEAR
2016
1
128
178P/Hug-Bell
2014
3
129
180P/NEAT
2016
2
130
183P/Korlevic-Juric
06.04.2018
1
131
184P/Lovas
2013
1
132
185P/Petriew
06.04.2018
2
133
187P/LINEAR
19.04.2018
1
134
188P/LINEAR-Mueller
2017
2
135
190P/Mueller
27.08.2024
3
136
191P/McNaught
2014
1
137
192P/Shoemaker-Levy 1
30.08.2024
1
138
193P/LINEAR-NEAT
12.09.2021
4
139
194P/Kowal
2016
1
140
195P/Hill
25.12.2024
1
141
199P/Shoemaker
03.04.2022
1
142
200P/Larsen
02.08.2018
1
143
201P/LONEOS
2015
2
144
202P/Scotti
03.12.2023
1
145
203P/Korlevic
30.11.2019
2
146
204P/LINEAR-NEAT
18.01.2023
3
147
205P/Giacobini
2015
1
148
207P/NEAT
07.03.2024
2
149
208P/McMillan
01.09.2024
3
150
209P/LINEAR
2014
8
151
210P/Christensen
25.04.2020
6
152
211P/Hill
21.02.2023
3
153
213P/Van Ness
2017
1
154
216P/LINEAR
07.03.2024
1
155
217P/LINEAR
2017
2
156
218P/LINEAR
2015
2
157
219P/LINEAR
2016
2
158
221P/LINEAR
2015
1
159
223P/Skiff
11.09.2018
2
160
226P/Pigott-LINEAR-Kowalski
09.01.2024
4
161
227P/Catalina-LINEAR
03.03.2024
2
162
228P/LINEAR
01.01.2020
1
163
229P/Gibbs
01.09.2024
2
164
230P/LINEAR
2015
1
165
231P/LINEAR
31.03.2019
2
166
234P/LINEAR
02.02.2025
1
167
235P/LINEAR
04.04.2018
1
168
236P/LINEAR
2017
2
169
237P/LINEAR
04.09.2023
2
170
238P/Read
2016
1
171
239P/LINEAR
06.04.2019
1
172
240P/NEAT
27.02.2019
1
173
242P/Spahr
01.02.2025
2
174
243P/NEAT
06.08.2018
1
175
244P/Scotti
2014
1
176
245P/WISE
14.08.2018
2
177
246P/NEAT
16.04.2020
8
178
247P/LINEAR
27.02.2019
1
179
249P/LINEAR
14.04.2020
4
180
250P/Larson
21.02.2018
1
181
252P/LINEAR
2016
3
182
253P/PANSTARRS
30.07.2024
1
183
257P/Catalina
2013
4
184
260P/McNaught
26.10.2019
7
185
261P/Larson
03.09.2019
3
186
263P/Gibbs
15.03.2023
3
187
266P/Christensen
22.03.2020
4
188
268P/Bernardi
01.02.2025
2
189
269P/Jedicke
2015
3
190
270P/Gehrels
2014
1
191
273P/Pons-Gambart
2013
1
192
274P/Tombaugh-Tenagra
27.02.2022
1
193
276P/Vorobjov
04.11.2024
2
194
277P/LINEAR
14.11.2020
3
195
278P/McNaught
19.04.2020
2
196
279P/La Sagra
2016
1
197
282P
04.04.2021
1
198
284P/McNaught
02.09.2021
3
199
285P/LINEAR
01.09.2022
8
200
286P/Christensen
29.08.2022
3
201
287P/Christensen
07.09.2023
1
202
288P
2016
1
203
289P/Blanpain
21.01.2020
3
204
290P/Jager
2014
5
205
291P/NEAT
2013
2
206
292P/Li
2013
1
207
293P/Spacewatch
2014
