UKIRT Newsletter : Issue 3 : Research : Asteroids
Direct Hit on a Near Miss
John Davies
UKIRT Support Scientist, Joint Astronomy Centre, Hilo
In August, UKIRT demonstrated its flexibility and reliabilty by
snatching high quality near-infrared spectra of a rapidly moving object
visible briefly during the pre-dawn twilight.
At about lunchtime on August 10th Hawaii time (22:30 UT) the Earth had
a close encounter as the recently discovered asteroid 1998 ML14 flew within
2.7 million kilometers of our planet. The asteroid, a member of the class
of "Near Earth Objects" of which several hundred are known, had been discovered
about 6 weeks earlier. This was too little warning for a regular PATT application
but, by co-incidence, UKIRT was already scheduled to be observing asteroids
that night as part of Andrew Rivkin's (Lunar and Planetary Laboratory,
Arizona) CGS4 study of hydrated minerals in main belt asteroids.
As I was at the telescope with him anyway, we decided to try to get
some near-IR spectra of 1998 ML14. However the asteroid was a long way
South (Dec -35) and so was not well placed for UKIRT, worse still, it would
not rise into UKIRT's pointing envelope until minutes before dawn.
With the inevitable uncertainty in the orbit of a newly discovered object,
especially one whose path was under the influence of the Earth's own gravitational
pull, it promised to be a challenging observation.
Rather than risk losing time from our primary project preparing for
an observation that might not even be possible, we planned to use the first
night as a dry run to confirm that we could at least find the rapidly moving
target. Just after the asteroid rose, and already nine minutes into nautical
twilight, Chris Davis slewed UKIRT to the predicted position and within
a few moments we had something in sight. Moments later the object's motion
of more than half an arc second per second in both RA and Dec confirmed
the identification. Chris centred the asteroid in the guide box and turned
on the autoguider. The fast-guider locked on and, even though it was now
getting quite light, we started peaking up CGS4. This done we began integrating
and to our great satisfaction managed to get a few minutes of data before
the asteroid vanished in the rapidly brightening sky.
Flushed with this sucess we decided to repeat the attempt the following
night, but this time we set up our standard stars and pointing before the
asteroid rose and ambushed it, locking on the guider within a minute
of it coming over UKIRT's horizon and squeezing in spectra in two separate
wavebands, plus a final standard, before dawn. Even though the asteroid
was fading at a rate of about one magnitude every day (due to increasing
distance and increasing solar phase angle as seen from Earth) we repeated
the exercise the following morning and finished up with enough data to
produce a high signal to noise spectrum from about 1.1 to 2.5 microns (Fig
1.)
 |
FIGURE 1 : A preliminary composite spectrum of 1998
ML14. All five spectral fragments have been normalised and combined. The
structure just longward of 2 microns is not reliable, it is due to poor
atmospheric cancellation in this region. |
Apart from the intrinsic value of this spectrum, which will enable us
to identify specific minerals on the asteroid and help to classify it,
these observations show how well UKIRT can operate as an observatory system.
On the final night I kept notes of how the observing compared to our plan
and the table below shows the result.
| Activity |
Planned Time (UT) |
Actual Time (UT) |
| Begin FLAT-ARC for 1st standard |
14:15
|
14:15
|
| Slew to BS1532 & peakup |
14:20
|
14:19
|
| Start integrating on BS1532 |
14:25
|
14:26
|
| Begin slew to asteroid & peakup |
14:35
|
14:36
|
| Start integration on asteroid |
14:40
|
14:41
|
| Slew to BS1532 & start integrating |
14:55
|
14:57
|
| Change grating to new wavelength |
15:00
|
?
|
| Slew back to asteroid, peakup & start integration |
15:05
|
15:07
|
| Slew to BS174 & start integrating |
15:25
|
15:21
|
| Do FLAT & ARC for 2nd grating setting |
15:30
|
15:27
|
All of this was done at the end of a busy night, at an airmass of between
2.05 and 1.7, in astronomical or nautical twilight, on a moving object
of uncertain position and with full tip-tilt correction on the asteroid.
To me this seems a pretty impressive technical performance and really shows
just what UKIRT, plus its instruments and operations team, can achieve.
What did we learn? From the absorption band around 2 microns we deduce
the prescence of the mineral pyroxene, which means 1998 ML14 is probably
a S type, or stony, asteroid. From this we can guess the albedo (reflectivity)
and estimate its diameter to be about 1km. Objects this size impact the
Earth on average every 150,000 years and strike with an energy of about
100,000 megatons of TNT, dwarfing the largest nuclear weapon ever built.
Had 1998 ML14 struck, it would indeed have been a Deep Impact.
And on the same subject...
Although from near-infrared spectra you can determine the spectral type
of an asteroid, and hence get an idea of its albedo and so its size, if
you want to determine the diameters of asteroids accurately, UKIRT can
do much better than this. With only the reflected light to go on you can't
really tell if you are looking at a large dark object (like a bit of coal)
or a small white object (like a snowball). The way around this is to observe
in both visible light and at wavelengths of 10 and 20 microns. This works
because some of the sunlight arriving at the asteroid is reflected, and
you measure that in the visible, and the rest is absorbed and warms up
the asteroid. This is then re-emitted as thermal infrared radiation which
can be measured using instruments such as CGS3 and Michelle. Since the
asteroid is in equilibrium with the sunlight it receives, from the ratio
of the reflected (visible) and emitted (infrared) light you can determine
both the size and albedo of the object.
 |
FIGURE 2 : An example of thermal model fits to UKIRT
data is shown, which is taken from Harris et al. (1998). The curves correspond
to three different thermal models, after adjusting parameters such as diameter
and albedo to give the best fit in each case. Of all the models the dotted
curve, which corresponds to the near-Earth asteroid model mentioned in
the text, fits the data best. |
Alan Harris from the German Aerospace Centre's Institute of Planetary
Exploration in Berlin is the PI of a UKIRT programme to do just this. Using
CGS3 as a spectrophotometer and synchronising observations with optical
observers around the world, he and I have sucessfully observed over half
a dozen near-Earth asteroids since 1997. Alan has applied his new thermal
model, which is designed specifically for observations of small objects
at the high solar phase angles typical of those encountered when observing
objects close to the Earth, to determine sizes and albedos of the asteroids
(see Harris, A.W., Davies, J.K, Green, S.F. (1998). Thermal Infrared
Spectrophotometry of the Near Earth Asteroids 2100 Ra-Shalom, and 1991
EE, Icarus, in press). We were unable to apply this technique to 1998
ML14 as CGS3 was not planned to be on UKIRT in August and it did not seem
worth installing it for just a single observation. However, when Michelle
is mounted at UKIRT it will be available for a good fraction of the time
and will hopefully be used in its imaging or spectrophotometric modes for
similar targets of opportunity. In fact, with Michelle and UFTI/UIST on
at the same time, UKIRT will be able to do both reflected (JHK) and thermally
emitted (NQ) radiation almost simultaneously, making it a powerful tool
for performing these types of observations.
P.S : For those of you who have seen the film Armageddon don't
worry, there is no known asteroid the size of Texas. For the Deep Impact
fans you can worry a bit, the scenario enacted by this movie is fairly
realistic, although unlikely in our lifetimes.
|