How to Search for Small Comets
Can the naked eye spot a small comet before it disrupts in the atmosphere? Can a pair of binoculars? Can a small telescope? Dr. Louis A. Frank explains how you can--or why you can't--in this brief technical note.
First of all, consider the naked, rested eye. The apparent brightness of
the small comets at the distance previously detected with the Spacewatch
Camera at a range of 137,000 km (85,600 miles) is typically V=19
magnitude. At a target range of 1000 km (625 miles) the apparent
brightness is about V=8.3 because you have gained V=10.7. For the naked
eye, the threshold brightness has been estimated by Opik and Millman in
terms of the percentage of objects detected as a function of brightness.
Opik claims 8% and 50% of the objects are detected at V=5 and V=4,
respectively. Millman estimates less than 0.5% and 25% at V=5 and V=2,
respectively. Clearly, under the best viewing conditions, the threshold
of the naked human eye is about V=5. Thus the small comets would be
dimmer than the threshold of the naked eye by V=3.3, or a factor of about
20 in light intensity. The naked eye simply cannot detect the small
comets at a range of 1000 km (625 miles).
Can the small comets be detected with binoculars? We have previously
estimated the detection rate with telescopes owned by amateur astronomers
and have shown that the detection rate is about 1 or 2 per night of
clear-sky viewing, if the telescope is pointed in the proper position
just after dusk and just prior to dawn. But let us take a look at the
binocular situation for a range to the small comet of 1000 km (625
miles). We will use binoculars with a magnification of 7X and a clear
entrance pupil of 50 mm in diameter. For the human eye, the entrance
pupil varies but a diameter of 5 mm is typical. Thus the binoculars
increase the light-gathering capability of the human eye by a factor of
100, or V=5. As seen through the binoculars then, the brightness of a
small comet with V=8.3 is V= (8.3 - 5) = 3.3 and is detectable with the
eye.
Consequently, the frequency of detection of the small comets with the
binoculars is of interest. The viewing geometry is quite constrained
because the objects will not be seen in the darkness of Earth's shadow
and certainly not through the sunlit atmosphere. In fact, the atmospheric
brightness is not less than V=3.1, and similar to the brightness of the
small comet, until about 72 minutes after sunset and during the period 72
minutes before sunrise. We estimate that there are approximately
30-minute windows for detection of these small comets at solar phase
angles in the range of 18 degrees to 40 degrees which are contiguous to
and on the dark side of the above two windows. Importantly, the
binoculars must be pointed at the intersection of Earth's shadow and the
1000-km (625-mile) range. The apparent motions of the small comets will
be in the range of about 1 degree/s and will remain in the field-of-view
of binoculars with a field-of-view of 10 degrees for about 10 seconds.
Now we must calculate the frequency of the small comet detections with
your binoculars. The viewing is through the Earth's shadow so that part
of the detection area must be subtracted because, obviously, if the sun
doesn't shine on the comets they are essentially invisible.(See the
viewing geometry in the accompanying drawing.) With an apex at your
binoculars and the two lines extending to 1000 km (625 miles), a rough
estimate of the area in sunlight is approximately 2/3 of the total area
of the triangle. If your field-of-view is 10 degrees then the detection
area in sunlight is about 6 x 104
km2. For the present purposes of simple
estimation we use the average interplanetary rate of 1.2 x
10-9 small
comets/km2-s intercepting the above detection
area and neglect the effects of Earth's gravitational focusing. Thus the
detection rate is about (1.2 x 10-9) x (6 x
104) = 7 x 10-5
events/s, or 1 event every 5 hours. Since your viewing time is about 30
minutes each for the pre-dawn and post-dusk samples, one would expect to
see one event every 5 days of viewing with these binoculars. The short
period for viewing is due to the rotation of the Earth and the rapid
geometric degradation of the viewing geometry.
For telescopes with larger apertures the viewing geometry remains the
same as shown in the accompanying figure. The viewing geometry is
generally parallel to the ecliptic plane. Basically, you can estimate
your detection rate by comparing your telescope's characteristics with
those for the binoculars as given above. For example, if you have a
collecting aperture of 90-mm diameter, then the range of your telescope
is approximately proportional to the diameter, or about 1800 km (1125
miles), since the object brightness decreases as
r-2. At this distance, for an object with an
apparent speed of 10 km/s, the apparent angular speed is about 0.3
degree/second. The event rate is proportional to the fan collecting
area, i.e., proportional to the square of the above range times the
viewing angle of your telescope. If the field-of-view of your telescope
is the same as that of the above binoculars (probably smaller) then your
event rate will be (1800/1000)2 x (10/10) = 3.2
greater than with the binoculars. This is about 1 event every 1.5 hours
for the average interplanetary rate. The occurrence frequency is greater
than this average for the months of June through the first week of
November due to seasonal variations by factors in the range of 2 to 3.
The rates are lesser for the other months with January at the minimal
rates.
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For a summary of the capability of the human eye for the detection of faint meteors, see D.W.R. McKinley, Meteor Science and Engineering, McGraw-Hill Book Company, New York, pp. 106-107, 1961.
For the variation of sky brightness throughout twilight, see C.W. Allen, Astrophysical Quantities, 3rd Edition, Athlone Press, London, p. 134, 1973.
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