2
208
294P/LINEAR
2014
1
209
296P/Garradd
2014
2
210
297P/Beshore
2014
2
211
299P/Catalina-PANSTARRS
2016
1
212
302P/Lemmon-PANSTARRS
2016
1
213
303P/NEAT
2014
1
214
304P/Ory
21.08.2020
1
215
305P/Skiff
30.11.2024
5
216
307P/LINEAR
2014
1
217
312P/NEAT
21.08.2020
1
218
314P/Montani
2015
1
219
315P/LONEOS
2017
5
220
318P/McNaught-Hartley
2015
1
221
325P/Yang-Gao
02.07.2022
2
222
327P/Van Ness
06.09.2022
5
223
328P/LONEOS-Tucker
02.09.2024
4
224
329P/LINEAR-Catalina
2015
1
225
330P/Catalina
2016
1
226
332P/Ikeya-Murakami
2016
2
227
333P/LINEAR
19.01.2025
7
228
334P/NEAT
20.05.2018
1
229
337P/WISE
01.07.2022
2
230
338P/McNaught
30.08.2024
4
231
340P/Boattini
2016
1
232
341P/Gibbs
2016
1
233
343P/NEAT-LONEOS
2016
2
234
344P/Read
2016
1
235
345P/LINEAR
2016
1
236
346P/Catalina
2016
1
237
347P/PANSTARRS
05.09.2023
2
238
349P/Lemmon
2017
1
239
352P/Skiff
2017
2
240
355P/LINEAR-NEAT
2017
2
241
356P/WISE
2017
1
242
360P/WISE
2017
1
243
361P/Spacewatch
2017
2
244
362P/(457175)
2017
1
245
364P/PANSTARRS
27.03.2023
6
246
365P/LINEAR
04.04.2018
1
247
366P/LINEAR
07.04.2018
1
248
368P/NEAT
15.09.2018
3
249
369P/Hill
12.09.2018
1
250
370P/NEAT
18.09.2018
1
251
371P/LINEAR-Skiff
12.09.2018
1
252
373P/Rinner
06.04.2019
1
253
375P/Hill
31.03.2019
2
254
376P/Loneos
30.04.2019
3
255
377P/Scotti
23.03.2020
1
256
378P/McNaught
30.08.2022
1
257
379P/Spacewatch
23.04.2019
2
258
380P/PANSTARRS
30.04.2019
1
259
382P/Larson
07.08.2022
2
260
384P/Kowalski
28.12.2019
3
261
385P/Hill
30.11.2019
1
262
390P/Gibbs
21.01.2020
2
263
392P/LINEAR
30.11.2019
1
264
395P/Catalina-NEAT
14.11.2022
4
265
397P/Lemmon
21.08.2020
1
266
398P/Boattini
07.03.2021
3
267
399P/PANSTARRS
2013
1
268
402P/LINEAR
28.02.2022
2
269
404P/Bressi
17.12.2023
2
270
405P/Lemmon
14.11.2020
2
271
407P/PANSTARRS-Fuls
14.04.2020
3
272
408P/Novichonok-Gerke
03.09.2021
2
273
409P/LONEOS-Hill
04.04.2021
2
274
413P/Larson
04.04.2021
2
275
415P/Tenagra
08.04.2021
1
276
418P/LINEAR
08.04.2021
1
277
425P/Kowalski
07.09.2021
1
278
433P/(248370)
15.08.2021
2
279
440P/Kobayashi
26.03.2022
3
280
442P/McNaught
02.09.2022
2
281
445P/Lemmon-PANSTARRS
01.09.2022
2
282
446P/McNaught
06.08.2022
1
283
450P/LONEOS
04.12.2024
1
284
452P/Sheppard-Jewitt
21.02.2023
1
285
453P/WISE-Lemmon
17.03.2023
