Skip to main content
NASA Author Manuscripts logoLink to NASA Author Manuscripts
. Author manuscript; available in PMC: 2020 May 26.
Published in final edited form as: Minor Planet Bull. 2013 Jul-Sep;40(3):180–184.

LIGHTCURVE PHOTOMETRY OPPORTUNITIES: 2013 JULY-SEPTEMBER

Brian D Warner 1, Alan W Harris 2, Petr Pravec 3, Josef Ďurech 4, Lance AM Benner 5
PMCID: PMC7249727  NIHMSID: NIHMS1569912  PMID: 32457951

Abstract

We present lists of asteroid photometry opportunities for objects reaching a favorable apparition and have no or poorly-defined lightcurve parameters. Additional data on these objects will help with shape and spin axis modeling via lightcurve inversion. We also include lists of objects that will be the target of radar observations. Lightcurves for these objects can help constrain pole solutions and/or remove rotation period ambiguities that might not come from using radar data alone.


We present lists of “targets of opportunity” for the period 2013 July-September. For background on the program details for each of the opportunity lists, refer to previous issues, e.g., Minor Planet Bulletin 36, 188. In the first three sets of tables, “Dec” is the declination and “U” is the quality code of the lightcurve. See the asteroid lightcurve data base (LCDB) documentation for an explanation of the U code:

http://www.minorplanet.info/lightcurvedatabase.html

Objects with U = 1 should be given higher priority over those rated U = 2 or 2+ but not necessarily over those with no period. On the other hand, do not overlook asteroids with U = 2/2+ on the assumption that the period is sufficiently established. Regardless, do not let the existing period influence your analysis since even high quality ratings have been proven wrong at times. Note that the lightcurve amplitude in the tables could be more or less than what’s given. Use the listing only as a guide.

The first list is an abbreviated list of those asteroids reaching V < 15.0 at brightest during the period and have either no or poorly-constrained lightcurve parameters. An asterisk (*) follows the name if the asteroid is reaching a particularly favorable apparition.

The goal for these asteroids is to find a well-determined rotation rate. The target list generator on the CALL web site allows you to create custom lists for objects reaching V ≤ 18.0 during any month in the current year, e.g., limiting the results by magnitude and declination.

http://www.minorplanet.info/PHP/call_OppLCDBQuery.php

In a general note, small objects with periods up to 4 hours or even longer are possible binaries. For longer periods (4–6 hours or so), the odds of a binary may be less, but the bonus is that the size of the secondary, if it exists, is likely larger (see Pravec et al. (2010), Nature 466, 1085–1088), thus eclipses, if they occur, will be deeper and easier to detect.

The Low Phase Angle list includes asteroids that reach very low phase angles. The “α” column is the minimum solar phase angle for the asteroid. Getting accurate, calibrated measurements (usually V band) at or very near the day of opposition can provide important information for those studying the “opposition effect.” You will have the best chance of success working objects with low amplitude and periods that allow covering, e.g., a maximum, every night. Objects with large amplitudes and/or long periods are much more difficult for phase angle studies since, for proper analysis, the data have to be reduced to the average magnitude of the asteroid for each night. Without knowing the period and/or the amplitude at the time, that reduction becomes highly uncertain. As an aside, some use the maximum light to find the phase slope parameter (G). However, this can produce a significantly different value for both H and G versus using average light, which is the method used for values listed by the Minor Planet Center.

The third list is of those asteroids needing only a small number of lightcurves to allow spin axis and/or shape modeling. Those doing work for modeling should contact Josef Ďurech at the email address above and/or visit the Database of Asteroid Models from Inversion Techniques (DAMIT) web site for existing data and models:

http://astro.troja.mff.cuni.cz/projects/asteroids3D

The fourth list gives a brief ephemeris for planned radar targets. Supporting optical observations to determine the lightcurve period, amplitude, and shape are needed to supplement the radar data. High-precision work, 0.01–0.02 mag, is preferred, especially if the object is a known or potential binary. Those obtaining lightcurves in support of radar observations should contact Dr. Benner directly at the email given above.

Future radar targets

http://echo.jpl.nasa.gov/~lance/future.radar.nea.periods.html

Past radar targets

http://echo.jpl.nasa.gov/~lance/radar.nea.periods.html

Arecibo targets

http://www.naic.edu/~pradar/sched.shtml

http://www.naic.edu/~pradar

Goldstone targets

http://echo.jpl.nasa.gov/asteroids/goldstone_asteroid_schedule.html

As always, we encourage observations of asteroids even if they have well-established lightcurve parameters and especially if they are lacking good spin axis and/or shape model solutions. Every lightcurve of sufficient quality supports efforts to resolve a number of questions about the evolution of individual asteroids and the general population. For example, pole directions are known for only about 30 NEAs out of a population of 8000. This is hardly sufficient to make even the most general of statements about NEA pole alignments, including whether or not the thermal YORP effect is forcing pole orientations into a limited number of preferred directions (see La Spina et al., 2004, Nature 428, 400–401). Data from many apparitions can help determine if an asteroid’s rotation rate is being affected by YORP, which can also cause the rotation rate of a smaller, irregularly-shaped asteroid to increase or decrease. See Lowry et al. (2007) Science 316, 272–274 and Kaasalainen et al. (2007) Nature 446, 420–422.

