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Trying to Get Hit: The Physics of Deep
Impact
The Story Illustrated
A Mathematical Explanation
Target Earth
Introduction
All Solar System objects undergo collisions. This fundamental fact,
recognized only in this century, now underlies much of our knowledge of
planetary geology.

It's popular, too, as a disaster scenario for movies and other media. Hollywood
actioneers taking shots at Earth have included the 1998 films Deep Impact
and Armageddon. A couple of generations earlier, When Worlds Collide
(1951) featured a runaway planet on a collision course with Earth. Books include
the recent novel Lucifer's Hammer, wherein Earth is pounded by
comets.
Of course, the theme goes way back in the science fiction genre. Consider
Jules Verne's Off On A Comet, written last century!
When I was child, I read these stories and also factual tales of such things
as astroblemes by authors like Dietz. As a eight-year-old, my favorite birthday
gift was a tektite. A two-inch glassy-black rock from Indochina, it looked a lot
like the obsidian I already knew from volcanic regions around my childhood home
in New Mexico. Later delvings went deeper and earlier: Ernst Opik's pioneering
thoughts on asteroid and comet collisions in the Solar System were particularly
intriguing.
The modern scientific popularizers of collisions as a major force in the
evolution of planets built on these earlier ideas. It's amazing to think that
the famous meteor crater in Arizona was believed to be of volcanic origin within
living memory. Shoemaker and others of this group helped prove that Barringer
Crater and other similar craters on the earth had an impact origin.
Even though my life and the exclusive culture of professional astronomy have
taken divergent paths, I'm still fascinated with the idea of planets as targets.
In July of 1994, I watched as craters were punched in Jupiter's atmosphere by
Comet Shoemaker-Levy 9. The impact sites of the comet fragments K, H, Q, etc.
were easily visible with a 10cm reflector telescope from my backyard in Wichita.
They looked like black holes. I followed them as the impacts were still
occurring, and then through July 1995. At that time, the Jovian latitudes around
45 degrees south still looked dusky.
Earlier, the 1968 close approach to the earth by 1566 Icarus and the 1973
fireball over the western U.S. were things I remember that got me thinking about
impact parameters and related topics.
When I read about the meteorite grazes on the pampas of Argentina, I wanted
to know the conditions leading to these unusual collisions.
Target Earth
The general circumstance of a comet or other object approaching the earth
from a great distance is described as a hyperbolic encounter between the
two.
The law of gravitation says two objects will move about each other in four
types of curves: hyperbola, parabola, ellipse and circle--the famous conic
sections of astrodynamics. You can think of it terms of speed as well as shape.
Something in an open-curved hyperbolic orbit will approach the earth with some
speed, no matter how far away it is. Also moving on an open curve, a parabolic
projectile will start out at zero speed at infinity, then speed up as it closes
with the earth. An elliptically orbiting satellite will always move alternately
towards and away from the earth in a cigar-shaped closed path, the speed
alternately increasing and decreasing, too. And a circularly orbiting satellite
is always at the same distance from the earth, always moving at the same speed.
Our comet's path will be a hyperbola whose size and shape will depend on two
things. The first one is how fast the comet's moving when it enters the earth's
sphere of influence. This region is a ball about a million kilometers in radius
and it is roughly where the earth's gravitational effects or influence
substantially equal or exceed the sun's influence on an object. The earth's
gravity is first "felt" by our comet at this distance, and its path is
deflected or bent towards the earth.
The second item is the miss distance: how close the comet would have come to
the earth if the earth had no effect on the comet's path. The technical name for
this distance is actually very appropriate: impact parameter.

Greater speed means less time in the stronger part of earth's gravitational
field, and less deflection. Same with distance--a bigger impact parameter means
less effect from earth's gravity.
Putting it all together, at a given speed, going too close will mean that
even though the miss distance is larger than an earth radius, the deflection
will be great enough that there will be a collision. The effective target size
is bigger than the planet. It's as if the earth is trying to get hit because
gravity focuses comets and other solar system objects onto a planet.

A grazing collision like the one that happened in prehistoric Argentina occurs
at the perigee of the hyperbolic orbit, tangent to the earth's surface and the
orbit. Inside the effective target radius, impacts will occur along other parts
of the incoming orbit, and impact at angles above the horizontal. The blanketing
effect of a beam of particles filling the entire collision cross-section is
greatest for those at and just inside the effective target radius and for low
approach speeds. The turning angle (deflection) is equal to the blanket angle
for an impact and can be as great as 180 degrees. You can be on the far side of
the earth from the comet's approach and still get hit!

Where will it hit? That depends on the orientation of the orbit in the solar
system relative to the earth, as does the radiant--the apparent direction of the
comet's approach. Timing is everything and the position of the comet in its
orbit will determine the longitude of impact. If broken up and stung out along
the orbit, then the string of pearls will hit repeatedly in a pattern like that
seen for Shoemaker-Levy 9's Jupiter impacts.
The Consequences 
How big a bang? The cometary speed and mass fixes how much energy and how
devastating the collision. The best comparisons to the consequences of
collisions with icy/rocky solar system objects are volcanic explosions and
eruptions. Volcanoes are a significant atmosphere-mediated energy injection
into our planet's environment, and can be quite similar to an equal energy
celestial impact. Krakatoa is a well-documented historical example, including a
massive explosion, tsunamis, debris storms, and a global pall like that of an
impact winter. With an energy of about 1-2 gigatons (about ten times more
energetic than the biggest H-bomb explosions) this Indonesian event is similar
to the impact of a 100s meter-sized asteroid with the earth. And events like
this are not rare--Mt. St. Helens, Santorini, Mt. Mazama and many others have
occurred within the past ten thousand years.
So, for energy input, volcanoes as catastrophes dominate short time spans,
perhaps up to 100 million years. Over the one billion-year span, impacts become
the most energetic explosive mechanism affecting the earth. Sixty-five million
years ago, the Chixulub collision was definitely a bad day for every life form
on the earth.
The long-term danger warrants attention by human beings, but can hardly be
used to justify a major program at the present time to protect us from earth
impacts. It would be more effective zoning islands with active volcanoes off
limits.
The Story Illustrated
A Mathematical Explanation
Target Earth
IMAGES AND CONTENT COPYRIGHT ©1999, 2000 BY ECLIPSAR (unless
otherwise credited)
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