In the preceding chapters, we have made several references to the fact that within each category of Solar System bodies, there appears to be a large variation in the sizes of these bodies, including the equivalence in size of bodies in different categories. For example, there are bodies called planets, such as Mercury and Pluto, that are equivalent in size to some of the satellites of Jupiter, such as Ganymede and Callisto, to be discussed in this chapter. Another example is that there is no comparison in size between Jupiter and Mercury or Pluto and yet all three are called planets; Jupiter is vastly larger than either. What this means for us is that our natural inclination to believe that bodies belonging to the same categories must be alike in either size, composition, appearance, or in some sense is not applicable to Solar System bodies. For example, we can not think about the various categories of Solar System bodies as a hierarchy of different sized objects, such that planets are always larger than satellites, which in turn are always larger than asteroids, etc. Not only is this true about size, but it is also true for chemical composition and appearance. As Chapters 8 and 9 have shown, the Terrestrial and Jovian planets are quite different in these two aspects. The categories of Solar System bodies that we have heard about since childhood are historical accidents based on what mankind thought they were discovering. Thus we must be careful to pay special attention to the diversity that exists in each category, which is especially true for the minor bodies of the Solar System--satellites, asteroids, meteoroids, and comets.
Only three satellites are known for the Terrestrial planets.
One is the Moon, which we discussed in Chapter 7. The other
two are the little satellites of Mars, which were discovered in
1877. Phobos, the inner one, and Deimos, the outer one, are potato-shaped
bodies with cratered surfaces. Phobos orbits eastward, just as
our Moon does, and in the same direction that Mars rotates, in
a period of 12.5 hours at a distance of about 6000 km from the
surface of Mars. This gives it an angular size, as seen from
the surface of Mars, of about half that of our Moon. Since it
revolves around Mars much faster than the planet rotates, it rises
on the western horizon and sets on the eastern horizon 5.5 hours
later. As observed from its primary, Phobos is the only natural
satellite in the Solar System whose motion is of this form.
Phobos (Figure 10.1) is about 27 km long, 21 km high, and 19
km wide. Both Phobos and Deimos have been shaped by high-velocity
impacts, which appear to have sheared off large sections of each
satellite. In addition, both have many craters, but no significant
amount of ejected material or craters with central peaks, a reasonable
result since their gravitational attraction is very small. Some
of the material ejected during cratering simply escapes and does
not fall back to the satellites' surfaces.
Phobos seems more heavily cratered than Deimos, the largest crater,
Stickney, being about 10 km across. It also has mysterious long
parallel grooves across a large part of its surface, as can be
seen in Figure 10.1. They are a few hundred meters wide and a
few tens of meters deep and may have been formed by the same impact
that caused the crater Stickney.
Deimos is about half the size of Phobos--some 15 km by 12 km.
It orbits Mars some 20,000 km from the planet's surface in a
period of 30.3 hours. Its angular size, as seen from Mars, is
quite small, roughly equivalent to a quarter viewed at a distance
of about 40 m. Its orbital period is somewhat longer than the
rotational period of Mars, so it rises on the eastern horizon
and sets on the western horizon nearly 3 days later, while going
through its phases twice.
The darkness of the surface of both satellites is probably due
to carbon- and water-rich minerals, such as are found in black,
crumbly meteorites known as carbonaceous chondrites. A number
of asteroids appear to have similar surfaces. This has led to
the speculation that Mars's satellites may be captured asteroids
acquired early in the planet's life.
On January 1, 1801, a Sicilian astronomer, Giuseppe Piazzi (1746-1826),
accidentally discovered a faint object whose orbital motion was
that of a body 2.8 AU from the Sun. Although Piazzi thought it
was a comet, others noted that it was located about where a major
planet would be expected according to Bode's law (Section 3.6).
The object was later named Ceres, after the Roman goddess of
agriculture. Shortly afterward, three more objects were discovered
with orbits near 2.8 AU: Pallas in 1802, Juno in 1804, and Vesta
in 1807. Since photographic techniques were introduced into astronomical
research in the 1890s, more than 3000 of these bodies have been
discovered.
So instead of one planet in the slot at 2.8 AU, many small bodies
orbit in the region between Mars and Jupiter. William Herschel
called these objects asteroids because in a telescope they
looked like stars. Better than 90 percent of them have orbits
in an asteroid belt between 2.2 and 3.3 AU, with periods from
3 to 6 years. For several asteroids, their orbits are more elliptic
than are those of the planets and more inclined to the ecliptic.
However, they move in the same direction as the planets around
the Sun.