The ephemeris listings for the optical-radar listings include lunar elongation and phase. Phase values range from 0.0 (new) to 1.0 (full). If the value is positive, the moon is waxing – between new and full. If the value is negative, the moon is waning – between full and new. The listing also includes the galactic latitude. When this value is near 0°, the asteroid is likely in rich star fields and so may be difficult to work. It is important to emphasize that the ephemerides that we provide are only guides for when you might observe a given asteroid. Obviously, you should use your discretion and experience to make your observing program as effective as possible.

Once you’ve analyzed your data, it’s important to publish your results. Papers appearing in the Minor Planet Bulletin are indexed in the Astrophysical Data System (ADS) and so can be referenced by others in subsequent papers. It’s also important to make the data available at least on a personal website or upon request.

Funding for Warner and Harris in support of this article is provided by NASA grant NNX10AL35G and by National Science Foundation grant AST-1032896.

Lightcurve Opportunities

Brightest LCDB Data
# Name Date Mag Dec Period Amp U
458 Hercynia 07 01.3 14.4 −12 22.3 0.33–0.35 2
618 Elfriede* 07 02.2 12.3 −18 14.801 0.12–0.20 2
1228 Scabiosa 07 02.3 15.0 −25
6271 Farmer* 07 03.2 14.7 −28 250. 0.13–0.22 2
29742 1999 BQ12* 07 08.8 14.9 −26 4.3 0.7 1+
10731 1988 BL3 07 09.3 15.0 −18 28.02 0.23–0.41 2
1409 Isko 07 11.7 14.7 −12 11.6426 0.20 2
961 Gunnie 07 11.9 14.7 −40
3977 Maxine* 07 11.9 14.6 +0
1159 Granada 07 12.1 14.4 −42 31. 0.28 2
1886 Lowell* 07 12.2 14.7 −35
6307 Maiztegui 07 12.6 14.9 −20 4.68 0.15 2
1686 De Sitter* 07 12.7 14.2 −23
576 Emanuela* 07 12.8 12.2 −25 8.192 0.05–0.06 2−
2543 Machado* 07 13.1 14.1 −47 31.72 0.15 2
589 Croatia 07 13.6 13.5 −7 11.7 0.16 2
4226 Damiaan 07 13.6 14.2 −13 24. 0.05 1
2104 Toronto 07 14.3 14.5 −4 8.9669 0.32 2+
6032 Nobel 07 14.7 14.9 −6
455 Bruchsalia 07 14.9 11.1 −35 11.838 0.10–0.35 2+
1753 Mieke 07 15.2 14.8 −36 8.8 0.2 2
916 America 07 15.6 13.8 −35 38. 0.28 1
741 Botolphia 07 16.5 13.6 −24 23.93 0.12– 0.4 2−
1043 Beate 07 16.7 13.7 −12 44.3 0.47 2+
866 Fatme* 07 18.8 13.6 −26 20.03 0.06–0.21 2
1629 Pecker* 07 19.1 14.2 −15 8.2166 0.08 2
6914 Becquerel 07 19.4 14.8 −24
859 Bouzareah 07 19.6 14.6 −40 23.2 0.13 2−
421 Zahringia 07 19.7 15.0 −9 6.42 0.07–0.12 2
722 Frieda* 07 20.1 13.7 −32 0.04
1145 Robelmonte 07 20.3 13.7 −29 9.01 0.05–0.18 2
1646 Rosseland 07 20.6 14.4 −20 69.2 0.13 2
582 Olympia 07 20.7 14.0 +8 36. 0.05– 0.6 2
9938 Kretlow* 07 20.8 15.0 −25
6386 Keithnoll 07 22.2 14.1 −20 3.1381 0.08 2+
874 Rotraut 07 22.9 14.7 −5 14.586 0.24 2
862 Franzia 07 24.1 13.5 −20 7.52 0.07–0.22 2
481 Emita 07 24.6 12.7 −32 14.35 0.09–0.30 2
1186 Turnera 07 25.2 13.1 −36 12.066 0.25–0.34 2+
1351 Uzbekistania 07 26.7 14.6 −32 73.9 0.20–0.34 2
2829 Bobhope* 07 27.0 13.8 −28 6.0888 0.50–0.55 2
7536 Fahrenheit* 07 27.0 14.6 −19
305 Gordonia 07 28.7 13.9 −13 16.2 0.16–0.17 2
931 Whittemora 07 30.5 13.9 −23 19.2 0.2 2
