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Astron. Astrophys. 341, 912-917 (1999) 3. ResultsIn the following, we describe for each comet separately the results obtained from our CCD image analysis and photometry. The (equivalent) radius was calculated from the mean (averaged over the available measurements) filter brightness of the comets following the standard equation as given for instance in Huebner (1992; Eq. (2.1), Sect. 2.2.1). The albedo was assumed to be 0.04, for the (linear) phase angle correction of the radius value a darkening coefficient of 0.03 mag/deg was used. The summary of the results is given in Table 2. R(1,1,0) and V(1,1,0) are the R and V magnitudes of the comets at 1 AU Sun and Earth distance and for 0 deg phase angle. The V-R colour of the Sun is 0.55 mag. Table 2. Photometry, colour, radius, rotation and activity status of 26P/GS and 73P/SW3. Errors are 1 sigma. 3.1. 26P/Grigg-SkjellerupAt the time of our observations (i.e. when the comet was at about 3.8 AU from the Sun) 26P/GS was inactive when moving outbound after the 1992 encounter with the GIOTTO spaceprobe of ESA. This is concluded from the star-like appearance of the comet and from the absence of a weak coma in our coadded image (Fig. 1). The equivalent radius of the nucleus is 1.45-1.50 km with a good agreement in both measured filters R and V (Table 2). The V-R colour is slightly bluish as compared to the Sun (Table 2). The lightcurve of the nucleus does not seem to be properly sampled by our observations (Fig. 4). However, a minor variability of (at least) 0.1 mag peak-to-peak is noticeable. This would correspond to a small-to-large-axis ratio of 0.9. The detected variability of the nucleus brightness seems to be real since it is larger than the 1-sigma uncertainty of the photometric magnitudes (and it is very similar in both the absolute and the relative photometry data). From the temporal development of the observed brightness variation we conclude that a rotation period of less than 0.5 days would hardly match our (partial) lightcurve of the nucleus.
3.2. 73P/Schwassmann-Wachmann 3In late December 1994 73P/SW3 was at 3 AU solar distance moving
inbound to its next perihelion passage in autumn 1995. It had already
developed a weak dust coma and tail as can be seen in our images
(Figs. 2 and 3). Hence, the photometry of the comet may no longer give
the light reflected at the surface of the nucleus alone, but it is
contaminated by some light from the coma (which was estimated not to
exceed about 20 percent of the total light from the object).
Therefore, the radius value of 1.1 km (which was determined using the
uncorrected flux) represents an upper limit for the nucleus size
(almost identical in R and V; Table 2). The V-R colour of 73P/SW3
was solar (within the errors of our photometry; Table 2). The R
filter brightness increased by about 0.25 mag within 1 day (Fig. 5).
However, our observations do not indicate whether this was a secular
(due to a general brightness increase) or a periodic (due to nucleus
rotation) effect. The coadded images of the comet show a weak coma and
a short tail (Figs. 2 and 3). The estimated radial diameter of the
coma was 11800 km, the lateral one was 8300 km. The tail had a length
of 13200 km and pointed to a position angle of 281
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