Asteroids vary in size from Ceres (960 km) down to an estimated
1 million that are more than 1 km in diameter and countless numbers
of even smaller ones. All the asteroids together add up to no
more than six ten-thousandths of Earth's mass. Ceres alone constitutes
about 20 percent of the mass of all the asteroids (Figure 10.2).
Six of the larger asteroids are listed in Table 10.2.
Photometric studies of asteroids have for some time been interpreted
as showing that they differ in size, shape, and rotation. All
but the largest ones are too small to show a measurable disk.
From the variations in their brightness, it has been assumed
that most have somewhat irregular shapes with periods of rotation
measured in hours.
Their colors put nearly all asteroids into two categories: Some
are bright reddish or sandy-colored, a sign of iron and magnesium
silicates, and they populate mostly the inner part of the asteroid
belt. Most asteroids, however, have the darker neutral color
of material containing various carbon- or water-rich compounds
(carbonaceous) and occupy mainly the outer part of the belt.
Collisions between two asteroids may produce effects ranging
from craters (if a small one collides with a large one) to fragmenting
of both asteroids (if they are of comparable size). For example,
if the body producing crater Stickney on Mars's satellite Phobos
(Figure 10.1) had been a little larger, Phobos might have been
broken into many small pieces. As it is, the grooves on Phobos
may be large cracks produced by the impact.
In October of 1977, the asteroid Chiron was discovered traveling
in a highly eccentric orbit (eccentricity = 0.38) at an angle
of 6.9o to the plane of the ecliptic. It ranges between 8.5 and
18.9 AU, or roughly between the orbits of Saturn and Uranus, with
a period of 50.7 years. Although a couple of other asteroids
are known to have aphelion points near Saturn's orbit, Chiron
is the most distant yet discovered. Because of its great distance
from the asteroid belt, there is a question whether it might be
the first discovery in an outer zone of asteroids. Or possibly
it confirms the suspicion that asteroids and comets are objects
related to each other, although not having the same composition.
Together they are all that remains of the small bodies, called
planetesimals, that once filled the Solar System and ultimately
coalesced to form the planets 4.6 billion years ago (Section 11.4).
There are at least a thousand asteroids with diameters greater
than 1 km that at some time during their orbit come close to Earth.
Eventually, some of these will collide with Earth, as other asteroids
have done in the past, for example, the 35-m-diameter one that
caused the Barringer Meteor Crater (Figure 10.3). Current estimates
are that, for those with diameters under 0.1 km, one will collide
with Earth every 10,000 years, releasing as much energy as a 1000
atomic bombs (13 million tons of TNT). An asteroid with a diameter
close to 10 km should strike Earth once every 100 million years
with an energy equivalent to 1 billion atomic bombs (13 trillion
tons of TNT). In fact, it has been proposed that the well-documented
extinction, the so-called Cretaceous-Tertiary Extinction, of approximately
60 percent of all animal species that occurred about 65 million
years ago was caused by climatic changes from the dust kicked
up by the impact of a 10-km asteroid. So massive was the dust
that was ejected into the atmosphere that a layer of clay 1 to
2 cm thick was deposited worldwide of which about 7 percent was
carbonaceous matter from the asteroid. Work is currently in progress
to determine whether or not other wholesale periods of extinction
may have been caused by asteroid impacts.
As much as 1000 tons of cosmic debris--billions of microscopic
particles--pepper the Earth daily. We are aware only of those
weighing a significant fraction of a gram, which produce the so
called shooting stars that flash across the sky. All but a few
are too small to leave luminous trails. These solid particles
are called meteoroids before they encounter Earth. Those
large enough to survive flight through our atmosphere and land
are called meteorites. And the luminous trails of the
smaller particles that are completely vaporized in the atmosphere
are called meteors. The largest and brightest meteors
are referred to as fireballs or bolides.
Our atmosphere slows incoming meteoroids and transforms their
kinetic energy into radiant and thermal energy. A meteoroid passing
through the atmosphere leaves a wide, dense column of electrons
stripped from atoms and molecules in its path. As ionized atoms
regain their electrons, they deexcite, emitting photons that make
the momentary luminous trail we see from the ground as a meteor
or shooting star. Anything that remains of the vaporized meteoroid
slowly filters down through the air as dust and solidified droplets
of melted meteoroid.
When meteoritic particles strike the Earth, they are moving anywhere
from about 10 up to 72 km/s, depending on the angle at which they
encounter Earth. The velocities convince us that meteoroids belong
to the Solar System, moving in independent orbits around the Sun.