1
286
465P/Hill
15.08.2023
1
287
466P/PANSTARRS
07.09.2023
1
288
471P/2010 YK3
03.12.2023
3
289
472P/NEAT-LINEAR
01.02.2025
3
290
473P/NEAT
07.03.2024
5
291
475P/Spacewatch-LINEAR
08.03.2024
1
292
476P/PANSTARRS
18.01.2025
1
293
478P/ATLAS
28.03.2024
1
294
479P/Elenin
07.03.2024
4
295
482P/PANSTARRS
09.03.2024
1
296
487P/Siding Spring
24.11.2024
4
297
488P/NEAT-PANSTARRS
11.08.2024
1
298
492P/LINEAR
26.12.2024
2
299
493P/LONEOS
29.10.2024
1
300
496P/Hill
01.02.2025
3
301
6478 Gault (comet like asteroid)
30.03.2019
1
302
C/1975 V1 (West)
1976
1
303
C/2006 S3 (Loneos)
2015
6
304
C/2006 W3 (Christensen)
2009
1
305
C/2007 Q3 (SidingSpring)
2010
1
306
C/2008 S3 (Boattini)
2014
2
307
C/2009 F4 (McNaught)
2014
1
308
C/2009 K5 (McNaught)
2010
1
309
C/2010 S1 (LINEAR)
2014
7
310
C/2010 U3 (Boattini)
27.02.2019
3
311
C/2011 J2 (LINEAR)
2015
13
312
C/2011 KP36 (Spacewatch)
2016
5
313
C/2011 L4 (PANSTARRS)
2014
13
314
C/2011 R1 (McNaught)
2013
4
315
C/2012 A1 (PANSTARRS)
2013
1
316
C/2012 A2 (Linear)
2013
2
317
P/2012 B1 (PANSTARRS)
2014
1
318
P/2012 F2 (PANSTARRS)
2013
1
319
C/2012 F3 (PANSTARRS)
2015
3
320
C/2012 F6 (Lemmon)
2014
9
321
C/2012 J1 (Catalina)
2014
3
322
C/2012 K1 (PANSTARRS)
2014
17
323
C/2012 K6 (McNaught)
2014
5
324
C/2012 K8 (Lemmon)
2014
3
325
C/2012 LP26 (Palomar)
2016
4
326
C/2012 S1 (ISON)
2013
2
327
C/2012 S3 (PANSTARRS)
2013
4
328
C/2012 S4 (PANSTARRS)
2013
1
329
C/2012 U1 (PANSTARRS)
2013
1
330
C/2012 X1 (LINEAR)
2014
6
331
C/2013 A1 (Siding Spring)
2015
2
332
C/2013 C2 (Tenagra)
2014
2
333
C/2013 E1 (McNaught)
2014
1
334
C/2013 E2 (Iwamoto)
2013
2
335
C/2013 F2 (Catalina)
2014
2
336
C/2013 F3 (McNaught)
2013
1
337
C/2013 G1 (Kowalski)
2014
1
338
C/2013 G3 (PANSTARRS)
2014
3
339
C/2013 G5 (Catalina)
2013
1
340
C/2013 G8(PANSTARRS)
2014
1
341
C/2013 G9(Tenagra)
2014
1
342
C/2013 H1(La Sagra)
2013
1
343
C/2013 H2(Boattini)
2014
1
344
P/2013 J2 (McNaught)
2013
5
345
C/2013 P2 (PANSTARRS)
2014
1
346
C/2013 P3 (Palomar)
2014
1
347
C/2013 P4 (PANSTARRS)
2014
1
348
C/2013 R1 (Lovejoy)
2014
11
349
P/2013 R3 (Catalina-PANSTARRS)
2013
2
350
P/2013 T2 (Schwartz)
2013
1
351
C/2013 TW5
2015
4
352
C/2013 U1 (Catalina)
2013
1
353
C/2013 U2 (Holvorcem)
2015
3
354
C/2013 UQ4 (Catalina)
2014
9
355
C/2013 US10 (Catalina)
