I. In this last section of the course, we'll be concerned with the
lithosphere, which is the rock and mineral sphere of our planet (that is,
most of it!).
A. The branch of physical geography concerned with the lithosphere is
called "geomorphology."
B. Remember how biogeography was the branch of physical geography
concerned with the biosphere and how it was shared with biology?
Well, geomorphology is shared with geology: Some geomorphologists are
geographers and some are geologists. Sometimes our tidy disciplinary
structures don't quite coïncide with what people are actually
doing!
C. Anyhow, in this section, we will be concerned with:
1. The structure and composition of the planet itself.
2. Processes by which the earth's surface is built up (tectonism).
3. Processes by which the earth's surface is worn smooth, as by
rivers, glaciers, waves, and winds (gradation).
II. Structure of Planet Earth.
A. Earth is structured in layers. There are two different ways of
classifying these layers (there's that classification thing again).
B. The first of these entails classification by the physical state of
matter and general chemical composition. I'll start at the center of
the earth and work out to the surface in this discussion.
1. The innermost part of the planet is believed to exist in a solid
state: This is called the "solid inner core."
a. It extends out some 1,250 km out from the center of the earth,
or just under 20 percent of the way out from the center to the
surface (the earth's radius is roughly 6,330 km: Lecture 2).
b. It is made up of iron (Fe) with some nickel (Ni), very dense and
heavy elements.
c. This can be surmised from the following argument:
i. The average density of the most abundant materials making
up asteroids in our solar system is about 5.5 g/cubic
centimeter (iron is the most common solid in outer space,
particularly in the inner solar system, where Earth is
located).
ii. The average density of Earth's crustal materials, however,
is only 3.3 g/cubic meter.
iii. Assuming Earth formed from the materials most common in the
inner solar system, the heavy stuff has to be present
somewhere in the earth.
iv. Earth, like the other inner planets, went through a molten
phase early in its history, which allowed gravity to
stratify substances by density. So, iron and nickel would
settle at the "bottom" of the gravity well: the center of
the young planet.
v. The solidity of the inner core is surmised from the
performance of iron and nickel in the laboratory and in
massive computer models at pressures similar to those at
the core of the planet: Even though it's incredibly hot in
the earth's interior (current estimates are that it's about
5,500 K, which is close to the temperature of the surface
of the sun!), the pressure is so great that the melting
point of iron contaminated by nickel is elevated far beyond
those high temperatures (6,500 K), leaving the nickel-iron
as a solid.
2. The next layer out is the liquid outer core.
a. This, too, is dominated by nickel-iron.
b. This is known from the earth's strong magnetic field, which can
be produced by currents in liquid iron.
c. It extends out to some 3,450 km from the center of the earth,
which means it's about 2,200 km thick.
d. It is known to exist in a liquid state because of the behavior
of earthquake waves, particularly shear body waves or secondary
waves.
i. Liquid cannot respond to shear forces (lateral or side by
side forces), so it can't transmit shear waves.
ii. As a result, there is a seismic shadow on the side of the
earth antipodal to an earthquake's epicenter: Seismic
stations there will not receive secondary waves, though
they will get primary (compressional) waves from a given
earthquake. Primary waves, too, generate a shadow centered
roughly 120° from the focus due to being refracted or
bent inward as they slow down crossing into the liquid
inner core.
iii. It's not quite as direct as the size of the seismic shadow
equalling the size of the liquid outer core, because
seismic waves speed up as they travel through denser solids
and refract or bend when they pass through different
materials, and this curves their path back out to the
surface. Factoring that in, we can still compute the size
of the outer liquid core's outer boundary from the size of
the shear wave seismic shadow on the opposite side of the
earth.
Shear wave seismic shadow:
Primary wave seismic shadow due to velocity change:
3. The earth's mantle is the third layer out.
a. It covers everything from the liquid outer core to the bottom of
the earth's crust.
b. It extends, then, from about 3,450 km out from the center all
the way to within anywhere between 5 and 100 km of the surface.