1952 Hesburgh 08 01.4 14.9 −34 47.7 0.18 2
1799 Koussevitzky 08 02.5 14.8 −10 6.325 0.25 2
3002 Delasalle 08 02.5 14.4 −21
2437 Amnestia 08 02.8 14.6 −12 85. 0.45 2
1042 Amazone 08 02.9 14.4 −46 540. 0.10–0.25 2
569 Misa 08 03.9 13.9 −17 13.52 0.25 2
1073 Gellivara* 08 04.0 14.8 −20 11.32 0.35 2
4333 Sinton* 08 04.3 14.7 −15
2138 Swissair 08 05.9 14.5 −21
17939 1999 HH8* 08 06.5 14.9 −19 5.1 0.18–0.26 2
6495 1992 UB1 08 10.1 14.9 −3 5.697 0.29–0.45 2
52760 1998 ML14* 08 12.4 15.0 −31 14.98 0.12 2
503 Evelyn 08 13.5 13.5 −21 38.7 0.30– 0.5 2
1337 Gerarda 08 13.7 14.8 −5 12.52 0.23 2
1315 Bronislawa 08 14.1 14.3 −4 9.565 0.16–0.24 2
3581 Alvarez* 08 14.1 14.3 +38 33.42 0.06 2
823 Sisigambis 08 16.4 13.9 −8 146. 0.05– 0.7 2
2873 Binzel 08 16.6 14.8 −21
570 Kythera 08 20.2 13.0 −10 8.12 0.15–0.18 2
1358 Gaika* 08 20.2 14.2 −16
1372 Haremari* 08 20.3 14.3 −12 15.25 0.12 2
581 Tauntonia 08 20.6 14.6 −33 16.54 0.07–0.20 2
1683 Castafiore* 08 21.6 13.9 −11 13.931 0.66 2+
1048 Feodosia 08 22.4 13.6 −33 10.46 0.14 2
19082 Vikchernov* 08 22.4 14.9 −12
1290 Albertine 08 22.7 14.9 −8
5847 Wakiya* 08 25.3 14.5 −1 23.95 0.10 1
11574 d’Alviella* 08 25.5 14.7 −17 12.549 0.15 2
3768 Monroe* 08 25.7 14.4 −12
2089 Cetacea 08 26.5 13.9 −30 39.12 0.25–0.40 2
774 Armor 08 29.7 12.3 −1 25.107 0.11–0.34 2
8992 Magnanimity* 08 29.7 14.7 −1
1714 Sy 08 29.8 14.8 −1 0.95
702 Alauda 08 30.0 11.9 +13 8.348 0.07–0.10 2
1486 Marilyn* 08 30.2 14.0 −9 2.2837 0.40 1+
2430 Bruce Helin 08 30.2 14.2 −53 128. 0.6 2
3300 McGlasson 08 30.2 14.1 −30 22.91 0.16 2
1149 Volga 08 31.4 14.3 +8 27.5 0.26 2
4729 Mikhailmil’ 09 01.4 14.0 −4 17.74 0.36 2−
7234 1986 QV3* 09 01.5 14.4 −15
527 Euryanthe* 09 03.6 13.1 −17 26.06 0.11 2−
5913 1990 BU* 09 04.2 14.2 +0 52. 0.10 1
6434 Jewitt* 09 04.2 14.7 −19
1184 Gaea* 09 04.6 14.2 −11 2.94 0.09–0.25 2
2865 Laurel 09 04.7 14.4 +1 21.5 0.15 2
3346 Gerla 09 04.7 15.0 −19
3257 Hanzlik 09 04.8 14.6 −15
346 Hermentaria 09 05.1 10.6 −19 28.43 0.07–0.20 2
357 Ninina* 09 05.7 12.9 −16 35.98 0.12 2
1385 Gelria* 09 05.8 13.8 −15 0.36
2244 Tesla 09 05.8 14.9 −17
1728 Goethe Link 09 08.9 14.3 +6 81. 0.39 2
3770 Nizami* 09 09.2 15.0 −5
1347 Patria 09 13.2 14.6 +11 29.5 0.12 2
768 Struveana 09 15.2 14.2 −22 8.76 0.26–0.54 2+
2107 Ilmari 09 15.2 14.7 +7 0.06
5001 EMP* 09 15.2 14.3 −4
1005 Arago* 09 15.5 13.7 −1 8.7819 0.22 2
1124 Stroobantia 09 18.0 14.5 −7 16.39 0.15 1
1118 Hanskya 09 19.1 14.2 +11 15.61 0.18–0.38 2
676 Melitta 09 19.7 13.0 −10 7.87 0.04–0.20 2
1010 Marlene* 09 20.6 14.0 −7 31.06 0.17–0.32 2+
449 Hamburga 09 20.7 13.2 −5 18.263 0.08–0.17 2+
892 Seeligeria 09 21.0 14.0 −2 41.4 0.15 2
596 Scheila 09 23.8 13.4 −17 15.851 0.06–0.09 2+
1622 Chacornac 09 24.0 14.3 +0 12.206 0.24–0.25 2
1461 Jean-Jacques 09 24.7 14.6 −19 16.56 0.09 2
541 Deborah 09 25.0 13.8 +9 13.91 0.04–0.07 2+
8265 1986 RB5 09 25.3 14.9 −8
384 Burdigala 09 26.3 12.8 −5 21.1 0.03 2−
10262 Samoilov* 09 26.5 14.6 −11
1468 Zomba* 09 27.4 13.7 +23 2.77 0.3 2
3255 Tholen* 09 30.4 14.3 +28 3. 0.08 1
994 Otthild* 09 30.5 12.7 +5 5.95 0.09–0.15 2+
1839 Ragazza 09 30.5 15.0 −9
3171 Wangshouguan 09 30.7 14.9 −4

