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. Author manuscript; available in PMC: 2020 May 22.
Published in final edited form as: Minor Planet Bull. 2017 Jan-Mar;44(1):12–19.

ASTEROID LIGHTCURVE ANALYSIS AT CS3-PALMER DIVIDE STATION: 2016 JULY-SEPTEMBER

Brian D Warner 1
PMCID: PMC7243973  NIHMSID: NIHMS1570129  PMID: 32455388

Abstract

Lightcurves for 25 main-belt asteroids were obtained at the Center for Solar System Studies-Palmer Divide Station (CS3-PDS) from 2016 July to September.


CCD photometric observations of 25 main-belt asteroids were made at the Center for Solar System Studies-Palmer Divide Station (CS3-PDS) from 2016 July to September. Table I lists the telescope/CCD camera combinations used for the observations. All the cameras use CCD chips from the KAF blue-enhanced family and so have essentially the same response. The pixel scales for the combinations range from 1.24–1.60 arcsec/pixel.

Table I.

List of CS3-PDS telescope/CCD camera combinations.

Desig Telescope Camera
Squirt 0.30-m f/6.3 Schmidt-Cass ML-1001E
Borealis 0.35-m f/9.1 Schmidt-Cass FLI-1001E
Eclipticalis 0.35-m f/9.1 Schmidt-Cass STL-1001E
Australius 0.35-m f/9.1 Schmidt-Cass STL-1001E
Zephyr 0.50-m f/8.1 R-C FLI-1001E

All lightcurve observations were unfiltered since a clear filter can result in a 0.1–0.3 magnitude loss. The exposure duration varied depending on the asteroid’s brightness and sky motion. Guiding on a field star sometimes resulted in a trailed image for the asteroid.

Measurements were made using MPO Canopus. The Comp Star Selector utility in MPO Canopus found up to five comparison stars of near solar-color for differential photometry. Catalog magnitudes were usually taken from the CMC-15 (http://svo2.cab.inta-csic.es/vocats/cmc15/) or APASS (Henden et al., 2009) catalogs. The MPOSC3 catalog was used as a last resort. This catalog is based on the 2MASS catalog (http://www.ipac.caltech.edu/2mass) with magnitudes converted from J-K to BVRI (Warner, 2007). The nightly zero points for the catalogs are generally consistent to about ± 0.05 mag or better, but on occasion reach 0.1 mag and more. There is a systematic offset among the catalogs so, whenever possible, the same catalog is used throughout the observations for a given asteroid. Period analysis is also done with MPO Canopus, which implements the FALC algorithm developed by Harris (Harris et al., 1989).

In the plots below, the “Reduced Magnitude” is Johnson V as indicated in the Y-axis title. These are values that have been converted from sky magnitudes to unity distance by applying –5*log (rΔ) to the measured sky magnitudes with r and Δ being, respectively, the Sun-asteroid and Earth-asteroid distances in AU. The magnitudes were normalized to the given phase angle, e.g., alpha(6.5°), using G = 0.15, unless otherwise stated. The X-axis is the rotational phase ranging from –0.05 to 1.05.

If the plot includes an amplitude, e.g., “Amp: 0.65”, this is the amplitude of the Fourier model curve and not necessarily the adopted amplitude for the lightcurve. The value is meant only to be a quick guide.

For the sake of brevity, only some of the previously reported results may be referenced in the discussions on specific asteroids. For a more complete listing, the reader is directed to the asteroid lightcurve database (LCDB; Warner et al., 2009a). The on-line version at http://www.minorplanet.info/lightcurvedatabase.html allows direct queries that can be filtered a number of ways and the results saved to a text file. A set of text files of the main LCDB tables, including the references with bibcodes, is also available for download. Readers are strongly encouraged to obtain, when possible, the original references listed in the LCDB for their work.

637 Chrysothemis

This Themis group member was in the field-of-view of a planned target for only one night. Without a second night, it was not possible to tell if the variations seen in the plot were systematic rather than due to rotation of the asteroid. The period shown in the plot is for informational purposes only.

graphic file with name nihms-1570129-f0001.jpg

699 Hela

Previous results for this Mars-crossing asteroid have varied from 2.63 h (Monson, 2011) to 4.765 h (Behrend, 2003w). Most, however, have been approximately 3.3 hours (e.g., Pilcher et al., 2000). The results from the PDS data in 2016 are in relatively good agreement with the majority of previous results.