2016
10
356
C/2013 V1 (Boattini)
2014
8
357
C/2013 V2 (Borisov)
2015
6
358
C/2013 V3 (Nevski)
2014
3
359
C/2013 V4 (Catalina)
2016
9
360
C/2013 V5 (Oukaimeden)
2014
5
361
P/2013 W1 (PANSTARRS)
2013
1
362
C/2013 X1 (PANSTARRS)
2015
5
363
C/2013 Y2 (PANSTARRS)
2014
1
364
P/2014 A2 (Hill)
2014
1
365
C/2014 A4 (SONEAR)
2016
7
366
C/2014 AA52 (Catalina)
2014
1
367
C/2014 B1 (Schwartz)
08.04.2018
4
368
C/2014 C3 (NEOWISE)
2014
2
369
P/2014 D2 (Catalina-PANSTARRS)
2014
2
370
C/2014 E2 (Jacques)
2014
12
371
C/2014 F1 (Hill)
2014
1
372
C/2014 F2 (Tenagra)
2015
2
373
C/2014 G3 (PANSTARRS)
2014
1
374
C/2014 H1 (Christensen)
2014
1
375
P/2014 L2 (NEOWISE)
2014
4
376
P/2014 L3 (Hill)
2014
2
377
C/2014 M3 (Catalina)
2014
1
378
P/2014 M4 (PANSTARRS)
2014
1
379
P/2014 MG4 (Spacewatch-PANSTARRS)
2014
1
380
C/2014 N3 (NEOWISE)
2015
5
381
C/2014 OE4 (PANSTARRS)
12.07.2018
6
382
C/2014 Q1 (PANSTARRS)
2014
2
383
C/2014 Q2 (Lovejoy)
2016
16
384
C/2014 Q3 (Borisov)
2014
6
385
C/2014 R1 (Borisov)
2015
1
386
C/2014 R3 (PANSTARRS)
18.05.2018
3
387
C/2014 R4 (Gibbs)
2014
1
388
C/2014 S2 (PANSTARRS)
2016
11
389
C/2014 W2 (PANSTARRS)
2016
8
390
C/2014 W9 (PANSTARRS)
2015
1
391
C/2014 W11 (PANSTARRS)
2015
2
392
P/2014 X1 (Elenin)
2015
3
393
C/2014 Y1 (PANSTARRS)
2015
3
394
C/2015 C1 (TOTAS-GIBBS)
2015
2
395
C/2015 C2 (SWAN)
2015
2
396
P/2015 CD60 (LINEAR)
01.02.2025
1
397
C/2015 D3 (PANSTARRS)
2015
1
398
C/2015 ER61 (PANSTARRS)
2017
4
399
C/2015 F2 (Polonia)
2015
1
400
C/2015 F3 (SWAN)
2015
2
401
C/2015 F4 (Jacques)
2015
2
402
C/2015 F5 (SWAN-Xingming)
2015
3
403
C/2015 G2 (MASTER)
2015
1
404
C/2015 GX (PANSTARRS)
2015
1
405
C/2015 H2 (PANSTARRS)
11.09.2018
1
406
C/2015 K1 (MASTER)
2015
1
407
C/2015 LC2 (PANSTARRS)
2016
1
408
C/2015 M3 (PANSTARRS)
2015
1
409
C/2015 O1 (PANSTARRS)
01.07.2018
7
410
C/2015 T2 (PANSTARRS)
2017
1
411
C/2015 T4 (PANSTARRS)
2015
1
412
P/2015 TP200 (LINEAR)
2016
2
413
C/2015 V1 (PANSTARRS)
2017
4
414
C/2015 V2 (Johnson)
2017
21
415
C/2015 V3 (PANSTARRS)
2015
1
416
C/2015 VL62 (Lemmon-Yeung-PanSTARRS )
2017
6
417
C/2015 W1 (Gibbs)
2016
1
418
P/2015 W2 (Catalina)
2015
1
419
C/2015 WZ (PANSTARRS)
2016
3
420
C/2015 X4 (Elenin)
2015
1
421
C/2015 X7 (ATLAS)
2017
3
422
C/2015 X8 (NEOWISE)
2015
1
423
C/2015 XY1 (Lemmon)
