Engelhardsberg observatory


Comets By Designation (table is sortable)

info Nr. comet last observed thumbnail observations
  1 2P/Encke 2017

10

  2 4P/Faye 2015 4
  3 7P/Pons-Winnecke 2014 1
  4 9P/Tempel 2016 6
  5 10P/Tempel 2015 4
  6 14P/Wolf 2017 1
  7 15P/Finlay 2015 5
  8 16P/Brooks 2014 1
  9 17P/Holmes 2015 3
  10 19P/Borrelly 2016 1
  11 21P/Giacobini-Zinner 18.09.2018 32
  12 22P/Kopff 2016 5
  13 24P/Schaumasse 22.02.2018 4
  14 29P/Schwassmann-Wachmann 01.09.2019 7
  15 30P/Reinmuth 2017 2
  16 31P/Schwassmann-Wachmann 07.03.2019 1
  17 32P/Comas-Sola 2015 7
  18 33P/Daniel 2016 2
  19 36P/Whipple 28.08.2019 1
  20 37P/Forbes 20.08.2018 4
  21 38P/Stephan-Oterma 27.02.2019 6
  22 40P/Väisälä 2015 1
  23 41P/Tuttle-Giacobini-Kresak 2017 10
  24 43P/Wolf-Harrington 2016 2
  25 44P/Reinmuth 2014 1
  26 45P/Honda-Mrkos-Pajdusakova 2017 12
  27 46P/Wirtanen 07.03.2019 5
  28 47P/Ashbrook-Jackson 2017 4
  29 48P/Johnson 15.08.2018 5
  30 49P/Arend-Rigaux 29.03.2019 1
  31 50P/Arend 2015 1
  32 52P/Harrington/Abell 2014 3
  33 53P/van Biesbroeck 2016 4
  34 56P/Slaughter-Burnham 2016 4
  35 57P/du Toit-Neujmin-Delporte 2015 1
  36 59P/Kearns-Kwee 2017 1
  37 60P/Tsuchinshan 30.03.2019 2
  38 61P/Shajn-Schaldach 2015 1
  39 62P/Tsuchinshan 1 19.02.2018 3
  40 63P/Wild 2013 1
  41 64P/Swift-Gehrels 18.09.2018 12
  42 65P/Gunn 05.09.2018 3
  43 66P/du Toit 13.08.2018 1
  44 67P/Churyumov-Gerasimenko 2016 2
  45 68P/Klemola 26.08.2019 5
  46 70P/Kojima 2015 3
  47 71P/Clark 2017 2
  48 73P/Schwassmann-Wachmann 3 2017 2
  49 74P/Smirnova-Chernykh 06.04.2018 5
  50 76P/West-Kohoutek-Ikemura 04.12.2019 1
  51 77P/Longmore 2016 3
52 78P/Gehrels 2 01.01.2020 5
  53 81P/Wild 2016 9
  54 84P/Giclas 2014 2
  55 88P/Howell 30.12.2019 2
  56 89P/Russell 2016 1
  57 90P/Gehrels 1 2017 1
  58 93P/Lovas 1 2017 3
  59 94P/Russell 2017 1
  60 95P/Chiron 2016 3
  61 98P/Takamizawa 2013 2
62 99P/Kowal 1 16.01.2020 1
  63 101P/Chernykh 30.11.2019 3
  64 102P/Shoemaker 2013 3
  65 103P/Hartley 2 08.04.2018 1
  66 104P/Kowal 2 2016 2
  67 105P/Singer Brewster 08.04.2018 2
  68 106P/Schuster 2014 1
  69 108P/Ciffreo 2014 4
  70 110P/Hartley 2014 2
71 112P/Urata-Niijima 15.01.2020 1
72 114P/Wiseman-Skiff 01.01.2020 4
  73 116P/Wild 2016 3
  74 117P/Helin-Roman-Alu 1 2016 3
  75 118P/Shoemaker-Levy 4 2015 1
  76 119P/Parker-Hartley 2015 2
  77 123P/West-Hartley 07.05.2019 6