Low Phase Angle Opportunities

# Name Date α V Dec Period Amp U
389 Industria 07 02.8 0.17 11.0 −23 8.53 0.18–0.34 3
1496 Turku 07 09.2 0.41 13.4 −23 6.47 −0.51 3−
559 Nanon 07 11.7 0.32 12.5 −21 10.059 0.09–0.26 3
8 Flora 07 20.0 0.56 8.7 −22 12.865 0.03–0.11 3
862 Franzia 07 24.1 0.14 13.5 −20 7.52 −0.13 2
2213 Meeus 07 30.0 0.05 13.9 −19
268 Adorea 07 31.9 0.15 12.6 −19 7.80 0.15–0.20 3
202 Chryseis 08 03.1 0.41 12.0 −16 23.670 0.04–0.23 3
569 Misa 08 03.9 0.13 13.9 −17 13.52 −0.25 2
28 Bellona 08 07.4 0.73 11.4 −14 15.706 0.03–0.31 3
1148 Rarahu 08 12.5 0.69 13.5 −13 6.5447 −0.94 3−
1241 Dysona 08 15.9 0.18 13.2 −13 8.6080 −0.25 3−
52 Europa 08 19.0 0.97 10.9 −16 5.6304 0.08–0.20 3
570 Kythera 08 20.1 0.83 13.1 −10 8.120 0.15–0.18 2
1683 Castafiore 08 21.7 0.36 13.9 −11 13.931 −0.66 2+
1638 Ruanda 08 23.1 0.19 14.0 −11 4.2397 0.06–0.10 3
1874 Kacivelia 08 24.7 0.55 13.6 −10
1486 Marilyn 08 30.3 0.19 14.0 −09 2.2837 −0.40 1+
263 Dresda 08 31.9 0.66 13.6 −07 16.809 0.32–0.55 3
171 Ophelia 09 01.3 0.86 13.2 −11 6.66535 0.14–0.46 3
839 Valborg 09 01.3 0.21 12.9 −08 10.366 −0.19 3
1062 Ljuba 09 02.3 0.14 13.9 −08 33.8 −0.17 3
955 Alstede 09 13.4 0.24 12.9 −04 5.19 −0.27 3
435 Ella 09 13.5 0.93 12.1 −05 4.623 0.30–0.45 3
1005 Arago 09 15.4 0.61 13.8 −01 8.7819 −0.22 2
892 Seeligeria 09 20.9 0.35 14.0 −02 41.40 −0.15 2
124 Alkeste 09 24.2 0.24 11.5 +01 9.921 0.08–0.15 3
139 Juewa 09 24.2 0.11 12.1 +00 20.991 −0.20 3
1035 Amata 09 24.8 0.14 13.4 +00 9.081 −0.44 3
69 Hesperia 09 28.3 0.12 11.1 +02 5.655 0.09–0.24 3
94 Aurora 09 29.5 0.29 11.5 +03 7.22 0.03–0.18 3
1610 Mirnaya 09 29.9 0.35 14.0 +03

Shape/Spin Modeling Opportunities

There are two lists here. The first is for objects for which good occultation profiles are available. These are used to constrain the models obtained from lightcurve inversion, eliminating ambiguous solutions and fixing the size of asteroid. Lightcurves are needed for modeling and/or to establish the rotation phase angle at the time the profile was obtained. The second list is of those objects for which another set of lightcurves from one more apparitions will allow either an initial or a refined solution.

Occultation Profiles Available

Brightest LCDB DATA
# Name Date Mag Dec Period Amp U
580 Selene 07 05.7 14.7 −23 9.47 0.27 3−
559 Nanon 07 11.7 12.5 −21 10.059 0.09–0.26 3
47 Aglaja 07 27.0 11.0 −26 13.178 0.02–0.17 3
81 Terpsichore 08 01.8 12.4 −27 10.943 0.06–0.10 3
93 Minerva 08 07.2 10.8 −27 5.982 0.04–0.20 3
78 Diana 08 07.6 12.4 −20 7.2991 0.02–0.30 3
476 Hedwig 08 12.8 11.7 −05 27.33 0.13 3
238 Hypatia 09 12.3 11.7 +00 8.8745 0.07–0.17 3
324 Bamberga 09 13.3 8.1 +05 29.43 0.07–0.12 3
139 Juewa 09 24.2 12.1 +00 20.991 0.20 3
124 Alkeste 09 24.2 11.4 +01 9.921 0.08–0.15 3
205 Martha 09 29.5 12.8 +09 14.912 0.10–0.50 3−
94 Aurora 09 29.6 11.5 +03 7.22 0.03–0.18 3
3171 Wangshouguan 09 30.7 14.9 −04