06.02.2018
2
424
C/2015 Y1 (LINEAR)
2016
1
425
C/2015 YG1 (NEOWISE)
2016
1
426
C/2016 A1 (PANSTARRS)
06.04.2018
4
427
C/2016 A8 (LINEAR)
2016
5
428
P/2016 BA14 (PANSTARRS)
2016
1
429
C/2016 B1 (NEOWISE)
2017
1
430
C/2016 C1 (PANSTARRS)
2016
1
431
P/2016 G1 (PANSTARRS)
2016
1
432
C/2016 KA (Catalina)
2016
1
433
C/2016 K1 (LINEAR)
2016
2
434
C/2016 M1 (PANSTARRS)
21.05.2018
13
435
C/2016 N4 (Master)
20.05.2018
5
436
C/2016 N6 (PANSTARRS)
18.04.2018
8
437
P/2016 P2 (PANSTARRS)
2016
1
438
C/2016 Q2 (PANSTARRS)
31.05.2021
2
439
C/2016 Q4 (Kowalski)
2016
1
440
C/2016 R2 (PANSTARRS)
02.07.2019
11
441
C/2016 T1 (Matheny)
2016
1
442
C/2016 T2 (Matheny)
2016
2
443
C/2016 T3 (PANSTARRS)
06.02.2018
2
444
C/2016 U1 (NEOWISE)
2016
2
445
C/2016 VZ18 (PANSTARRS)
2017
5
446
C/2016 X1 (Lemmon)
2016
1
447
C/2017 AB5 (PANSTARRS)
06.02.2018
1
448
C/2017 D2 (Barros)
2017
1
449
C/2017 D3 (ATLAS)
19.02.2018
1
450
C/2017 E3 (PANSTARRS)
18.04.2018
2
451
C/2017 E4 (Lovejoy)
2017
1
452
C/2017 K2 (PANSTARRS)
18.12.2023
37
453
C/2017 K4 (ATLAS)
16.07.2018
2
454
C/2017 K6 (Jacques)
19.02.2018
1
455
C/2017 M4 (ATLAS)
05.08.2018
7
456
C/2017 M5 (TOTAS)
14.08.2018
3
457
C/2017 O1 (ASASSN)
06.04.2018
6
458
C/2017 S3 (PANSTARRS)
03.08.2018
15
459
P/2017 S5 (ATLAS)
2017
1
460
C/2017 S6 (Catalina)
2017
1
461
C/2017 S7 (Lemmon)
2017
1
462
C/2017 T1 (Heinze)
2017
2
463
C/2017 T2 (PANSTARRS)
26.05.2020
24
464
C/2017 T3 (ATLAS)
2017
1
465
C/2017 U7 (PANSTARRS)
01.09.2021
2
466
C/2017 W2 (Leonard)
06.02.2018
1
467
P/2017 W3 (Gibbs)
08.04.2018
1
468
C/2018 A1 (PANSTARRS)
06.02.2018
1
469
C/2018 A3 (ATLAS)
23.08.2019
2
470
C/2018 A6 (Gibbs)
04.04.2018
2
471
C/2018 B1 (Lemmon)
03.03.2018
1
472
P/2018 C1 (Lemmon-Read)
18.02.2018
1
473
C/2018 C2 (Lemmon)
08.04.2018
1
474
C/2018 DO4 (Lemmon)
27.10.2019
1
475
C/2018 EF9 (Lemmon)
20.05.2018
1
476
C/2018 F1 (Grauer)
07.04.2018
1
477
C/2018 F4 (PANSTARRS)
18.04.2018
1
478
P/2018 H2 (PANSTARRS)
02.06.2018
1
479
C/2018 K1 (Weiland)
20.06.2018
1
480
C/2018 KJ3 (Lemmon)
14.08.2018
1
481
C/2018 L2 (ATLAS)
04.12.2018
2
482
P/2018 L4 (PANSTARRS)
03.07.2018
1
483
P/2018 L5 (Leonard)
18.07.2018
1
484
C/2018 M1 (Catalina)
13.07.2018
1
485
C/2018 N1 (NEOWISE)
08.09.2018
3
486
C/2018 N2 (ASASSN)
30.11.2019
8
487