graphic file with name nihms-1570129-f0002.jpg

2083 Smither

This Hungaria asteroid had been observed by the author on several previous occasions (Warner, 2007a; 2010; 2012a; 2015b). Each time the period was about 2.67 hours, which is the same result found from the 2016 data.

graphic file with name nihms-1570129-f0003.jpg

2108 Otto Schmidt

The only previous result in the LCDB for this inner main-belt asteroid is 15.24 h (Behrend, 2001w). The period spectrum based on the PDS data in 2016 does not support that result, but favors one of 6.90 h. A period of 6.31 hour cannot be formally excluded.

graphic file with name nihms-1570129-f0004.jpg

2150 Nyctimene

This is another Hungaria asteroid that was observed by the author on several previous occasions: e.g., Warner (2007a, 6.125 h; 2008, 6.129 h; 2015a, 6.130 h). Over the course of all the apparitions, the amplitude has varied between 0.59 and 0.76 mag, indicating a spin axis pole that is mostly upright, but still has a significant obliquity. Lightcurve inversion using all the data obtained by the author from 2007 through 2016 found a pole of λ = 285°, β = –74° and sidereal period of PSID = 6.125711 h. The negative latitude indicates that the asteroid is in retrograde rotation. These results and those for almost 200 other Hungarias will be presented in a future paper.

graphic file with name nihms-1570129-f0005.jpg

2919 Dali

This member of the Themis group has an estimated diameter of 19 km when assuming an albedo of pV ~ 0.08. Both using sparse data from the Palomar Transient Survey, Waszczak (2015) and Chang (2015) found a period of about 7.4 hours. The dense lightcurve from PDS in 2016 supports those results.

graphic file with name nihms-1570129-f0006.jpg

3443 Leetsungdao

Ivanova et al. (2002) found a period of 3.313 h for this Mars-crosser. Subsequent studies by Stephens (2002), Behrend (2001w), and Ferrero (2013) found a longer period of about 3.44 hours, as did the analysis using the 2016 PDS data.

graphic file with name nihms-1570129-f0007.jpg

4031 Mueller

This was the fourth apparition at which the author observed this Hungaria asteroid. All previous results and those from 2016 have a period near 2.94 h and amplitude that remained at A < 0.20 mag.

graphic file with name nihms-1570129-f0008.jpg

4164 Shilov

Shilov is a member of the Eunomia orbital group. It was a target of opportunity for two nights, i.e., it was in the same field as a targeted asteroid. Angeli and Barucci (1996) found a period of 18.35 h, but it is rated U = 1 (“probably wrong”) in the LCDB. The period of 18.4 hours reported here is based on a half-period solution of about 9.2 hours. This solution is rated only slightly higher, U = 2–. Future observations are encouraged.

graphic file with name nihms-1570129-f0009.jpg

5427 Jensmartin

The results from the 2016 PDS data give a period of 5.813 h. This is the fourth apparition at which the author observed this Hungaria and the fifth time it was worked by any CS3 observer. All previous results are in close agreement with the latest period (e.g., Warner, 2009c, 5.810 h; Stephens et al., 2014a, 5.812 h)

graphic file with name nihms-1570129-f0010.jpg

(6382) 1988 EL

Previous results by the author for this Hungaria include Warner (2005, 2.895 h; 2012b, 2.894 h; 2015c, 2.893 h). The 2016 results are in good agreement with those and other previous results.

graphic file with name nihms-1570129-f0011.jpg

6870 Pauldavies

Warner (2007b) and Stephens (2015) both found a period of 4.487 h. The period found from the 2016 data is essentially the same.

graphic file with name nihms-1570129-f0012.jpg

6911 Nancygreen

This is another Hungaria observed by the author as part of a final push before doing lightcurve inversion on more than 200 Hungaria asteroids. Previous results include Warner (2006, 5.3 h; 2009b, 4.33 h; 2014, 59.1 h). The mostly complete lightcurve with high amplitude in 2016 virtually assures a bimodal solution with a period of about 55 h (see Harris et al., 2014). The damping time from a tumbling state to principal axis rotation for the given period and estimated diameter is about 2–4 Gyr (see Pravec et al., 2005, 2010). If there were any indications of tumbling, they were hidden within the noise and incomplete coverage of the lightcurve.

graphic file with name nihms-1570129-f0013.jpg

7829 Jaroff

All previous results for this Hungaria are within 0.01 h of the period found from the 2016 data (e.g., Warner and Stephens, 2009b; Stephens 2015).

