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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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exact solution<br />

The path of a star in the Teff , L plane (the<br />

Hertzsprung–Russell, HR, diagram) as those<br />

physical parameters change is called the star’s<br />

evolutionary track. This track is primarily a<br />

function of the star’s initial mass. Collections<br />

of these tracks derived from theoretical stellar<br />

evolution models are often plotted on an HR diagram<br />

along with data from a collection of stars<br />

to estimate initial masses <strong>and</strong> ages.<br />

exact solution (of Einstein’s equations) A<br />

solution of Einstein’s equations, i.e., a metric.<br />

The term exact solution is used only when it is<br />

necessary to stress that the metric was derived<br />

from Einstein’s equations by strict mathematical<br />

procedures. The opposites of exact are an<br />

approximate (i.e., a perturbative solution) <strong>and</strong> a<br />

numerical solution. This opposition is irrelevant<br />

for several purposes; for example, all observational<br />

tests of the relativity theory necessarily<br />

involve approximations, <strong>and</strong> numerical calculations<br />

are often performed on top of exact solutions<br />

to obtain quantitative results. However,<br />

some theoretical problems (among them cosmic<br />

censorship <strong>and</strong> the existence of singularities)<br />

have been extensively studied within the<br />

framework of exact solutions.<br />

excitationtemperature Inagivenobject, the<br />

constituent atoms <strong>and</strong> molecules are in quantum<br />

mechanicallyexcitedstates, <strong>and</strong>theratiooftheir<br />

numbers in the ground state to the excited state<br />

is characterized by an excitation temperature,<br />

such that<br />

Nu<br />

Nl<br />

= gl<br />

e<br />

gu<br />

−hν/kTex<br />

where Nu <strong>and</strong> Nl are the number per volume<br />

in the upper <strong>and</strong> lower states, respectively, <strong>and</strong><br />

gl <strong>and</strong> gu are the statistical weights. The excitation<br />

temperature Tex characterizes this distribution<br />

for a given upper <strong>and</strong> lower state. If<br />

the atoms <strong>and</strong> molecules are in thermodynamic<br />

equilibrium (collision dominated), then the kinetictemperature,<br />

whichdescribesadistribution<br />

in speed of the atoms <strong>and</strong> molecules, is equal to<br />

the excitation temperature.<br />

exosphere The outermost part of the Earth’s<br />

atmosphere, beginning at about 500 to 1000 km<br />

above the surface. It is characterized by den-<br />

© 2001 by CRC Press LLC<br />

164<br />

sities so low that air molecules can escape into<br />

outer space.<br />

exotic terrane Continental deformation is<br />

partly achieved through folding, which preserves<br />

the juxtaposition of stratigraphic layers,<br />

but also through faulting. A terrane is a block of<br />

continent bounded by faults with a stratigraphy<br />

that is internally coherent but distinct from that<br />

of surrounding blocks. Mountain chains may be<br />

composed of several such blocks. A “suspect<br />

terrane” is a terrane whose geology appears to<br />

be unrelated to the surrounding rock. If it can<br />

be shown (through paleomagnetic methods, for<br />

example) that the rock in the terrane originated<br />

far away from the surrounding rock, then the<br />

terrane is known as an exotic terrane. This may<br />

happen if part of a continent is sliced away by<br />

a long strike-slip fault (such as the San Andreas<br />

fault) <strong>and</strong> is later attached to the continent or<br />

another continent elsewhere, or if an isl<strong>and</strong> arc<br />

or other oceanic l<strong>and</strong>form collides with <strong>and</strong> is<br />

engulfed by a continent.<br />

expansion The mathematical quantity (a<br />

scalar) that determines the rate of change of<br />

volume of a given small portion of a continuous<br />

medium (see also acceleration, kinematical<br />

invariants, rotation, shear). An observer<br />

placed in a medium in which acceleration, rotation,<br />

<strong>and</strong> shear all vanish while expansion is<br />

nonzero would see every point of the medium<br />

recede from (or collapse toward) him/her with<br />

the velocity v proportional to its distance from<br />

him/her, l, so that v = 1 3θl. The factor θ is the<br />

expansion (θ >0for receding motion, θ

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