  78 124P/Mrkos 05.12.2019 4
  79 125P/Spacewatch 2013 1
  80 128P/Shoemaker-Holt 1 2016 1
  81 129P/Shoemaker-Levy 14.08.2018 4
  82 130P/McNaught-Hughes 13.08.2018 2
  83 131P/Mueller 05.09.2018 1
  84 133P/Elst-Pizzaro 02.09.2019 1
  85 134P/Kowal-Vavrova 2014 6
  86 136P/Mueller 2016 1
  87 137P/Shoemaker-Levy 14.08.2018 4
  88 139P/Vaisala-Oterma 2017 2
  89 141P/Machholz 2015 1
  90 143P/Kowal-Mrkos 08.04.2018 1
  91 144P/Kushida 2016 2
  92 145P/Shoemaker-Levy 2017 1
  93 146P/Shoemaker-LINEAR 2016 1
  94 149P/Mueller 29.03.2019 1
  95 150P/Smirnova-Chernykh 2015 1
  96 154P/Brewington 2014 8
  97 155P/Shoemaker 30.12.2019 1
  98 157P/Tritton 2017 1
  99 158P/Kowal-LINEAR 2013 1
  100 159P/LONEOS 2017 1
  101 160P/LINEAR 31.10.2019 1
  102 162P/Siding Spring 2016 1
  103 164P/Christensen 27.02.2019 1
  104 170P/Christensen 2014 2
  105 171P/Spahr 18.09.2018 1
  106 172P/Yeung 2016 1
  107 173P/Mueller 28.12.2019 2
  108 174P/Echeclus 2016 2
  109 176P/LINEAR 2016 1
  110 178P/Hug-Bell 2014 3
  111 180P/NEAT 2016 2
  112 183P/Korlevic-Juric 06.04.2018 1
  113 184P/Lovas 2013 1
  114 185P/Petriew 06.04.2018 2
  115 187P/LINEAR 19.04.2018 1
  116 188P/LINEAR-Mueller 2017 2
  117 191P/McNaught 2014 1
  118 194P/Kowal 2016 1
  119 200P/Larsen 02.08.2018 1
  120 201P/LONEOS 2015 2
  121 203P/Korlevic 30.11.2019 2
  122 204P/LINEAR-NEAT 2015 1
  123 205P/Giacobini 2015 1
  124 208P/McMillan 2016 1
  125 209P/LINEAR 2014 8
  126 211P/Hill 2016 2
  127 213P/Van Ness 2017 1
  128 217P/LINEAR 2017 2
  129 218P/LINEAR 2015 2
  130 219P/LINEAR 2016 2
  131 221P/LINEAR 2015 1
  132 223P/Skiff 11.09.2018 2
  133 226P/Pigott-LINEAR-Kowalski 2016 3
134 228P/LINEAR 01.01.2020 1
  135 230P/LINEAR 2015 1
  136 231P/LINEAR 31.03.2019 2
  137 235P/LINEAR 04.04.2018 1
  138 236P/LINEAR 2017 2
  139 237P/LINEAR 2016 1
  140 238P/Read 2016 1
  141 239P/LINEAR 06.04.2019 1
  142 240P/NEAT 27.02.2019 1
  143 243P/NEAT 06.08.2018 1
  144 244P/Scotti 2014 1
  145 245P/WISE 14.08.2018 2
  146 246P/NEAT 30.12.2019 3
  147 247P/LINEAR 27.02.2019 1
  148 249P/LINEAR 2015 2
  149 250P/Larson 21.02.2018 1
  150 252P/LINEAR 2016 3
  151 257P/Catalina 2013 4
  152 260P/McNaught 26.10.2019 7
  153 261P/Larson 03.09.2019 3
  154 266P/Christensen 28.12.2019 3
  155 269P/Jedicke 2015 3
  156 270P/Gehrels 2014 1
  157 273P/Pons-Gambart 2013 1
  158 279P/La Sagra 2016 1
