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- From: nolan@lpl.arizona.edu (Mike Nolan)
- Newsgroups: sci.astro
- Subject: Re: Toutatis Captured by Radar Images
- Message-ID: <1993Jan24.205041.7529@organpipe.uug.arizona.edu>
- Date: 24 Jan 93 20:50:41 GMT
- References: <3191@tymix.Tymnet.COM> <C18v5H.6oA@well.sf.ca.us> <schumach.727766698@convex.convex.com>
- Sender: news@organpipe.uug.arizona.edu
- Organization: Lunar & Planetary Laboratory, Tucson AZ.
- Lines: 56
-
- In article <schumach.727766698@convex.convex.com> schumach@convex.com (Richard A. Schumacher) writes:
- > [Tom van Flandern writes:]
- >>what it tells us about origins. The rms velocity between any two asteroids
- >>is about 5 km/s -- somewhat more near the Earth's orbit. Collisions
- >>between such objects would be catastrophically destructive. So the joined
- >>fragments must have been previously in orbit as satellites of the asteroid,
- >>brought down gradually by tidal forces until a gentle contact occurred.
- >
- >Mmmm, not necessarily. A small body striking a larger one might easily
- >disrupt the larger without dispersing the pieces. No doubt someone has
- >already attempted to calculate a distribution of such collisions based
- >on the known distribution of asteroid sizes and orbits.
-
- In fact, most models of asteroid collisions predict quite low
- velocities for the majority of the ejecta: in a 5 km/s collision, the
- projectile (smaller asteroid) tends to vaporize itself and nearby parts
- of the target, which then leave at about the speed of sound. The rest
- of the target may fracture and be bumped around, but the ejection
- velocities tend to be < 100 m/s, with much material (most, if the
- target is not completely destroyed) moving less than 10 m/s. In our
- model, the smallest material tends to move the fastest, which makes
- some intuitive sense by equipartition of energy. This makes little
- pieces fly off and the big lumps tend to fall back together. This was
- for models, though. There are data, such as the existance of families
- of asteroids with relative velocities a few hundred m/s, which suggest
- that the actual behavior is not as the models predict. It's by no
- means a solved problem (it better not be, it's much of my thesis). But
- no matter what speed the bits leave at, it's still hard to get them in
- orbit. If they're moving at less than escape velocity, they'll likely
- fall back, faster and they just leave. The injection burn is hard to
- come by.
-
- Using Toutatis as an example, the escape velocity is about 2 m/s
- (depends where on the surface you're standing), that's equivalent to
- (scribble scribble) about a 8 inch (sorry people in the real world)
- vertical jump on Earth, so be careful, even I can do that. To get into
- orbit, you need to be moving about that speed, then get apply a
- tangential force to put you in orbit. I won't say it's impossible, but
- it's a small window.
-
- As far as detecting them by radar, while the resolution may be 100 m,
- the objects don't have to be that big to be detected. They do have to
- be about as big as the radar wavelength, 10 cm or so (they used
- several). They may (probably) have to be larger than that to give a
- detectable signal. On the other hand, satellites more that one
- diameter away might be harder to detect if they're not specifically
- looking for them, because of the way radar works: you shine the light
- for a bit, then shut up and listen. If the echo comes back before or
- after you listen, you don't detect it. Similarly if the velocity is
- different than you're looking for: out-of-band signals are filtered
- out, as they are presumably noise. I don't actually know what the
- limits are on this.
-
- Mike Nolan nolan@{lpl.arizona.edu,arizona.bitnet,looney.span}
- Lunar and Planetary Laboratory, University of Arizona, Tucson AZ 85721 USA
- Phone (602) 621 2344; Fax (602) 621 4933
-