Inversion Modeling Candidates

Brightest LCDB Data
# Name Date Mag Dec Period Amp U
686 Gersuind 07 03.9 11.9 −04 6.3127 0.30–0.37 3
252 Clementina 07 07.4 14.1 −08 10.864 0.32–0.44 3
851 Zeissia 07 07.9 14.2 −20 9.34 0.38–0.53 3
1496 Turku 07 09.2 13.4 −23 6.47 0.51 3−
1379 Lomonosowa 07 10.4 14.2 +01 24.488 0.63 3
6307 Maiztegui 07 12.6 14.9 −20 4.68 0.15 2
333 Badenia 07 14.8 13.5 −27 8.192 0.20–0.33 3−
762 Pulcova 07 16.2 13.0 −25 5.839 0.18–0.30 3
2036 Sheragul 07 18.3 13.9 −28 5.41 0.60–1.50 3
4713 Steel 07 19.5 14.5 −35 5.199 0.28–0.44 3
186 Celuta 07 21.9 11.3 −45 19.842 0.4 –0.55 3
1446 Sillanpaa 07 24.6 15.0 −29 9.6602 0.55 3
1503 Kuopio 07 28.4 14.2 −23 9.957 0.77 3
540 Rosamunde 07 29.2 13.5 −09 9.336 0.40–0.66 3−
1388 Aphrodite 08 07.0 14.7 −33 11.9432 0.35–0.65 3
6495 1992 UB1 08 10.1 14.9 −03 5.697 0.29–0.45 2
1900 Katyusha 08 10.2 14.7 −09 9.4999 0.56–0.74 3
503 Evelyn 08 13.5 13.5 −21 38.7 0.30–0.5 2
1835 Gajdariya 08 14.2 15.0 −14 6.3276 0.50 3
1423 Jose 08 16.1 14.3 −18 12.307 0.68–0.85 3
756 Lilliana 08 18.0 14.8 +12 7.834 0.18–0.99 3
1547 Nele 08 18.9 14.6 −04 7.100 0.30–0.45 3−
104 Klymene 08 21.7 12.6 −16 8.984 0.3 3
943 Begonia 08 23.5 14.9 −21 15.66 0.34 3
3300 McGlasson 08 30.2 14.1 −30 22.91 0.16 2
2430 Bruce Helin 08 30.2 14.2 −53 128. 0.6 2
3657 Ermolova 09 01.9 14.5 +02 2.6064 0.18–0.25 3
6406 1992 MJ 09 06.1 14.6 −11 6.819 1.18 3
1467 Mashona 09 07.7 12.7 +05 9.76 0.24 3
1728 Goethe Link 09 08.9 14.3 +06 81. 0.39 2
394 Arduina 09 09.3 12.0 −16 16.5 0.29–0.54 3
565 Marbachia 09 19.5 14.7 +11 4.587 0.20–0.65 3
1314 Paula 09 20.9 14.6 +08 5.9498 0.83 3
408 Fama 09 27.0 13.1 +13 202.10 0.05–0.58 3
994 Otthild 09 30.5 12.7 +05 5.95 0.09–0.14 2+

Radar-Optical Opportunities

Use the ephemerides below as a guide to your best chances for observing, but remember that photometry may be possible before and/or after the ephemerides given below. Some of the targets may be too faint to do accurate photometry with backyard telescopes. However, accurate astrometry using techniques such as “stack and track” is still possible and can be helpful for those asteroids where the position uncertainties are significant. Note that the intervals in the ephemerides are not always the same and that geocentric positions are given. Use these web sites to generate updated and topocentric positions:

MPC: http://www.minorplanetcenter.org/iau/MPEph/MPEph.html

JPL: http://ssd.jpl.nasa.gov/?horizons

In the ephemerides below, ED and SD are, respectively, the Earth and Sun distances (AU), V is the estimated Johnson V magnitude, and α is the phase angle. SE and ME are the great circles distances (in degrees) of the Sun and Moon from the asteroid. MP is the lunar phase and GB is the galactic latitude. “PHA” in the header indicates that the object is a “potentially hazardous asteroid”, meaning that at some (long distant) time, its orbit might take it very close to Earth.

(52760) 1998 ML14 (Jun-Aug, H = 17.6, PHA)

Hicks et al. (1998) determined a rotation period of 14.98 h for this 1 km NEA. Follow-up observations would be a great help. The object is visible for a number of weeks. The phase angle increase dramatically over the span of the ephemeris. In such cases, it is better not to create a single composite lightcurve over that full period but multiple lightcurves based on subsets of data obtained about 1–2 weeks apart. This allows following the evolution of the lightcurve’s amplitude and shape and provides even better modeling information.

DATE RA Dec ED SD V α SE ME MP GB
06/25 18 25.4 −31 10 0.40 1.41 16.7 5.8 172 23 −0.96 −9
07/02 18 15.4 −31 53 0.34 1.35 16.4 8.2 169 118 −0.32 −7
07/09 18 02.0 −32 34 0.28 1.29 16.1 14.6 161 152 +0.01 −5
07/16 17 44.9 −33 08 0.24 1.23 15.9 23.0 152 65 +0.49 −2
07/23 17 23.8 −33 30 0.20 1.17 15.7 33.0 141 44 −1.00 +1
07/30 16 56.9 −33 31 0.16 1.12 15.4 44.8 129 142 −0.47 +6
08/06 16 19.7 −32 50 0.12 1.07 15.2 59.4 115 123 −0.01 +12
08/13 15 21.0 −30 13 0.09 1.03 15.1 79.7 95 26 +0.34 +22

(153349) 2001 PJ19 (Jul-Aug, H = 18.0)

There is no previously determined period in the lightcurve database (LCDB; Warner et al., 2009) for this 600-meter NEA. While the asteroid doesn’t reach very low phase angles, the range is still substantial and so it may be worth obtaining blocks of data at several times and generating multiple lightcurves.

DATE RA Dec ED SD V α SE ME MP GB
07/20 00 23.1 +51 11 0.08 1.02 16.0 87.9 88 117 +0.89 −11
07/25 22 07.5 +35 58 0.10 1.07 15.7 56.6 119 42 −0.93 −16
07/30 21 18.6 +24 49 0.14 1.12 16.0 39.4 135 73 −0.47 −17
08/04 20 55.7 +18 03 0.19 1.18 16.5 30.0 145 130 −0.08 −17
08/09 20 42.9 +13 35 0.24 1.23 16.9 24.8 149 146 +0.04 −17
08/14 20 35.3 +10 23 0.30 1.28 17.4 22.4 151 89 +0.45 −18
08/19 20 30.8 +07 56 0.35 1.33 17.8 21.7 151 25 +0.94 −18
08/24 20 28.3 +05 59 0.41 1.38 18.2 22.1 149 60 −0.89 −18

2010 AF30 (Jul, H = 21.6)

The estimated size of this NEA (assuming taxonomic type S) is only 150 meters. In which case, there is a chance that it may have a rotation period of less than 2 hours and might even be tumbling. There are no entries in the LCDB.