The normal observed rate for meteors is about 10 per hour over
the entire sky. Fewer meteors are seen before midnight than after
midnight. This is so because during the evening hours we are
on the back side of Earth, facing the direction opposite to Earth's
orbital motion, and we see only the swift meteoroids overtaking
us from the rear. During the morning hours, Earth's rotation
has turned us so that we are facing in the same direction as its
orbital motion. Hence we see those meteoroids that we overtake
and those which meet us head on.
Several times during each year we see meteor showers,
swarms of shooting stars darting from a small area in the sky.
These showers can persist for hours or days. On such occasions,
Earth is passing through a large group of particles moving in
ribbonlike fashion along an orbit around the Sun. Perspective
makes their tracks seem to diverge from a small spot in the sky
called a radiant. Such showers are named after the constellation
in which the radiant appears. Some of the better known showers
are listed in Table 10.3.
About 100 years ago astronomers found that some meteoroids travel
in orbits much like those of some comets. They had found a link
between meteor showers and short-period comets (to be discussed
later in this chapter). The particle swarms are the resulting
debris left after the evaporation of a comet. For example, on
the night of November 13, 1833, watchers in the southern part
of the Atlantic seaboard were awestruck as over 100,000 shooting
stars per hour plummeted from the constellation Leo for 3 hours.
The great display was produced when Earth encountered a swarm
of meteors orbiting the Sun in a period of 33 years and associated
with comet Tempel (1866 I). The comet itself has long since vanished,
leaving the meteor shower as a remainder of its existence. The
subsequent meteoric displays of 1866, 1899, and 1932 were progressively
weaker; then on November 17, 1966, a fairly spectacular meteor
shower was observed in the southwestern part of the United States.
With the passage of time, a meteor stream--which is made
up of conglomerates of fine dust and ice-covered particles--is
strung out along the comet's orbit. This ribbon of particles
typically averages about 50,000 km in cross section. Thus Earth
must come fairly close to a meteor stream, therefore, in order
for us to see a meteor shower.
Most meteorites are discovered accidentally years after they
fall. Of some three dozen recovered meteorite falls weighing
more than a ton, only a few were seen descending. Not many falls
are ever recovered. Most meteorites land in the oceans or in
unoccupied places, where their fall is less likely to be observed.
No known record tells of a community destroyed or an individual
killed by a meteorite despite some close calls. Approximately
3000 meteorite specimens have been recovered and catalogued for
study.
Meteorites striking Earth have probably formed thousands of craters,
but only 200 or so have been found. One major impact in 10,000
years is a reasonable estimate, and at that rate at least 50,000
giant meteorites must have struck Earth in the past 500 million
years. But the fossil craters left by many of these may lie buried
and unnoticed in the Earth's crust (Figure 8.9). Probably most
of them have been obliterated by weathering, erosion, and geologic
processes.
One that we know about, near Winslow, Arizona, is the Barringer
Meteor Crater (Figure 10.3), created by a meteorite weighing at
least 30,000 tons. It struck the Earth about 25,000 years ago
and must have devastated all plant and animal life within a large
area. The crater is over 1.2 km across and 167 m deep. Thirty
tons of shattered iron fragments have been picked up within about
6 km of the crater.
At 7 A.M. on June 30, 1908, a tremendous fireball flashed across
the sky in Siberia. A great ball of flame brighter than the Sun
was seen leaping from a forested region near the Tunguska River.
The sight of the fire was followed by the sound of an explosion
powerful enough to level trees within approximately 50 km. Earth
tremors were recorded on seismographs throughout Europe, yet no
large crater was formed, only many small ones. The most plausible
explanation for the event is that a small comet (possibly part
of comet Encke) or a large, fragile, stony meteorite struck the
Earth, dissipated its kinetic energy on the forest and ground,
and completely vaporized.
Three classes of meteorites have been established based on their
chemical and metallurgical properties. The first group, known
as stony meteorites, is composed primarily of silicates
of iron, magnesium, aluminum, and other metals. These generally
have a relatively smooth, brown or grayish, fused crust indented
with pits and cavities. Buried inside all but a small fraction
of them are small pieces of glassy minerals, called chondrules,
that apparently formed from molten droplets, presumably during
the formation of the Solar System.
One subgroup of the stones is the carbonaceous chondrites,
which contain large amounts of carbon, water, and other volatiles
that would have been driven off with the slightest heating above
about 500 K. Therefore, these are the most primeval samples of
matter from the early Solar System that we have. They are doubly
interesting because they contain organic compounds, such as hydrocarbons,
amino acids, and lipids. These biologically important compounds
evidently formed in the primordial solar nebula without the assistance
of living organisms.