P/2018 P3 (PANSTARRS)
11.09.2018
1
488
P/2018 P4 (PANSTARRS)
04.09.2018
1
489
C/2018 P5 (PANSTARRS)
08.09.2018
1
490
C/2018 R3 (Lemmon)
07.04.2019
1
491
C/2018 U1 (Lemmon)
08.05.2021
6
492
C/2018 V1 (Machholz-Fujikawa-Iwamoto)
04.12.2018
1
493
C/2018 W2 (Africano)
03.09.2019
11
494
C/2018 X2 (Fitzsimmons)
07.03.2019
1
495
C/2018 Y1 (Iwamoto)
30.04.2019
5
496
P/2019 A2 (ATLAS)
29.03.2019
1
497
C/2019 B1 (Africano)
07.03.2019
1
498
P/2019 B2 (Groeller)
07.03.2019
1
499
C/2019 C1 (ATLAS)
22.03.2020
2
500
C/2019 D1 (Flewelling)
05.07.2019
6
501
C/2019 F1 (ATLAS-Africano)
19.04.2020
4
502
C/2019 F2 (ATLAS)
23.04.2019
1
503
C/2019 H1 (NEOWISE)
08.05.2019
1
504
C/2019 J2 (Palomar)
30.06.2019
2
505
C/2019 J3 (ATLAS)
02.07.2019
1
506
C/2019 K4 (Ye)
23.08.2019
4
507
C/2019 K5 (Young)
28.12.2019
3
508
A/2019 K6
16.04.2020
1
509
C/2019 K7 (Smith)
15.04.2021
5
510
C/2019 K8 (ATLAS)
31.08.2019
2
511
C/2019 L1 (PANSTARRS)
01.08.2019
1
512
C/2019 L2 (NEOWISE)
29.06.2019
1
513
C/2019 L3 (ATLAS)
20.03.2022
16
514
P/2019 LD2 (ATLAS)
07.09.2021
1
515
P/2019 LM4 (Palomar)
18.05.2020
2
516
P/2019 M2 (ATLAS)
01.08.2019
1
517
C/2019 M3 (ATLAS)
31.07.2019
1
518
C/2019 N1 (ATLAS)
15.05.2020
6
519
C/2019 O2 (PANSTARRS)
09.03.2024
1
520
C/2019 O3 (Palomar)
29.08.2022
5
521
2I/2019 Q4 (Borisov)
31.10.2019
1
522
C/2019 S4 (Lemmon)
01.04.2020
1
523
C/2019 T2 (Lemmon)
21.08.2020
2
524
C/2019 T3 (ATLAS)
02.09.2022
8
525
C/2019 T4 (ATLAS)
28.03.2023
3
526
P/2019 T6 (PANSTARRS)
30.11.2019
1
527
C/2019 U5 (PANSTARRS)
27.03.2023
11
528
C/2019 U6 (Lemmon)
05.11.2020
6
529
C/2019 V1 (Borisov)
30.11.2019
1
530
P/2019 X1 (Pruyne)
16.01.2020
1
531
C/2019 Y1 (ATLAS)
18.05.2020
22
532
P/2019 Y3 (Catalina)
01.02.2025
1
533
C/2019 Y4 (ATLAS)
15.05.2020
22
534
C/2020 A2 (Iwamoto)
19.03.2020
3
535
C/2020 B3 (Rankin)
22.03.2020
1
536
C/2020 F2 (ATLAS)
22.02.2023
3
537
C/2020 F3 (NEOWISE)
20.08.2020
7
538
C/2020 F5 (NEOWISE)
24.08.2022
2
539
C/2020 F8 (ATLAS)
19.05.2020
1
540
P/2020 G1 (PIMENTEL)
19.04.2020
1
541
C/2020 H2 (Pruyne)
11.05.2020
1
542
C/2020 H3 (Wierzchos)
19.05.2020
1
543
C/2020 H6 (ATLAS)
02.06.2022
7
544
C/2020 H7 (Lemmon)
28.05.2020
1
545
C/2020 H8 (PANSTARRS)
27.05.2020
1
546
C/2020 J1 (ATLAS)
07.03.2022
3
547
C/2020 K1 (PANSTARRS)
02.09.2022
12
548