DATE RA Dec ED SD V α SE ME MP GB
07/15 05 19.0 −41 38 0.05 1.00 18.9 106.7 71 98 +0.38 −34
07/16 04 49.9 −46 16 0.05 1.01 18.5 99.4 78 106 +0.49 −40
07/17 04 16.0 −50 21 0.05 1.01 18.2 92.2 85 110 +0.60 −45
07/18 03 37.7 −53 36 0.05 1.02 18.0 85.2 92 109 +0.70 −50
07/19 02 56.6 −55 52 0.05 1.02 17.8 78.5 99 103 +0.80 −54
07/20 02 15.1 −57 08 0.05 1.03 17.7 72.3 105 95 +0.89 −57
07/21 01 35.6 −57 29 0.05 1.04 17.7 66.6 111 84 +0.95 −59
07/22 01 00.1 −57 09 0.06 1.04 17.7 61.4 116 73 +0.99 −60

1627 Ivar (Jul-Nov, H = 13.2)

This may be one of the easier NEAs that you’ll ever observe. It is bright (be careful about overexposing) and well-placed for more than 3 months. Here’s a great opportunity to get multiple lightcurves over a range of phase angles. The period is well-known: 4.798 h. The amplitude has ranged from 0.25 to 1.4 mag.

DATE RA Dec ED SD V α SE ME MP GB
07/01 23 37.2 +07 29 0.32 1.13 12.5 62.4 101 22 −0.42 −51
07/21 00 58.9 +05 30 0.33 1.13 12.5 61.1 103 102 +0.95 −57
08/10 01 55.0 +01 09 0.34 1.18 12.5 54.2 110 143 +0.10 −58
08/30 02 21.6 −04 33 0.36 1.25 12.5 42.6 123 54 −0.35 −59
09/19 02 19.1 −10 17 0.40 1.34 12.5 28.3 141 46 +1.00 −63
10/09 01 56.6 −13 43 0.47 1.44 12.8 16.8 155 132 +0.19 −70
10/29 01 34.0 −13 23 0.60 1.55 13.5 17.8 152 126 −0.31 −73
11/18 01 25.0 −10 19 0.79 1.66 14.4 24.1 137 46 −1.00 −71

(7753) 1988 XB (Jul, H = 18.6)

There are no entries for this NEA in the LCDB. The estimated size ranges from 0.5 to 1.1 km, depending on the assumed albedo. The SMASS II survey found a taxonomic type of B, making it dark (low albedo) object, which leads to the larger size.

DATE RA Dec ED SD V α SE ME MP GB
07/01 13 03.3 −15 38 0.13 1.05 16.8 71.7 101 174 −0.42 +47
07/02 12 53.5 −15 10 0.13 1.04 16.8 75.0 98 165 −0.32 +48
07/03 12 43.5 −14 39 0.13 1.03 16.9 78.4 95 151 −0.23 +48
07/04 12 33.2 −14 06 0.12 1.03 17.0 81.9 91 137 −0.16 +49
07/05 12 22.7 −13 30 0.12 1.02 17.1 85.4 88 122 −0.09 +49
07/06 12 12.1 −12 52 0.12 1.01 17.2 89.0 84 108 −0.05 +49
07/07 12 01.3 −12 12 0.12 1.00 17.3 92.7 81 94 −0.02 +49
07/08 11 50.4 −11 29 0.12 1.00 17.4 96.4 77 79 +0.00 +49

(232691) 2004 AR1 (Jul-Aug, H = 19.8)

This NEA has an estimated size of about 300 meters. As such, its rotation period is probably 2 hours or more. This one is definitely for Southern Hemisphere observers.

DATE RA Dec ED SD V α SE ME MP GB
07/20 20 23.2 −51 15 0.24 1.23 18.3 25.1 149 49 +0.89 −35
07/25 20 10.7 −53 20 0.21 1.19 18.0 28.1 146 54 −0.93 −33
07/30 19 51.7 −55 35 0.18 1.16 17.7 32.6 142 108 −0.47 −30
08/04 19 21.8 −57 55 0.14 1.12 17.4 39.1 136 140 −0.08 −27
08/09 18 33.0 −60 02 0.12 1.09 17.1 48.1 127 107 +0.04 −21
08/14 17 11.0 −60 30 0.09 1.05 16.8 61.2 114 51 +0.45 −12
08/19 15 10.3 −54 32 0.07 1.02 16.8 81.8 94 66 +0.94 +3
08/24 13 14.2 −34 37 0.05 0.99 17.9 114.1 63 150 −0.89 +28

89 Julia (Jul-Nov, H = 6.6)

The rotation period for this inner main-belt asteroid is 11.38 hours. This makes it difficult for a single station to get complete coverage of the lightcurve without an prolonged campaign. A collaboration involving observers well-separated in longitude would be ideal. The estimated diameter is 151 km.