graphic file with name nihms-1570129-f0014.jpg

7959 Alysecherri

In 2013, Warner (2014) reported a period of 3.161 h for this Hungaria member. The 2016 data did not support this result, with the period spectrum showing only a minor drop below the noise in the RMS values for a period near 3.16 h. The data from 2013 were forced to fit the period found using the 2016 data. While the fit is not quite as good as to 3.161 h, it is still plausible given the noise and low amplitude. A period of 3.540 hours is adopted for this paper.

graphic file with name nihms-1570129-f0015.jpg

graphic file with name nihms-1570129-f0016.jpg

(8404) 1995 AN

Previous results for this Hungaria were ambiguous. Warner (2009d) found a period of 4.612 h but one of 3.204 h could not be formally excluded. Follow-up observations in 2012 (Warner, 2012c) led to a period of 3.200 hours, as did the results from the 2016 data analysis. A period of 3.202 h is adopted for this paper.

graphic file with name nihms-1570129-f0017.jpg

11152 Oomine

The period of 2.622 h reported here appears to be the first one for this Mars-crosser that was observed as a “full moon project.”

graphic file with name nihms-1570129-f0018.jpg

(16681) 1994 EV7

The 2016 apparition was the third one at which the author observed this Hungaria. The previous results (Warner, 2007b; 2012b) are in good agreement with the period found from the 2016 data.

graphic file with name nihms-1570129-f0019.jpg

(23974) 1999 CK12

The only previously reported lightcurve period is 5.485 h (Warner, 2012c). Masiero et al. (2012) observed this Hungaria with the WISE spacecraft and reported an albedo of pV = 0.697 using H = 14.5. This is unusually high, but not completely unreasonable if taking into account that the WISE survey may have at times been using faulty values for H (absolute magnitude) for many of the Hungaria members, mostly because the H values were probably determined at larger phase angles and may not have accounted for rotational variation.

If using H = 14.7 (the current value in MPCORB) and the correction algorithm from Harris and Harris (1997), pV becomes 0.61 ± 0.13. This is within 1-sigma of the average value for E-type asteroids (that of Hungaria collisional family member) as found by Warner et al. (2009). If using H = 14.8 ± 0.3 and G = 0.162 (Veres et al., 2015), pV = 0.57 ± 0.19, which is even closer to the average albedo for E-type asteroids in the LCDB.

graphic file with name nihms-1570129-f0020.jpg

(28992) 2001 MW28

This inner main-belt asteroid was a target of opportunity that stayed in the same field as the planned target for several nights. There were no previous entries in the LCDB for the asteroid.

graphic file with name nihms-1570129-f0021.jpg

(43003) 1999 UC14

1994 UC14 was another target of opportunity. The inner main-belt asteroid’s lightcurve had a small amplitude, which made finding a definitive period more difficult. The period spectrum shows several possible solutions with the one at about 5.5 hours favored even though it did not have the lowest RMS fit, which was near 10 hours. The shape of the lightcurve for the longer period was multimodal and asymmetric, implying a physically improbable shape.

It won’t be until 2023 October that 1999 UC14 will be brighter than V ~ 17.5. Between then, most apparitions are well into the 18th and 19th magnitude range.

graphic file with name nihms-1570129-f0022.jpg

graphic file with name nihms-1570129-f0023.jpg

(45898) 2000 XQ49

The 2016 apparition was the fourth one that the author observed this Hungaria asteroid. All previous results had a period near 5.42 hours (e.g., Warner 2014), making the results from 2016 in good agreement with those earlier findings.

graphic file with name nihms-1570129-f0024.jpg

(56591) 2000 JP37

This inner main-belt asteroid was in the field of a planned target for only one night. No period could be determined from the limited data set, though it seems probable that the period exceeds 10 hours and the amplitude was at least 0.2 mag.

graphic file with name nihms-1570129-f0025.jpg

(72007) 2000 XM7

There were no previously reported periods in the LCDB for this member of the Flora group, which was another target of opportunity. Fortunately, it was in the planned field for several nights, which allowed finding a reliable period estimate.

graphic file with name nihms-1570129-f0026.jpg

(96842) 1999 RH208

A middle main-belt asteroid, 1999 RH208 was in the same field as a planned target for two nights.

The period spectrum favored a period of 3.236 h, but a solution of 2.855 h cannot be formally excluded. The difference between the two is almost exactly one rotation over 24 hours. This uncertainty of the number of rotations over the span of the observations is sometimes called a rotational alias.

graphic file with name nihms-1570129-f0027.jpg

Table II.