C/2020 K3 (Leonard)
18.06.2020
1
549
C/2020 K7 (PANSTARRS)
21.07.2020
1
550
C/2020 K8 (Catalina-ATLAS)
19.06.2020
1
551
P/2020 K9 (Lemmon-PANSTARRS)
20.08.2020
1
552
C/2020 M3 (ATLAS)
14.11.2020
1
553
C/2020 M5 (ATLAS)
22.03.2022
5
554
C/2020 N1 (PANSTARRS)
06.11.2020
2
555
C/2020 O2 (Amaral)
08.08.2021
1
556
C/2020 P3 (ATLAS)
07.03.2021
2
557
C/2020 PV6 (PANSTARRS)
01.09.2021
3
558
C/2020 R2 (PANSTARRS)
05.09.2021
1
559
C/2020 R4 (ATLAS)
30.05.2021
6
560
C/2020 R7 (ATLAS)
27.02.2023
1
561
C/2020 S3 (Erasmus)
14.08.2021
1
562
C/2020 S4 (PANSTARRS)
18.01.2023
4
563
P/2020 S6 (Leonard)
14.11.2020
1
564
C/2020 S8 (Lemmon)
08.05.2021
5
565
C/2020 T2 (Palomar)
30.05.2021
8
566
P/2020 U2 (PANSTARRS)
07.03.2021
1
567
C/2020 U4 (PANSTARRS)
14.11.2022
4
568
C/2020 U5 (PANSTARRS)
21.08.2022
3
569
C/2020 V2 (ZTF)
24.08.2023
14
570
P/2020 V4 (Rankin)
19.02.2022
1
571
P/2020 WJ5 (Lemmon)
21.03.2023
1
572
C/2020 Y2 (ATLAS)
20.04.2021
1
573
C/2020 Y3 (ATLAS)
07.03.2021
1
574
C/2021 A1 (Leonard)
30.05.2021
3
575
C/2021 A2 (NEOWISE)
07.03.2021
1
576
C/2021 A4 (NEOWISE)
06.03.2021
1
577
C/2021 A9 (PANSTARRS)
27.03.2022
1
578
C/2021 C1 (Rankin)
08.03.2021
1
579
C/2021 C3 (Catalina)
08.03.2021
1
580
C/2021 D1 (SWAN)
30.03.2021
2
581
C/2021 D2 (ZTF)
23.02.2022
4
582
C/2021 E3 (ZTF)
03.09.2021
2
583
C/2021 F1 (Lemmon-PANSTARRS)
03.03.2022
2
584
C/2021 K1 (ATLAS)
04.09.2021
1
585
C/2021 L3 (Borisov)
09.03.2022
1
586
P/2021 N2 (Fuls)
08.09.2021
2
587
C/2021 O3 (PANSTARRS)
05.09.2021
3
588
C/2021 P4 (PANSTARRS)
02.06.2022
7
589
C/2021 Q3 (ATLAS)
01.09.2021
1
590
C/2021 Q4 (FULS)
05.09.2022
3
591
P/2021 Q5 (ATLAS)
08.09.2021
1
592
C/2021 QM45 (PANSTARRS)
06.09.2022
2
593
C/2021 S1 (ATLAS)
28.02.2022
2
594
C/2021 S3 (PANSTARRS)
05.08.2024
5
595
C/2021 S4 (Tsuchinshan)
10.01.2024
3
596
C/2021 T4 (Lemmon)
12.12.2022
3
597
C/2021 U5 (Catalina)
26.03.2022
1
598
P/2021 V2 (Fuls)
17.03.2023
1
599
C/2021 X1 (Maury-Attard)
07.09.2023
2
600
C/2021 Y1 (ATLAS)
17.12.2022
3
601
C/2022 A2 (PANSTARRS)
14.08.2023
4
602
C/2022 A3 (Lemmon-ATLAS)
19.01.2023
1
603
P/2022 C2 (PANSTARRS)
22.03.2022
2
604
P/2022 D1 (PANSTARRS)
27.03.2022
1
605
C/2022 E2 (ATLAS)
25.12.2024
10
606
C/2022 E3 (ZTF)
09.02.2023
15
607
C/2022 J2 (Bok)
17.12.2022
1
608
C/2022 L1 (Catalina)