It's not quite 2,900 km thick.
c. The mantle is rather variable, but it is dominated by actual
rock, not just iron alloys.
i. This is largely silicate in basic structure (built around
the silica and oxygen combination, SiO2).
ii. These rocks are, however, highly enriched in iron and
magnesium, so they are called "ultramafic" rocks ("ma" from
magnesium and "f" from the chemical symbol for iron, Fe).
iii. So, these rocks are extremely heavy and dense compared with
typical surface rocks, and they are usually very dark as
well because of the iron and magnesium in them.
iv. The mantle varies in its state of matter, from a soft and
nearly liquid condition near its inner boundary with the
liquid outer core and again near the top, a few kilomters
under the earth's crust. In other areas, it may show
nearly brittle solidity. The softest parts of the mantle
can flow in response to heat, kind of like "silly putty"?
4. The fourth and final layer out is the crust.
a. This is very, very thin, ranging from maybe 5 km under the
oceans to as thick as 100 km under certain mountainous areas of
the continents (usually, it's about 40 km thick under the
continents).
b. The Mohorovicic Discontinuity (often called, simply, "the Moho"
by its friends) marks the transition from the top of the mantle
to the bottom of the crust: It's an area where there is a sharp
increase in the velocity of seismic waves as they pass into an
area of different density and rigidity. Andrija Mohorovicic
first noticed this effect back in 1909, and it has since been
tied in theory with the mantle-crust transition.
c. Rocks in the crust are solid to the state of rigid and brittle.
d. They are also highly variable, including rocks of molten origin,
rocks of sedimentary deposition origin, and rocks that have
undergone all sorts of structural and chemical alterations.
e. The crust itself can be divided into one or two sublayers,
depending on where you are:
i. One kind of layer is found everywhere, under the oceans and
way under the contintents.
a. This layer is dominated by relatively heavy, dark, dense
rocks of "mafic" composition. Most of these mafic rocks
are of volcanic origin and are called "basalts."
b. This dense, heavy mafic layer is sometimes called the
"sima" (dominated by silicate rocks of mafic
composition) and sometimes the "mafic layer" and
sometimes the "basaltic" layer.
c. It tends to be relatively thin, usually from about 5-12
km in thickness.
ii. A second layer is normally found only on the continents.
a. It is made up of light rocks primarily composed of
silicates enriched in the lighter elements, such as
aluminum (Al), potassium (K), and sodium (Na).
b. This layer is sometimes called the "sial" (dominated by
silicate rocks with lighter elements mixed in, such as
aluminum) or the "silicic layer" (overwhelmingly
silicic) or the "felsic layer" (for potassium-rich
versions of feldspar). These rocks commonly occur in
the earth's crust as "granite," so this layer is
sometimes called the granitic layer.
c. This layer is considerably thicker than the basaltic
lower layer, around 40 km.
5. So, that takes care of the first system for classifying the layers
of the planet, the one that classifies the layers by states of
matter (liquid, solid, and ductile or soft solid) and general
chemical composition (nickel-iron, ultramafic rock, mafic rock, and
felsic rock). This system gives rise to the solid inner core, the
liquid outer core, the mantle, and the crust, with the crust
subdivided into sima and sial.
C. The second classification of the layers within the planet is strictly
by states of matter only: solid, liquid, or ductile solid. It is
mechanical, then, rather than compositional.
1. This classification was developed specifically for the needs of
plate tectonic theory (about which beaucoup later), for
understanding the drift of the continents in deep geological time.
a. Since this one concerns the surface plates and the processes
driving them around, I'll start with the surface and work down
this time.
b. In this system, the word "lithosphere" means the hardest, most
rigid layer of the outermost planet, the layer subject to
failure and division into plates (yes, this can be confusing,
because the word "lithosphere" also has a more generic usage,
describing the entire rock and mineral part of the planet).
i. It extends down to about where compressional heating of
rocks and minerals reaches roughly 1,300° C. Past the
immediate surface of the earth, temperatures of rock start
climbing because of the compression of all the material
lying above it. Rocks cooler than 1,300° C in general
behave in a rigid manner, while those warmer begin to
weaken and behave in a soft, plastic manner (capable of
flowing around).