  159 284P/McNaught 2014 1
  160 288P 2016 1
161 289P/Blanpain 16.01.2020 2
  162 290P/Jager 2014 5
  163 291P/NEAT 2013 2
  164 292P/Li 2013 1
  165 293P/Spacewatch 2014 2
  166 294P/LINEAR 2014 1
  167 296P/Garradd 2014 2
  168 297P/Beshore 2014 2
  169 299P/Catalina-PANSTARRS 2016 1
  170 302P/Lemmon-PANSTARRS 2016 1
  171 303P/NEAT 2014 1
  172 305P/Skiff 2014 2
  173 307P/LINEAR 2014 1
  174 314P/Montani 2015 1
  175 315P/LONEOS 2017 5
  176 318P/McNaught-Hartley 2015 1
  177 327P/Van Ness 2015 1
  178 328P/LONEOS-Tucker 2015 1
  179 329P/LINEAR-Catalina 2015 1
  180 330P/Catalina 2016 1
  181 332P/Ikeya-Murakami 2016 2
  182 333P/LINEAR 2016 2
  183 334P/NEAT 20.05.2018 1
  184 337P/WISE 2016 1
  185 338P/McNaught 2016 1
  186 340P/Boattini 2016 1
  187 341P/Gibbs 2016 1
  188 343P/NEAT-LONEOS 2016 2
  189 344P/Read 2016 1
  190 345P/LINEAR 2016 1
  191 346P/Catalina 2016 1
  192 347P/PANSTARRS 2016 1
  193 349P/Lemmon 2017 1
  194 352P/Skiff 2017 2
  195 355P/LINEAR-NEAT 2017 2
  196 356P/WISE 2017 1
  197 360P/WISE 2017 1
  198 361P/Spacewatch 2017 2
  199 362P/(457175) 2017 1
  200 364P/PANSTARRS 21.02.2018 2
  201 365P/LINEAR 04.04.2018 1
  202 366P/LINEAR 07.04.2018 1
  203 368P/NEAT 15.09.2018 3
  204 369P/Hill 12.09.2018 1
  205 370P/NEAT 18.09.2018 1
  206 371P/LINEAR-Skiff 12.09.2018 1
  207 373P/Rinner 06.04.2019 1
  208 375P/Hill 31.03.2019 2
  209 376P/Loneos 30.04.2019 3
  210 379P/Spacewatch 23.04.2019 2
  211 380P/PANSTARRS 30.04.2019 1
  212 384P/Kowalski 28.12.2019 3
  213 385P/Hill 30.11.2019 1
214 390P/Gibbs 16.01.2020 1
  215 392P/LINEAR 30.11.2019 1
  216 6478 Gault (comet like asteroid) 30.03.2019 1
  217 C/2006 S3 (Loneos) 2015 6
  218 C/2006 W3 (Christensen) 2009 1
  219 C/2007 Q3 (SidingSpring) 2010 1
  220 C/2008 S3 (Boattini) 2014 2
  221 C/2009 F4 (McNaught) 2014 1
  222 C/2009 K5 (McNaught) 2010 1
  223 C/2010 S1 (LINEAR) 2014 7
  224 C/2010 U3 (Boattini) 27.02.2019 3
  225 C/2011 J2 (LINEAR) 2015 13
  226 C/2011 KP36 (Spacewatch) 2016 5
  227 C/2011 L4 (PANSTARRS) 2014 13
  228 C/2011 R1 (McNaught) 2013 4
  229 C/2012 A1 (PANSTARRS) 2013 1
  230 C/2012 A2 (Linear) 2013 2
  231 P/2012 B1 (PANSTARRS) 2014 1
  232 P/2012 F2 (PANSTARRS) 2013 1
  233 C/2012 F3 (PANSTARRS) 2015 3
  234 C/2012 F6 (Lemmon) 2014 9
  235 C/2012 J1 (Catalina) 2014 3
  236 C/2012 K1 (PANSTARRS) 2014 17
  237 C/2012 K6 (McNaught) 2014 5