Observing circumstances. The phase angle (α) is given at the start and end of each date range, unless it reached a minimum, which is then the second of three values. If a single value is given, the phase angle did not change significantly and the average value is given. LPAB and BPAB are each the average phase angle bisector longitude and latitude (see Harris et al., 1984), unless two values are given (first/last date in range). The Group column gives the orbital group to which the asteroid belongs. The definitions and values are those used in the LCDB (Warner et al., 2009). THM = Themis; H = Hungaria; MC = Mars-crosser; V = Vestoid; MB-I = Inner main-belt; MB-M = middle main-belt; FLOR = Flora.

Number Name 2016 mm/dd Pts Phase LPAB BPAB Period P.E. Amp A.E. Group
637 Chrysothemis 07/28–07/28 53 9.9,9.9 338 0 3.7 0.3 0.06 0.01 THM
699 Hela 07/24–07/27 375 40.7,40.4 2 20 3.396 0.0005 0.16 0.01 MC
2083 Smither 07/14–07/16 213 14.9,14.4 305 19 2.675 0.001 0.11 0.01 H
2108 Otto Schmidt 07/29–08/01 135 15.0,13.8 337 0 6.9 0.05 0.16 0.01 MB-I
2150 Nyctimene 08/07–08/13 126 29.3,29.7 259 29 6.133 0.005 0.58 0.03 H
2919 Dali 08/01–08/03 179 11.6,10.9 337 0 7.43 0.01 0.45 0.02 THM
3443 Leetsungdao 07/19–07/21 93 34.1,33.7 356 7 3.439 0.005 0.47 0.03 MC
4031 Mueller 08/16–08/24 132 34.3,34.1 34 8 2.942 0.001 0.17 0.02 H
4164 Shilov 08/10–08/11 58 24.5,24.4 27 6 18.5 0.5 0.29 0.02 V
5427 Jensmartin 07/14–07/16 175 33.5,33.4 355 22 5.813 0.005 0.45 0.02 H
6382 1988 EL 08/18–08/21 109 31.8,31.7 33 10 2.904 0.002 0.2 0.03 H
6870 Pauldavies 07/11–07/13 112 28.2,27.7 335 4 4.488 0.005 0.51 0.02 H
6911 Nancygreen 08/11–08/20 421 32.9,31.2 13 16 54.7 0.5 0.75 0.05 H
7829 Jaroff 07/20–07/24 222 15.9,14.8 317 18 4.4 0.002 0.55 0.05 H
7959 Alysecherri 09/16–09/24 178 29.4,26.9 41 13 3.54 0.002 0.12 0.02 H
8404 1995 AN 09/23–09/30 149 27.9,26.6 48 19 3.202 0.001 0.14 0.01 H
11152 Oomine 07/25–08/01 210 20.7,17.7 333 0 2.622 0.001 0.1 0.01 MC
16681 1994 EV7 08/10–08/15 204 32.9,32.3 17 10 5.315 0.005 1.12 0.03 H
23974 1999 CK12 08/21–08/27 141 31.4,30.3 14 20 5.481 0.005 0.67 0.05 H
28992 2001 MW28 07/29–08/02 156 18.4,16.5 336 0 16.6 0.2 0.79 0.05 MB-I
43003 1999 UC14 07/28–08/01 119 21.3,19.3 332 0 5.459 0.006 0.12 0.01 MB-I
45898 2000 XQ49 09/16–09/18 153 25.1,24.6 35 17 5.415 0.005 1 0.03 H
56591 2000 JP37 08/14–08/14 20 30.0,30.0 25 5 0.25 MB-I
72007 2000 XM7 07/30–08/02 75 17.6,16.3 336 0 4.89 0.05 0.25 0.03 FLOR
96842 1999 RH208 08/12–08/13 56 26.6,26.5 23 11 3.236 0.006 0.36 0.03 MB-M

Acknowledgements

Funding for PDS observations, analysis, and publication was provided by NASA grant NNX13AP56G. Work on the asteroid lightcurve database (LCDB) was also funded in part by National Science Foundation grant AST-1507535. This research was made possible in part based on data from CMC15 Data Access Service at CAB (INTA-CSIC) (http://svo2.cab.inta-csic.es/vocats/cmc15/) and the AAVSO Photometric All-Sky Survey (APASS), funded by the Robert Martin Ayers Sciences Fund. This publication makes use of data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation. (http://www.ipac.caltech.edu/2mass/)

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