DATE RA Dec ED SD V α SE ME MP GB
07/01 23 50.5 +06 44 1.71 2.11 10.6 28.4 99 19 −0.42 −53
07/21 00 03.2 +11 56 1.49 2.10 10.3 26.6 112 91 +0.95 −49
08/10 00 05.3 +16 45 1.31 2.09 9.9 22.5 128 162 +0.10 −45
08/30 23 54.7 +20 31 1.18 2.09 9.4 16.4 144 79 −0.35 −40
09/19 23 34.4 +22 22 1.13 2.09 9.2 11.3 156 23 +1.00 −37
10/09 23 14.5 +22 01 1.16 2.09 9.3 13.6 150 109 +0.19 −36
10/29 23 06.0 +20 32 1.28 2.10 9.7 19.6 135 147 −0.31 −36
11/18 23 11.8 +19 15 1.46 2.12 10.2 24.2 119 66 −1.00 −38

324 Bamberga (Jul-Nov, H = 6.82)

This middle main-belt asteroid has an estimated diameter of 230 km. It’s a type CP (Tholen, 1989), meaning is has a lower albedo on the order of 0.06. The rotation period of 29.4 h makes this another object where a collaboration among observers will have the best chance of securing a complete lightcurve.

DATE RA Dec ED SD V α SE ME MP GB
07/01 23 19.9 −06 57 1.37 1.98 10.3 28.7 111 31 −0.42 −60
07/21 23 33.7 −03 05 1.14 1.92 9.8 25.5 125 79 +0.95 −60
08/10 23 36.1 +00 34 0.96 1.87 9.2 19.2 143 178 +0.10 −57
08/30 23 25.2 +03 42 0.85 1.83 8.5 9.9 162 91 −0.35 −53
09/19 23 06.1 +05 55 0.81 1.80 8.2 6.8 168 7 +1.00 −48
10/09 22 51.5 +07 15 0.86 1.79 8.7 16.9 149 99 +0.19 −45
10/29 22 51.4 +08 22 0.97 1.78 9.3 25.2 130 159 −0.31 −44
11/18 23 06.4 +09 53 1.13 1.79 9.7 30.0 115 69 −1.00 −45

(277475) 2005 WK4 (Aug-Sep, H = 20.2, PHA)

2005 WK4 is an NEA with an estimated size of 280 meters. There are no entries in the LCDB for it. While brightest around mid-August, rapid sky motion at that time may make good photometry a bit difficult. If you have the resources and are in the Southern Hemisphere, observations soon after closest approach might be more productive.

DATE RA Dec ED SD V α SE ME MP GB
08/05 04 33.7 +49 22 0.03 1.00 17.0 116.5 62 48 −0.04 +1
08/10 01 40.2 +07 53 0.02 1.02 14.1 67.5 111 146 +0.10 −53
08/15 23 59.3 −27 53 0.03 1.04 14.3 34.4 144 107 +0.56 −78
08/20 23 11.2 −38 54 0.06 1.06 15.3 29.5 149 40 +0.98 −66
08/25 22 45.0 −42 55 0.08 1.08 16.1 30.4 147 64 −0.81 −60
08/30 22 29.2 −44 33 0.11 1.10 16.8 32.3 145 115 −0.35 −57
09/04 22 19.1 −45 04 0.13 1.11 17.3 34.2 142 143 −0.02 −55
09/09 22 12.8 −44 58 0.16 1.13 17.8 36.1 139 105 +0.13 −54

(137126) 1999 CF9 (Aug-Sep, H = 17.9, PHA)

The estimated diameter for this NEA is 800 meters. The rotation period is not known, or at least is not included in the LCDB. The end of August and early September may offer the best compromise between brightness, sky motion, and changing phase angle.

DATE RA Dec ED SD V α SE ME MP GB
08/20 14 35.9 +04 27 0.07 0.99 16.1 106.8 69 95 +0.98 +56
08/25 17 32.8 −10 08 0.07 1.04 14.4 65.7 111 118 −0.81 +12
08/30 19 40.4 −17 04 0.10 1.08 14.6 39.2 137 150 −0.35 −18
09/04 20 40.1 −18 31 0.15 1.13 15.3 29.7 146 162 −0.02 −32
09/09 21 11.2 −18 42 0.20 1.18 16.0 26.7 148 106 +0.13 −39
09/14 21 30.3 −18 32 0.26 1.23 16.6 26.0 148 41 +0.65 −43
09/19 21 43.6 −18 13 0.32 1.28 17.1 26.2 146 29 +1.00 −46
09/24 21 53.8 −17 50 0.38 1.33 17.6 26.9 143 91 −0.79 −48

2007 CN26 (Aug-Oct, H = 21.0, PHA)

As with many other asteroids presented this quarter, there is no reported rotation period in the LCDB. 2007 CN26 is an NEA with an estimated diameter of 200 meters. This puts it on the edge of being a candidate for having a rotation rate of less than 2 hours. Until you know one way or the other, keep exposures to a minimum but long enough so that scintillation noise doesn’t dominate (~10 sec for backyard telescopes).