  238 C/2012 K8 (Lemmon) 2014 3
  239 C/2012 LP26 (Palomar) 2016 4
  240 C/2012 S1 (ISON) 2013 2
  241 C/2012 S3 (PANSTARRS) 2013 4
  242 C/2012 S4 (PANSTARRS) 2013 1
  243 C/2012 U1 (PANSTARRS) 2013 1
  244 C/2012 X1 (LINEAR) 2014 6
  245 C/2013 A1 (Siding Spring) 2015 2
  246 C/2013 C2 (Tenagra) 2014 2
  247 C/2013 E1 (McNaught) 2014 1
  248 C/2013 E2 (Iwamoto) 2013 2
  249 C/2013 F2 (Catalina) 2014 2
  250 C/2013 F3 (McNaught) 2013 1
  251 C/2013 G1 (Kowalski) 2014 1
  252 C/2013 G3 (PANSTARRS) 2014 3
  253 C/2013 G5 (Catalina) 2013 1
  254 C/2013 G8(PANSTARRS) 2014 1
  255 C/2013 G9(Tenagra) 2014 1
  256 C/2013 H1(La Sagra) 2013 1
  257 C/2013 H2(Boattini) 2014 1
  258 P/2013 J2 (McNaught) 2013 5
  259 P/2013 O2 (PANSTARRS) 2013 1
  260 C/2013 P2 (PANSTARRS) 2014 1
  261 C/2013 P3 (Palomar) 2014 1
  262 C/2013 P4 (PANSTARRS) 2014 1
  263 C/2013 R1 (Lovejoy) 2014 11
  264 P/2013 R3 (Catalina-PANSTARRS) 2013 2
  265 P/2013 T2 (Schwartz) 2013 1
  266 P/2013 TL117 2014 1
  267 C/2013 TW5 2015 4
  268 C/2013 U1 (Catalina) 2013 1
  269 C/2013 U2 (Holvorcem) 2015 3
  270 C/2013 UQ4 (Catalina) 2014 9
  271 C/2013 US10 (Catalina) 2016 10
  272 C/2013 V1 (Boattini) 2014 8
  273 C/2013 V2 (Borisov) 2015 6
  274 C/2013 V3 (Nevski) 2014 3
  275 C/2013 V4 (Catalina) 2016 9
  276 C/2013 V5 (Oukaimeden) 2014 5
  277 P/2013 W1 (PANSTARRS) 2013 1
  278 C/2013 X1 (PANSTARRS) 2015 5
  279 C/2013 Y2 (PANSTARRS) 2014 1
  280 P/2014 A2 (Hill) 2014 1
  281 C/2014 A4 (SONEAR) 2016 7
  282 C/2014 AA52 (Catalina) 2014 1
  283 C/2014 B1 (Schwartz) 08.04.2018 4
  284 C/2014 C3 (NEOWISE) 2014 2
  285 P/2014 D2 (Catalina-PANSTARRS) 2014 2
  286 P/2014 E1 (Larson) 2014 1
  287 C/2014 E2 (Jacques) 2014 12
  288 C/2014 F1 (Hill) 2014 1
  289 C/2014 F2 (Tenagra) 2015 2
  290 C/2014 G3 (PANSTARRS) 2014 1
  291 C/2014 H1 (Christensen) 2014 1
  292 P/2014 L2 (NEOWISE) 2014 4
  293 P/2014 L3 (Hill) 2014 2
  294 C/2014 M3 (Catalina) 2014 1
  295 P/2014 M4 (PANSTARRS) 2014 1
  296 P/2014 MG4 (Spacewatch-PANSTARRS) 2014 1
  297 C/2014 N3 (NEOWISE) 2015 5
  298 C/2014 OE4 (PANSTARRS) 12.07.2018 6
  299 C/2014 Q1 (PANSTARRS) 2014 2
  300 C/2014 Q2 (Lovejoy) 2016 16
  301 C/2014 Q3 (Borisov) 2014 6
  302 C/2014 R1 (Borisov) 2015 1
  303 C/2014 R3 (PANSTARRS) 18.05.2018 3
  304 C/2014 R4 (Gibbs) 2014 1
  305 C/2014 S2 (PANSTARRS) 2016 11
  306 C/2014 W2 (PANSTARRS) 2016 8