The second group, known as stony-iron meteorites, is a
mix of stone and iron. Their brownish crust sometimes contains
pockets of the yellow mineral olivine. Inside the meteorite the
iron may have a veinlike or globular structure.
The third category, iron meteorites, is almost exclusively
composed of iron, with some nickel. These meteorites are easily
identified by their characteristic pitted, brownish exterior and
high density. Cut, etched, and polished, they usually have a
peculiar crystalline pattern unlike any in terrestrial iron.
They show evidence of melting and signs of other heating and cooling
processes.
Stones are the most brittle kind of meteorite, and they are far
more fragile than irons. Even though most falls are stones, more
of the recovered meteorites are irons because they are relatively
easy to identify and they resist weathering.
Those meteorites which have been dated by their natural radioactivity
average tens of millions of years for stones and 600 million years
for irons. These are their ages only since the breakup of the
larger mass of which they were probably a part. The most ancient
specimens are about 4.6 billion years old, the same age as Earth.
The chemical and mineralogical sequences in the different classes
of meteorites indicate that they share the same heritage as that
of the rest of the Solar System.
We are still not totally sure of the origin of meteorites. It
is possible that meteoroids are primarily debris from asteroids
and comets, in which case they formed by accretion in the early
Solar System. However, some could be ejected bits and pieces
of matter from the Moon and Mars originating during the intense
cratering period early in the Solar System's history or later.
Another possibility is that meteorites may be descended from
a few chemically differentiated asteroids that were whittled down
by repeated collisions early in the Solar System's history. In
such a case, stony meteorites come from the original crusts, the
stony-irons from the intermediate parts, and the irons from the
core. Regardless of our ability to understand their origins,
it is evident that asteroids and meteorites are representatives
of the unused building material from which the Terrestrial planets
formed at the birth of the Solar System.
The space between the planets is a vacuum by terrestrial standards,
but it is not devoid of matter, since some gas and small, solid
dust particles exist there. The particulate part of the interplanetary
medium, called interplanetary dust, consists of particles
blown out from the Sun's atmosphere by the solar wind, micrometeoric
debris scattered by comets, and perhaps some granular powder strewn
about by asteroid and meteoroid collisions. Interplanetary dust
has even formed dust rings about the Sun analogous to Saturn's
rings.
We have learned about interplanetary dust from several sources.
One is the zodiacal light, which is most easily observed in our
Northern Hemisphere in spring after sundown in the west and in
fall before dawn in the east. It appears as a faint pyramidal
band of light tapering upward from the horizon along the line
of the ecliptic. The spectrum of zodiacal light is a faint replica
of the solar spectrum; it is produced by small particles lying
in the plane of the planets' orbits that scatter solar photons
in our direction.
Most direct evidence of interplanetary dust comes to us from
spacecraft experiments. Electronic sensors on the skin of the
spacecraft are arranged to count small dust particles as they
strike the surface. From the numbers of impacts, it is estimated
that the average spacing between interplanetary dust particles
is many meters. The total mass of dust particles is estimated
to be about 1020 g, or about a hundred-millionth of Earth's mass.
Most interplanetary matter is in the form of an ionized gas that
comprises the solar wind. It consists of an almost continuous
stream of particles, mostly protons and electrons, flowing out
from the Sun's corona. As the solar wind moves forward, it forms
an expanding spiral pattern due to the Sun's rotation, and its
velocity increases until, several solar radii from the Sun, it
equals the speed of sound in the plasma. Its velocity continues
to increase as it flows outward, much as rocket gases are accelerated
to supersonic velocities in a rocket nozzle. Near Earth the solar
wind reaches a velocity of about 400 km/s. Beyond Earth its speed
remains very nearly constant.
At Earth's distance the wind's density is down to about five
protons and five electrons per cubic centimeter on average, but
it can rise on occasion to 100 particles/cm3. Compare that with
the number of molecules in your room, about 1019 particles/cm3.
The temperature of the wind particles is about 200,000 K in the
vicinity of the Earth. This is less than their approximately
1 million K temperature when they were in the inner parts of the
Sun's corona. The density is so very low, however, that the wind
transfers no appreciable quantity of heat to the Earth.
The solar wind rushes past Terrestrial planets and flows out
to the outer Solar System, the realm dominated by four giant planets--the
Jovian planets.
10.1. Satellites of the Terrestrial Planets
10.2. Asteroids and Meteoroids
10.2.1. The Asteroid Belt
10.2.2. Asteroid Collisions with Earth
10.2.3. Meteoroid Debris and Showers
10.2.4. Recovered Meteorites
10.3. Interplanetary Medium
10.3.1. Interplanetary Dust
10.3.2. Interplanetary Gas