ii. The 1,300° C isotherm lies a few kilometers below the
bottom of most of the ocean floor (except where ocean floor
piles up at certain plate boundaries, where it can thicken
to 100-150 km or so) and up to 250-300 km under the deep
mountain roots and the shield areas at the heart of the
continents.
iii. As such, the lithosphere includes all of the crust in the
other classification system, plus the most rigid part of
the upper mantle. This is the zone subject to breakage
into new, rigid plates.
c. In this mechanical system, the word "æsthenosphere"
(loosely rendered, the "wimpy sphere" or the "weak sphere")
refers to the softest, most plastic part of the upper mantle, an
area where rock weakens because it's awfully close to its
melting point (and localized pockets DO in fact melt, providing
magma for volcanoes and such).
i. Interestingly enough, there is seismological evidence for
the probable existence of the æsthenosphere. Seismic
shear waves generally slow down rather remarkably as they
enter this zone of not-quite-liquid (remember shear waves
can't pass through liquids, so it's not surprising that
they would slow down as they pass through rocks just this
side of liquid). This "low velocity zone" is taken as
empirical support for the existence of the
æsthenosphere.
ii. The æsthenosphere extends down to roughly 700 km, at
which point the rocks are under enough pressure to
overcompensate for the great temperature and resume a more
rigid mechanical condition.
iii. The lithospheric plates move about on top of the
æsthenosphere, in response to currents of flow in the
æsthenosphere that may reflect conduction of heat up
from the core. More on all that later.
d. The next layer down is the "mesosphere."
i. Yep, you're right, you DID hear that word before. In a
maddening disconnect between geology and climatology,
between one end of physical geography and another, someone
picked and popularized a word that already has a well-
established meaning in studies of weather and climate. The
mesophere you met already is the third layer up in the
atmosphere; here it's the third layer down in the planet!
Isn't that exasperating!?
ii. Anyhow, the mesophere now refers to the most rigid part of
the lower mantle, below about 700 km or so. This is where
pressure compensates for (compressional) temperature
increases to return mantle rocks to a more rigid, solid
condition.
e. The fourth layer down is exactly the same one we bumped into
before: the liquid outer core, extending down from about 2,900
km. Here, we've passed beyond the lighter silicate rocks and
into the realm of nearly pure iron (iron with some nickel). So,
the temperatures are high enough to transcend the melting point
of iron even at these pressures, and we get the liquid outer
core.
f. The fifth and last layer down is the solid inner core we met
before, below about 5,100 km and extending right to the center
of the earth. Once again the pressures are so great as to force
the melting point of even pure metal above the actual
temperatures down there, and so we believe the inner core is
solid nickel-iron.
g. Here are the two systems side by side:
Well, that's enough of the layered structure of the planet. There are two
different systems for classifying these gravity-induced layers: States of
matter plus general chemical composition and the strictly mechanical states of
matter system.
The first classification system really brings out the rôle of gravity in
layering our once-molten planet: The heaviest, densest (and locally most
abundant) stuff, nickel-iron, settled out at the bottom of the planet's
gravity well, its center. This gave us the core. All rock materials were
displaced towards the surface, giving us the mantle and crust. These are also
seen to reflect gravity layering: The mantle is made up of the heavier
ultramafic rock, while the basalt layer of the crust is made up of mafic rock,
and the granitic layer of the crust (on top of the continents) is made up of
felsic rocks, the lightest of them all.
The second classification is specific to the needs of understanding plate
tectonics, so it focusses on mechanical properties and behavior: strictly the
states of matter (solid, plastic, and liquid). This helps us conceptualize
the rigid, brittle lithospheric plates sloshing around on the weaker
æsthenosphere below and gives us room to think about mechanisms driving
the currents in the æsthenosphere (such as convection of heat from the
core, ultimately).
Next time, I'll go into the composition of the crust: elements, minerals, and
rocks, and how rocks transform from one type to another.
Document and © maintained by Dr.
Rodrigue
First placed on web: 11/11/00
Last revised: 07/03/07