  307 C/2014 W9 (PANSTARRS) 2015 1
  308 C/2014 W11 (PANSTARRS) 2015 2
  309 P/2014 X1 (Elenin) 2015 3
  310 C/2014 Y1 (PANSTARRS) 2015 3
  311 C/2015 C1 (TOTAS-GIBBS) 2015 2
  312 C/2015 C2 (SWAN) 2015 2
  313 C/2015 D3 (PANSTARRS) 2015 1
  314 C/2015 ER61 (PANSTARRS) 2017 4
  315 C/2015 F2 (Polonia) 2015 1
  316 C/2015 F3 (SWAN) 2015 2
  317 C/2015 F4 (Jacques) 2015 2
  318 C/2015 F5 (SWAN-Xingming) 2015 3
  319 C/2015 G2 (MASTER) 2015 1
  320 C/2015 GX (PANSTARRS) 2015 1
  321 C/2015 H2 (PANSTARRS) 11.09.2018 1
  322 C/2015 K1 (MASTER) 2015 1
  323 C/2015 LC2 (PANSTARRS) 2016 1
  324 C/2015 M3 (PANSTARRS) 2015 1
  325 C/2015 O1 (PANSTARRS) 01.07.2018 7
  326 C/2015 T2 (PANSTARRS) 2017 1
  327 C/2015 T4 (PANSTARRS) 2015 1
  328 P/2015 TP200 (LINEAR) 2016 2
  329 C/2015 V1 (PANSTARRS) 2017 4
  330 C/2015 V2 (Johnson) 2017 21
  331 C/2015 V3 (PANSTARRS) 2015 1
  332 C/2015 VL62 (Lemmon-Yeung-PanSTARRS ) 2017 6
  333 C/2015 W1 (Gibbs) 2016 1
  334 P/2015 W2 (Catalina) 2015 1
  335 C/2015 WZ (PANSTARRS) 2016 3
  336 C/2015 X4 (Elenin) 2015 1
  337 C/2015 X7 (ATLAS) 2017 3
  338 C/2015 X8 (NEOWISE) 2015 1
  339 C/2015 XY1 (Lemmon) 06.02.2018 2
  340 C/2015 Y1 (LINEAR) 2016 1
  341 C/2015 YG1 (NEOWISE) 2016 1
  342 C/2016 A1 (PANSTARRS) 06.04.2018 4
  343 C/2016 A8 (LINEAR) 2016 5
  344 P/2016 BA14 (PANSTARRS) 2016 1
  345 C/2016 B1 (NEOWISE) 2017 1
  346 C/2016 C1 (PANSTARRS) 2016 1
  347 P/2016 G1 (PANSTARRS) 2016 1
  348 C/2016 KA (Catalina) 2016 1
  349 C/2016 K1 (LINEAR) 2016 2
  350 C/2016 M1 (PANSTARRS) 21.05.2018 13
  351 C/2016 N4 (Master) 20.05.2018 5
  352 C/2016 N6 (PANSTARRS) 18.04.2018 8
  353 P/2016 P2 (PANSTARRS) 2016 1
  354 C/2016 Q2 (PANSTARRS) 2016 1
  355 C/2016 Q4 (Kowalski) 2016 1
  356 C/2016 R2 (PANSTARRS) 02.07.2019 11
  357 C/2016 T1 (Matheny) 2016 1
  358 C/2016 T2 (Matheny) 2016 2
  359 C/2016 T3 (PANSTARRS) 06.02.2018 2
  360 C/2016 U1 (NEOWISE) 2016 2
  361 C/2016 VZ18 (PANSTARRS) 2017 5
  362 C/2016 X1 (Lemmon) 2016 1
  363 C/2017 AB5 (PANSTARRS) 06.02.2018 1
  364 C/2017 D2 (Barros) 2017 1
  365 C/2017 D3 (ATLAS) 19.02.2018 1
  366 C/2017 E3 (PANSTARRS) 18.04.2018 2
  367 C/2017 E4 (Lovejoy) 2017 1
  368 C/2017 K2 (PANSTARRS) 31.10.2019 14
  369 C/2017 K4 (ATLAS) 16.07.2018 2
  370 C/2017 K6 (Jacques) 19.02.2018 1
  371 C/2017 M4 (ATLAS) 05.08.2018 7
  372 C/2017 M5 (TOTAS) 14.08.2018 3
  373 C/2017 O1 (ASASSN) 06.04.2018 6
