Asteroid Lightcurve Data File
Hamanowa Astronomical Observatory
MPC code D91 Adati
| 8567 1996HW1 |
Result | Rotation Period : 0.364409 +/- 0.00003 day Amplitude : 1.04+/- 0.02 mag, |
![]() Fig, 1 The lightcurve of 8567 1996HW1 phased to a period of 0.364409 day. (Phase-angle: not corrected) ![]() Fig, 1 The lightcurve of 8567 1996HW1 phased to a period of 0.364409 day. (Phase-angle: corrected) |
||
| Observational date: 2008-Jul, 28 Aug, 07 08 17 Sep, 08 09 10
12 22 Oct, 01 02 (12 nights) Zero time of the graph: 2008 Jul, 28.40000 day (UT) Observational site: Hamanowa Astronomical Observatory (fukushima-pref, Japan) Telescope : Pellow telescope (D=400mm fl=1800mm Newtonian F=4.5 CCD camera : SBIG ST-8 Filter system : Idas-R (UBVRI) Dark and Flat : Dark-frame and Flat-field were corrected. Light time : corrected. Remarks : | ||
| Observations of 8567 1996HW1 was carried
out over 12 nights in July, August and September
of 2008.@The synodic period was determined
as 8.7458 } 0.0002 hr with a mean amplitude
of 1.04 } 0.02 mag was derived. . Minor planet 8567 1996HW1 was discovered by Spacewatch-Steward Observatory, Kitt Peak-Spacewatch in April 1996. This is an Amor asteroid with a diameter of 2.5 - 5.6 km (Near Earth Objects - Dynamic Site). The latest list of rotational parameters (Harris and Warner, 2006) has 8.7573hr with an amplitude 0.25 mag. Photometric data for 8567 1996HW1 were collected using a 0.4 m Newtonian telescope, a SBIG ST-8E camera, and R filter (UBVRI) with guided exposure times ranging from 120 seconds to 360 seconds at Hamanowa Astronomical Observatory. The image scale was 2.0 arc-seconds per pixel and camera temperature held at -15c for all measurements. The sky condition was good over the whole observation period. All images were dark subtracted and flat-fielded before measuring using IRAF (Tody 1986) and Stella Image ver, 5 (Astro Arts). Data were collected by light travel time from the asteroid to the Earth, and times are for mid-exposure. We also used Cyclocode (B. Dermawan 2003) to determine the period. The phase changes as the observation time progresses because 8567 1996HW1 is NEO. Therefore, we used data of September 8, 9 and 10 where few phase-changes occur to make a period clear. Analysis of this data set showed a yielded rotation period of 8.7458 } 0.0003 day. Figure 1 is created by applying a sought period to all observation data and shows the phase of the curve be behind, by observation time's progressing. The data of all days must revise a difference in the period which is caused by the change of phase-angle. Because 8567 1996 HW1 of the observation period showed a big magnitude variation, an offset value was mainly fixed by the change element in the celestial-longitude. Figure 2 is created by applying this offset and is correcting the difference of the phase well. The peak to peak amplitude was the 0.7 mag in the early stages of the observation, in the middle was 0.9 mag, and it increased from the observation on September 8th to the 1.04 mag. Table 1 The aspect data of 8567 1996HW1, and the offset value which used for the correction.
|