DATE RA Dec ED SD V α SE ME MP GB
08/30 05 16.7 +27 29 0.03 1.00 17.0 101.9 76 9 −0.35 −6
09/04 03 57.5 +05 45 0.04 1.02 16.5 75.2 103 85 −0.02 −34
09/09 03 16.8 −06 46 0.05 1.03 16.7 58.7 119 151 +0.13 −50
09/14 02 51.9 −13 37 0.07 1.05 17.0 48.3 129 116 +0.65 −59
09/19 02 34.3 −17 37 0.09 1.07 17.3 41.1 136 51 +1.00 −64
09/24 02 20.6 −20 03 0.11 1.09 17.6 35.6 141 42 −0.79 −68
09/29 02 09.1 −21 30 0.13 1.11 17.9 31.6 145 91 −0.33 −71
10/04 01 59.2 −22 14 0.15 1.13 18.2 28.7 147 140 −0.01 −74

(329437) 2002 OA22 (Aug-Oct, H = 19.3, PHA)

Behrend et al. (2012) report a period of 10.5 h for 2002 OA22, a 400 meter NEA. The period is based mostly on a single night of observations that appeared to include a maximum and minimum (0.41 mag amplitude). However, a second night showed a nearly flat lightcurve. For a period of 10.5 h, the tumbling damping time is about 1.4 Gyr, so it’s not entirely out of the question that the asteroid is tumbling. Make no assumptions and go where the data lead.

DATE RA Dec ED SD V α SE ME MP GB
08/20 01 06.9 +20 43 0.20 1.14 18.0 48.6 123 71 +0.98 −42
08/27 01 17.7 +20 03 0.17 1.12 17.5 45.7 127 25 −0.63 −42
09/03 01 28.8 +18 21 0.14 1.11 17.0 42.2 133 105 −0.06 −44
09/10 01 41.2 +14 52 0.11 1.09 16.2 38.0 138 166 +0.22 −46
09/17 01 57.2 +07 53 0.08 1.07 15.4 33.7 144 69 +0.92 −52
09/24 02 23.6 −07 11 0.05 1.05 14.5 34.1 144 31 −0.79 −60
10/01 03 27.8 −39 41 0.04 1.02 14.3 57.5 121 96 −0.16 −55
10/08 07 33.0 −68 56 0.04 0.99 16.0 96.4 81 83 +0.11 −22

(152664) 1998 FW4 (Sep, H = 19.5, PHA)

Here’s another NEA with no reported rotation period. The estimated diameter is 340 meters.

DATE RA Dec ED SD V α SE ME MP GB
09/01 00 22.2 −01 31 0.29 1.28 18.6 20.4 154 103 −0.18 −63
09/05 00 29.6 −00 28 0.24 1.23 18.0 19.8 156 149 +0.00 −63
09/09 00 39.8 +01 04 0.19 1.19 17.5 19.8 157 160 +0.13 −62
09/13 00 55.6 +03 31 0.14 1.14 16.8 21.1 156 110 +0.54 −59
09/17 01 24.6 +08 02 0.10 1.09 16.1 26.0 152 61 +0.92 −54
09/21 02 34.2 +17 51 0.06 1.05 15.4 41.5 136 24 −0.97 −39
09/25 05 56.7 +32 26 0.05 1.01 16.0 84.8 93 24 −0.70 +4
09/29 09 18.1 +25 56 0.07 0.96 18.9 124.3 53 23 −0.33 +43

Contributor Information

Brian D. Warner, Palmer Divide Observatory/MoreData!, 17995 Bakers Farm Rd., Colorado Springs, CO 80908 USA

Alan W. Harris, MoreData!, La Cañada, CA 91011-3364 USA

Petr Pravec, Astronomical Institute, CZ-25165 Ondřejov, CZECH REPUBLIC.

Josef Ďurech, Astronomical Institute, Charles University in Prague, 18000 Prague, CZECH REPUBLIC.

Lance A.M. Benner, Jet Propulsion Laboratory, Pasadena, CA 91109-8099 USA

References

  1. Behrend R (2012) Observatoire de Geneve web site. http://obswww.unige.ch/~behrend/page_cou.html.
  2. Hicks M; Weissman P (1998) IAUC 6987. [Google Scholar]
  3. Kaasalainen M, Durech J, Warner BD, Krugly Y, Gaftonyuk N, Ninel M (2007). “Acceleration of the rotation of asteroid 1862 Apollo by radiation torques.” Nature 446, 420–422. [DOI] [PubMed] [Google Scholar]
  4. La Spina A; Paolicchi P; Kryszczyńska A; Pravec P (2004). “Retrograde spins of near-Earth asteroids from the Yarkovsky effect.” Nature 428, 400–401. [DOI] [PubMed] [Google Scholar]
  5. Lowry SC; Fitzsimmons A; Pravec P; Vokrouhlický D; Boehnhardt H; Taylor PA; Margot J-L; Galád A; Irwin M; Irwin J; Kusnirák P (2007). “Direct Detection of the Asteroidal YORP Effect.” Science 316, 272–274. [DOI] [PubMed] [Google Scholar]
  6. Pravec P, Vokrouhlicky D, Polishook D, Scheeres DJ, Harris AW, Galad A, Vaduvescu O, Pozo F, Barr A, Longa P, and 16 coauthors. (2010). “Formation of asteroid pairs by rotational fission,” Nature 466, 1085–1088. [DOI] [PubMed] [Google Scholar]
  7. Tholen DJ (1989). “Asteroid taxonomic classifications.” IN: Asteroids II; Proceedings of the Conference, Tucson, AZ, Mar. 8–11, 1988 (A90–27001 10–91). Tucson, AZ, University of Arizona Press, 1989, p. 1139–1150. [Google Scholar]
  8. Warner BD, Harris AW, Pravec P (2009). “The Asteroid Lightcurve Database.” Icarus 202, 134–146. Updated 2013 February. http://www.minorplanet.info/lightcurvedatabase.html [Google Scholar]

RESOURCES