  374 C/2017 S3 (PANSTARRS) 03.08.2018 15
  375 P/2017 S5 (ATLAS) 2017 1
  376 C/2017 S6 (Catalina) 2017 1
  377 C/2017 S7 (Lemmon) 2017 1
  378 C/2017 T1 (Heinze) 2017 2
379 C/2017 T2 (PANSTARRS) 15.01.2020 12
  380 C/2017 T3 (ATLAS) 2017 1
  381 C/2017 W2 (Leonard) 06.02.2018 1
  382 P/2017 W3 (Gibbs) 08.04.2018 1
  383 C/2018 A1 (PANSTARRS) 06.02.2018 1
  384 C/2018 A3 (ATLAS) 23.08.2019 2
  385 C/2018 A6 (Gibbs) 04.04.2018 2
  386 C/2018 B1 (Lemmon) 03.03.2018 1
  387 P/2018 C1 (Lemmon-Read) 18.02.2018 1
  388 C/2018 C2 (Lemmon) 08.04.2018 1
  389 C/2018 DO4 (Lemmon) 27.10.2019 1
  390 C/2018 EF9 (Lemmon) 20.05.2018 1
  391 C/2018 F1 (Grauer) 07.04.2018 1
  392 C/2018 F4 (PANSTARRS) 18.04.2018 1
  393 P/2018 H2 (PANSTARRS) 02.06.2018 1
  394 C/2018 K1 (Weiland) 20.06.2018 1
  395 C/2018 KJ3 (Lemmon) 14.08.2018 1
  396 C/2018 L2 (ATLAS) 04.12.2018 2
  397 P/2018 L4 (PANSTARRS) 03.07.2018 1
  398 P/2018 L5 (Leonard) 18.07.2018 1
  399 C/2018 M1 (Catalina) 13.07.2018 1
  400 C/2018 N1 (NEOWISE) 08.09.2018 3
  401 C/2018 N2 (ASASSN) 30.11.2019 8
  402 P/2018 P3 (PANSTARRS) 11.09.2018 1
  403 P/2018 P4 (PANSTARRS) 04.09.2018 1
  404 C/2018 P5 (PANSTARRS) 08.09.2018 1
  405 C/2018 R3 (Lemmon) 07.04.2019 1
  406 C/2018 U1 (Lemmon) 31.10.2019 3
  407 C/2018 V1 (Machholz-Fujikawa-Iwamoto) 04.12.2018 1
  408 C/2018 W2 (Africano) 03.09.2019 11
  409 C/2018 X2 (Fitzsimmons) 07.03.2019 1
  410 C/2018 Y1 (Iwamoto) 30.04.2019 5
  411 P/2019 A2 (ATLAS) 29.03.2019 1
  412 C/2019 B1 (Africano) 07.03.2019 1
  413 P/2019 B2 (Groeller) 07.03.2019 1
  414 C/2019 D1 (Flewelling) 05.07.2019 6
  415 C/2019 F1 (ATLAS-Africano) 30.04.2019 2
  416 C/2019 F2 (ATLAS) 23.04.2019 1
  417 C/2019 H1 (NEOWISE) 08.05.2019 1
  418 C/2019 J2 (Palomar) 30.06.2019 2
  419 C/2019 J3 (ATLAS) 02.07.2019 1
  420 C/2019 K4 (Ye) 23.08.2019 4
  421 C/2019 K5 (Young) 28.12.2019 3
  422 C/2019 K8 (ATLAS) 31.08.2019 2
  423 C/2019 L1 (PANSTARRS) 01.08.2019 1
  424 C/2019 L2 (NEOWISE) 29.06.2019 1
425 C/2019 L3 (ATLAS) 16.01.2020 4
  426 P/2019 M2 (ATLAS) 01.08.2019 1
  427 C/2019 M3 (ATLAS) 31.07.2019 1
  428 C/2019 N1 (ATLAS) 08.08.2019 2
  429 2I/2019 Q4 (Borisov) 31.10.2019 1
430 C/2019 T3 (ATLAS) 16.01.2020 2
  431 P/2019 T6 (PANSTARRS) 30.11.2019 1
  432 C/2019 V1 (Borisov) 30.11.2019 1
433 P/2019 X1 (Pruyne) 16.01.2020 1
434 C/2019 Y1 (ATLAS) 16.01.2020 2
435 C/2019 Y4 (ATLAS) 16.01.2020 1