28.08.2022
4
609
C/2022 L2 (ATLAS)
10.08.2023
3
610
P/2022 L3 (ATLAS)
12.12.2022
6
611
C/2022 N1 (Attard-Maury)
19.07.2022
1
612
C/2022 N2 (PANSTARRS)
03.11.2024
6
613
C/2022 P1 (NEOWISE)
03.09.2022
3
614
P/2022 P2 (ZTF)
05.09.2022
1
615
C/2022 P3 (ZTF)
08.02.2023
1
616
C/2022 Q2 (ATLAS)
14.11.2022
1
617
C/2022 QE78 (ATLAS)
19.01.2025
3
618
C/2022 R3 (Leonard)
16.12.2022
2
619
C/2022 S4 (Lemmon)
12.09.2023
2
620
C/2022 U1 (Leonard)
17.12.2023
3
621
C/2022 U2 (ATLAS)
09.02.2023
4
622
C/2022 U3 (Bok)
01.02.2025
3
623
C/2022 U4 (Bok)
27.03.2023
4
624
C/2022 W2 (ATLAS)
08.02.2023
1
625
C/2022 W3 (Leonard)
07.02.2023
1
626
C/2023 A1 (Leonard)
26.02.2023
2
627
C/2023 A3 (Tsuchinshan-ATLAS)
30.11.2024
14
628
P/2023 B1 (PANSTARRS)
27.03.2023
3
629
C/2023 E1 (ATLAS)
05.09.2023
5
630
C/2023 H2 (Lemmon)
10.09.2023
2
631
C/2023 H5 (Lemmon)
30.01.2025
6
632
C/2023 P1 (Nishimura)
09.09.2023
8
633
C/2023 Q1 (PANSTARRS)
25.12.2024
4
634
C/2023 Q2 (PANSTARRS)
15.06.2024
1
635
C/2023 R1 (PANSTARRS)
19.01.2025
5
636
C/2023 RN3 (ATLAS)
17.12.2023
1
637
P/2023 S1
01.02.2025
5
638
C/2023 S2 (ATLAS)
03.12.2023
1
639
C/2023 T2 (Borisov)
10.01.2024
2
640
C/2023 TD22 (Lemmon)
16.08.2024
3
641
C/2023 V4 (Camarasa-Duszanowicz)
25.08.2024
6
642
C/2023 X1 (Leonard)
18.12.2023
1
643
C/2023 X2 (Lemmon)
17.01.2025
2
644
C/2023 X4 (Hogan)
17.12.2023
1
645
C/2024 A1 (ATLAS)
18.01.2025
1
646
C/2024 A2 (ATLAS)
01.09.2024
1
647
C/2024 B1 (Lemmon)
04.11.2024
4
648
C/2024 C1 (PANSTARRS)
08.03.2024
1
649
C/2024 C2 (PANSTARRS)
08.03.2024
2
650
C/2024 C4 (ATLAS)
12.04.2024
1
651
C/2024 E1 (Wierzchos)
03.11.2024
5
652
C/2024 F2 (PANSTARRS)
12.04.2024
1
653
C/2024 G1 (Wierzchos)
04.06.2024
1
654
C/2024 G3 (ATLAS)
13.01.2025
1
655
C/2024 G4 (PANSTARRS)
24.06.2024
1
656
C/2024 J2 (Wierzchos)
17.01.2025
6
657
C/2024 J4 (Lemmon)
12.08.2024
2
658
C/2024 L1 (PANSTARRS)
08.07.2024
1
659
C/2024 M1 (ATLAS)
25.11.2024
1
660
P/2024 N2 (PANSTARRS)
16.07.2024
1
661
C/2024 N3 (Sarneczky)
26.12.2024
2
662
C/2024 N4 (Sarneczky)
25.12.2024
4
663
P/2024 T1 (Rankin)
26.12.2024
1
664
P/2024 T2 (Rankin)
30.11.2024
1
665
C/2024 V1 (Borisov)
26.01.2025
2
666
C/2024 X1 (Fazekas)
18.01.2025
1
667
C/2025 A3 (Tsuchinshan)
30.01.2025
1
668
C/2025 B1 (PANSTARRS)
29.01.2025
1